WEBVTT 1 00:04:25.450 --> 00:04:27.540 Lynne Jones: Alright, good morning, everybody. 2 00:04:28.410 --> 00:04:33.149 Lynne Jones: We'll wait a few more minutes, it looks like. There's still people coming in. 3 00:04:44.800 --> 00:04:52.619 Lynne Jones: I hope yesterday was… was useful to people. I know that there was some overlap with what we talked about in the science assemblies, but, 4 00:04:53.420 --> 00:04:54.880 Lynne Jones: I didn't… 5 00:04:55.000 --> 00:05:00.570 Lynne Jones: Not everybody made it to the Science Assembly, and I did try to make it a little bit different. 6 00:05:41.840 --> 00:05:46.760 Lynne Jones: Good morning to those of you just joining us. I'm just gonna… 7 00:05:47.030 --> 00:05:50.559 Lynne Jones: We had a few minutes for people to finish trickling in. 8 00:06:08.700 --> 00:06:17.970 Lynne Jones: Well, I don't want to wait too long, because actually, this first part of today is kind of super packed, so, unfortunately. 9 00:06:18.310 --> 00:06:21.440 Lynne Jones: The content and the time span for that. 10 00:06:21.580 --> 00:06:24.250 Lynne Jones: It turned out weren't as great a match as I thought. 11 00:06:24.390 --> 00:06:30.959 Lynne Jones: So, let's get going. Good morning, and welcome again to the SELC Workshop page, Day 2. 12 00:06:31.460 --> 00:06:38.079 Lynne Jones: This is your SEOC and all of the members, and I… we… on the… 13 00:06:38.240 --> 00:06:43.639 Lynne Jones: from LSST, we really appreciate all of the work the SEOC do. 14 00:06:44.250 --> 00:06:52.750 Lynne Jones: Today, we're going to talk about, more details of some of the things we talked about yesterday. 15 00:06:53.460 --> 00:07:12.829 Lynne Jones: Code of conduct reminder, please be kind. We're here to help make Rubin the most awesome thing it can be together, so let's, be kind, be honest, be inclusive. If you do have a problem, please reach out to me, or Federica Bianco, or your science collaboration point of contact. 16 00:07:14.500 --> 00:07:28.820 Lynne Jones: Okay, quick review of what we did yesterday. We went through the current, options, and we talked about metrics, primarily in sort of a high level, over the whole survey kind of point of view. 17 00:07:29.080 --> 00:07:33.590 Lynne Jones: And today we'll talk about some particular aspects of those 18 00:07:33.720 --> 00:07:37.750 Lynne Jones: Simulations and what we're… what we're actually seeing. 19 00:07:38.870 --> 00:07:43.720 Lynne Jones: From data management, from, various aspects. 20 00:07:44.710 --> 00:07:47.150 Lynne Jones: And at the end of today, we have the… 21 00:07:47.270 --> 00:07:53.710 Lynne Jones: the, a time to talk more specifically about DESI. So… 22 00:07:53.860 --> 00:08:04.279 Lynne Jones: that we'll… we will cover that today, and David, I see you're here. I wasn't able to… to make sure we had the right time, but I think you're up for… for doing… 23 00:08:04.470 --> 00:08:08.049 Lynne Jones: If we're talking about Desi in that last section a little bit, right? 24 00:08:08.210 --> 00:08:09.590 David Schlegel: I'm here all day. 25 00:08:09.590 --> 00:08:11.000 Lynne Jones: Perfect, thank you. 26 00:08:12.270 --> 00:08:13.340 Lynne Jones: Alright. 27 00:08:15.810 --> 00:08:21.439 Lynne Jones: Right, and on Monday, we have this, session to get feedback from the science collaborations. 28 00:08:21.820 --> 00:08:29.799 Lynne Jones: So we can adjust these times as needed for what people's feedback wants to be. 29 00:08:32.450 --> 00:08:34.230 Lynne Jones: Alright, so today. 30 00:08:34.440 --> 00:08:40.229 Lynne Jones: The first thing up is details of the, FBS configuration. 31 00:08:40.669 --> 00:08:48.070 Lynne Jones: and what we're starting the survey with. So this is the chunk of today that is quite dense, and 32 00:08:49.700 --> 00:09:02.040 Lynne Jones: it's hard to talk about the FBS and how it's doing what it's doing in a way that makes sense to people without actually telling you a little bit about what's going on inside the FBS. So that's what I'm going to do. 33 00:09:02.350 --> 00:09:03.870 Lynne Jones: And, 34 00:09:04.280 --> 00:09:16.860 Lynne Jones: If you have absolutely no interest in the inner workings of the FBS, this might not be for you, but I actually think it's pretty fascinating, so hopefully it'll be interesting to you, too. Some of this might be a little bit, 35 00:09:17.170 --> 00:09:20.480 Lynne Jones: fast going through, because, like I said, we… 36 00:09:20.890 --> 00:09:31.630 Lynne Jones: We made the time… the agenda before we made the… before we figured out exactly what had to go in this pot, and but I'm gonna… I'm gonna try for that. 37 00:09:32.320 --> 00:09:39.079 Lynne Jones: Anyway, here we go. Light introduction to the inside of the FBS, and what that means for the start of the survey with V5.3. 38 00:09:39.750 --> 00:09:42.399 Lynne Jones: So… Inside the FBS. 39 00:09:42.800 --> 00:09:57.940 Lynne Jones: how… what we have is the whole scheduler configuration, and inside the FES, there is a list of lists of surveys. The list is what we call tiers, so it's like, this is… you can think of it as prioritizing. 40 00:09:58.100 --> 00:10:02.639 Lynne Jones: A higher tier always has priority over a lower tier. 41 00:10:03.590 --> 00:10:11.369 Lynne Jones: So if we put deep drilling over, a tier with lots of pairs, if the deep drilling survey can request an observation, it will. 42 00:10:11.680 --> 00:10:31.370 Lynne Jones: Within a tier, those surveys compete. So if you have multiple surveys inside a tier, they can compete with each other to say, oh, I really want this observation, or, somebody else may say, I kind of want this one, but they'll go side to side-to-head to see which survey is going to choose the observation for the… 43 00:10:31.800 --> 00:10:33.980 Lynne Jones: Upcoming observations be taken. 44 00:10:34.620 --> 00:10:35.680 Lynne Jones: So… 45 00:10:35.970 --> 00:10:50.339 Lynne Jones: So this is important to keep in mind. We have this concept of tiers, which are priority. If a higher tier survey can take an observation, even if it's a lower priority for that survey than one in a lower tier, the higher tier survey will win. 46 00:10:50.790 --> 00:10:55.259 Lynne Jones: So, tiers prioritize, and then within a tier, the surveys compete. 47 00:10:56.660 --> 00:11:00.219 Lynne Jones: That's the basics. The next thing is, what are surveys? 48 00:11:00.530 --> 00:11:20.120 Lynne Jones: So not every survey makes decisions in the same way, and this is not just true of, like, what goes into the decision in a particular survey, but that they also have different decision-making methods. And so, Peter says, you know, it's a modular decision tree, so we have some of those modules are the tiers 49 00:11:20.120 --> 00:11:39.759 Lynne Jones: And then, within the tiers, the decisions from the surveys. But also, it's because there's a modular range of surveys. So we have things like scripted surveys, which take a list of desired observations, along with some constraints, like, the time window, the hour angle, what the sun altitude is. 50 00:11:39.920 --> 00:11:48.779 Lynne Jones: And then it will try to acquire the observations in that list when the constraints for those… that particular observation is matched. 51 00:11:49.140 --> 00:12:00.000 Lynne Jones: So we use this for the deep drilling fields, you could also use it for engineering tests, and there's lots of use for this, but it's a very, sort of, prescriptive survey. 52 00:12:01.470 --> 00:12:04.100 Lynne Jones: If something can be done, it will, basically. 53 00:12:04.760 --> 00:12:07.160 Lynne Jones: And then we have, 54 00:12:07.180 --> 00:12:26.459 Lynne Jones: Markov, which is our… we actually have many subclasses of this kind of survey. It's basically saying this is a survey that uses a lot of basis functions, potentially a lot of basis functions, to make decisions about which observation to take, and we use these for a wide area survey, for the most part. 55 00:12:26.620 --> 00:12:32.120 Lynne Jones: Sometimes we use them for more like a single pointing, and those are field surveys. They are… 56 00:12:32.450 --> 00:12:36.150 Lynne Jones: They're related, they're… it's just they only have one. 57 00:12:36.590 --> 00:12:38.190 Lynne Jones: Position on the sky. 58 00:12:39.510 --> 00:12:54.449 Lynne Jones: For field surveys, you can put in a sequence to be… to be obtained every time you… that survey would request an observation. For the Markov surveys, it's more like you choose one observation, but you can choose it based on anywhere on the sky. 59 00:12:55.070 --> 00:13:10.659 Lynne Jones: Now, really, to fully define a survey, you also… and to know, like, this survey is this survey, and not a slightly different survey. You do have to dig into all of the basis functions to say, like, how is this survey making its decisions? 60 00:13:10.660 --> 00:13:15.729 Lynne Jones: I am not going to go through all of the basis functions for every survey. 61 00:13:16.350 --> 00:13:20.820 Lynne Jones: Here, because that would not be interesting to people, and it would be very long. 62 00:13:20.910 --> 00:13:31.330 Lynne Jones: But for now, let's just say that for most of the Markov-based surveys, the typical balance we look for is between the footprint, the, 63 00:13:31.370 --> 00:13:46.250 Lynne Jones: what we call M5 difference, which is the 5-sigma point source limiting magnitude that we estimate you would have now over the sky versus the dark sky depth. So it's an estimate, not just of where it's, where it's, 64 00:13:46.580 --> 00:13:53.279 Lynne Jones: Where you have the most limiting magnitude right now, but also just compared to what that would be under dark sky conditions. 65 00:13:53.410 --> 00:13:57.330 Lynne Jones: And then we have, a slew time basis function. 66 00:13:57.990 --> 00:14:06.030 Lynne Jones: And these are sort of our big three. You can think of as, like, if you have a wide area survey, these are the big three. 67 00:14:06.340 --> 00:14:18.319 Lynne Jones: basis functions that you'll be trying to balance. And it goes so that you have in… you can balance even coverage, efficient observations with the slew time, and 68 00:14:18.670 --> 00:14:20.750 Lynne Jones: Photon collection with the depth. 69 00:14:22.540 --> 00:14:28.609 Lynne Jones: And there's… there's numbers that you can use to change how these balance against each other, for example. 70 00:14:28.800 --> 00:14:35.769 Lynne Jones: These are all some of the things that go into making a full survey configuration, but this is the basic, basic. 71 00:14:36.800 --> 00:14:42.119 Lynne Jones: And then another thing we do for the use at the summit, is we have 72 00:14:42.270 --> 00:14:53.789 Lynne Jones: some standard masks, which we apply to every survey. And these are basically that we're… we're putting in the administrative constraints, or the just general con… 73 00:14:54.140 --> 00:14:59.639 Lynne Jones: A little bit more than that because of Venus and Jupiter, but these are constraints that every survey will follow. 74 00:14:59.870 --> 00:15:09.239 Lynne Jones: So we have, avoiding the moon, by about 30 degrees. Every survey will respect the altitude limits for the telescope. 75 00:15:09.630 --> 00:15:28.509 Lynne Jones: So we don't… so this will mask off the sky below our lower limit and around zenith. And every survey, in the FES avoids Venus, Mars, and Jupiter, merely because they're so bright and they move fast, so it's just not worth, us looking at them. 76 00:15:29.600 --> 00:15:39.199 Lynne Jones: And we can also add temporary masks, so for example, if we need to avoid a given azimuth range on a particular night, we can… we can add this in. 77 00:15:43.360 --> 00:15:47.360 Lynne Jones: So that's the basics of what goes into 78 00:15:49.140 --> 00:15:57.690 Lynne Jones: our FPS configurations on the sky. And, like, this is the specifics for what we have now in V5.3. 79 00:15:57.970 --> 00:16:02.689 Lynne Jones: So, you can see there's a lot of things on this list. We have 8 tiers. 80 00:16:03.210 --> 00:16:15.289 Lynne Jones: And then within those tiers, we have 40 surveys, but all those are not necessarily in the same tier, so those 40 surveys aren't all competing against each other, they're only competing within their same tier. 81 00:16:17.010 --> 00:16:33.589 Lynne Jones: Okay, so when we say this is what the FES is doing, what we mean is at a particular time, the FES gets updated with the conditions, so the… where the telescope is, what the seeing is like, what the weather's like, what the sky brightness is. 82 00:16:34.380 --> 00:16:48.630 Lynne Jones: And then it goes through this list of tiers until it comes to a tier that says, yes, this is perfect, I can take an observation now, and then that tier will choose an observation. 83 00:16:48.800 --> 00:16:50.370 Lynne Jones: For the survey. 84 00:16:51.250 --> 00:17:02.650 Lynne Jones: For the whole survey. This is where it gets a little tricky. So we have our survey objects, and then we have the survey we're doing, but here, I mean, I'll try to make sure I'm saying survey by the survey objects. 85 00:17:02.840 --> 00:17:03.700 Lynne Jones: So… 86 00:17:06.540 --> 00:17:15.980 Lynne Jones: These are our tiers. I'm going to go through each tier and just say this is the kind of observations this would take and what they look like in our 5.3 simulation. 87 00:17:17.180 --> 00:17:21.450 Lynne Jones: So we have the target of opportunity tier, the TO tier. 88 00:17:22.390 --> 00:17:38.650 Lynne Jones: This, is a set of… basically a set of scripted observations that are waiting for information that says, oh, this event happened. If the event matches the type of object it's supposed to follow up, then it follows the scripted, 89 00:17:38.720 --> 00:17:45.030 Lynne Jones: the predefined observation plan, which comes from the 2024 TO Workshop Report. 90 00:17:45.870 --> 00:17:47.060 Lynne Jones: So… 91 00:17:47.180 --> 00:17:57.620 Lynne Jones: this is a top-tier survey, the very top tier, so if a TO event comes in, and a survey… one of these, TOO surveys. 92 00:17:57.990 --> 00:18:12.299 Lynne Jones: matches the event, and the observations are possible, like, the list of observations from a scripted survey says, yes, this matches the conditions, then this will be the next thing that's observed. 93 00:18:14.830 --> 00:18:31.000 Lynne Jones: I'm gonna introduce here, not just our sky plot on the left, but on the right. This is an LTAS distribution of where those observations were in V5.3. So you see, these are… these are being picked up over 94 00:18:31.670 --> 00:18:39.380 Lynne Jones: On the left, you can see over it pretty much all over the sky, and that's, by chance, of course, because… 95 00:18:39.580 --> 00:18:42.000 Lynne Jones: We don't know where the real TOs are going to be. 96 00:18:42.420 --> 00:18:49.230 Lynne Jones: And on the right is, like, telling you where, from the telescope's point of view, it was observing in order to 97 00:18:49.390 --> 00:18:52.459 Lynne Jones: to see these duos. 98 00:18:54.660 --> 00:19:06.640 Lynne Jones: Our next tier is, a survey that's trying to coordinate with the Roman Galactic playing field. So, this results in… it's set up to obtain about, 99 00:19:06.640 --> 00:19:16.030 Lynne Jones: just over 2,000 visits, spanning 5 years. This is frequent monitoring while the field is available, so… and it goes through GRIZ bands. 100 00:19:16.060 --> 00:19:18.359 Lynne Jones: And the idea is to coordinate with Roman. 101 00:19:18.600 --> 00:19:30.550 Lynne Jones: This does not request any observations within year one, and it is a survey that we need to update and make sure we're actually coordinating, because we don't have this full information yet. So… 102 00:19:30.650 --> 00:19:37.280 Lynne Jones: These observations in the full 5.3 simulation are a little bit of a placeholder, but it's about what we want to do. 103 00:19:40.760 --> 00:19:45.690 Lynne Jones: Our next year is… The deep drilling fields. 104 00:19:46.870 --> 00:19:52.710 Lynne Jones: So, this is a single scripted survey containing all of the predefined DDF 105 00:19:53.340 --> 00:20:00.129 Lynne Jones: desired observations. So this survey is configured a little bit differently than a lot of our other things. 106 00:20:00.300 --> 00:20:10.979 Lynne Jones: For a scripted survey, you basically can give it a list to say ahead of time, to say, here, these are the observations I want to take. Please try to take these observations if you can. 107 00:20:11.960 --> 00:20:14.939 Lynne Jones: And obviously, each of those observations come with 108 00:20:15.050 --> 00:20:23.670 Lynne Jones: Some constraints, the most important of which is usually the time window that that observation could be acquired in. 109 00:20:24.810 --> 00:20:33.960 Lynne Jones: So, to set up our desired DDF observations, we optimize those independently ahead of time. And this is so that 110 00:20:34.320 --> 00:20:46.219 Lynne Jones: because these are a very limited set of pointings, we can do this. We can say, when would be the best time to observe this field when we have this particular number of observations we want to get in the season. 111 00:20:46.580 --> 00:21:01.559 Lynne Jones: With some cadence constraints, perhaps, and then pick the best time in the night based on the sky brightness, to obtain that observation. And also, that way we can skip times when the moon is bright, and so on. 112 00:21:03.050 --> 00:21:20.200 Lynne Jones: So, the DDFs are handled a little bit differently than most of the other things. We're going ahead, before we even get to the survey to say, this is when we should take these observations over the season. Obviously, we don't know when the weather's going to be good or bad, but that's where the scripted survey can handle that. 113 00:21:20.250 --> 00:21:26.830 Lynne Jones: Because you can give it each of those observations, a time window of when to… to actually run. 114 00:21:27.830 --> 00:21:34.509 Lynne Jones: So when we set up our list, we take into account the time window and flexibility, for example. 115 00:21:35.650 --> 00:21:39.809 Lynne Jones: So, the… we have, again, on the bottom here, the… 116 00:21:39.910 --> 00:21:52.520 Lynne Jones: RADEX, distribution on the sky for the deep drilling fields. I think this is fairly familiar to most people. In the middle, the distribution of those visits over altitude and azimuth. 117 00:21:52.520 --> 00:22:00.579 Lynne Jones: And this is kind of interesting because you can see that there's this little hole in the middle. You probably can't see my mouse cursor, but there. 118 00:22:00.660 --> 00:22:06.259 Lynne Jones: I mean, that's the zenith exclusion region, because we can't track the telescope through zenith. 119 00:22:06.630 --> 00:22:11.090 Lynne Jones: So we can observe on either side of Zenith, but not right at Zenith. 120 00:22:11.580 --> 00:22:18.019 Lynne Jones: And then on the right, here is now, another new plot. So what this one shows is… 121 00:22:18.260 --> 00:22:25.359 Lynne Jones: On the y-axis, it's time away from local midnight, and on the x-axis, it's just, 122 00:22:25.650 --> 00:22:27.890 Lynne Jones: Basically, the night of the survey. 123 00:22:27.920 --> 00:22:46.319 Lynne Jones: So, you can see the length of the night changing over… this is just the first two years of the survey. So, you can see the length of the night changing with those red lines getting narrower and then wider. And then the times of the deep drilling fields and their filters are shown by the little lines on the inside. 124 00:22:46.940 --> 00:22:49.729 Lynne Jones: And it is a little bit hard to, 125 00:22:50.500 --> 00:23:03.979 Lynne Jones: There's a problem with, like, scale and how much data you're trying to show, so some of these points in the plot are not super easy to see, but hopefully you were able to pick up the link to my slides. 126 00:23:04.160 --> 00:23:07.189 Lynne Jones: But you can… what you can see here is that 127 00:23:07.350 --> 00:23:10.770 Lynne Jones: As the field becomes available, we observe the field. 128 00:23:11.390 --> 00:23:15.190 Lynne Jones: At the best time of the night for, 129 00:23:15.520 --> 00:23:26.959 Lynne Jones: for the time where the field is visible. And then you can see the similar thing happening for, like, the other fields, because this is all the deep join fields together. They're not quite at the same RA, but they're very clustered. 130 00:23:27.110 --> 00:23:29.550 Lynne Jones: And then began the same. 131 00:23:31.130 --> 00:23:34.939 Lynne Jones: So that, that is all of the deep drilling fields, so they have slightly different 132 00:23:35.080 --> 00:23:40.069 Lynne Jones: RA ranges and times, but you can see how we're observing, 133 00:23:42.140 --> 00:23:51.269 Lynne Jones: At the best… hopefully at the best time of the night for all of those that we've chosen the time when the sky brightness is the best. 134 00:23:52.080 --> 00:23:53.600 Lynne Jones: Alright, so… 135 00:23:55.610 --> 00:24:10.119 Lynne Jones: Right, I need to say a little bit more about the deep drilling fields. For each deep drilling visit, we have, rotational and translational dithers applied. It's a 3-degree rotational dither between visits, so until we change the filter, we just… 136 00:24:10.380 --> 00:24:19.390 Lynne Jones: Click along by 3 degrees. And then the translational offset is a radial dither around the field center of 0.2 degrees. 137 00:24:19.660 --> 00:24:27.599 Lynne Jones: For, the Euclid deep drilling field, it's a little bit different, because we don't do a radial dither, we do dither towards the other field, but 138 00:24:27.920 --> 00:24:33.080 Lynne Jones: It's… it's easier to just describe these for the rest of the deep drilling fields. 139 00:24:33.520 --> 00:24:35.580 Lynne Jones: The sequences, 140 00:24:35.880 --> 00:24:48.199 Lynne Jones: For these… the sequences we set up in the pre-calculated requests, so this is what we're trying to obtain, are in deep seasons, those are the shallow seasons or deep seasons, 141 00:24:48.940 --> 00:24:58.669 Lynne Jones: It alternates. So on even days, we would get two visits in G and 2 visits in I, and on odd days, we'd get two visits in R and 2 visits in C. 142 00:24:59.520 --> 00:25:09.719 Lynne Jones: And then every few days, so that it lines up with these, but it's not quite every day, we have 3 visits in U and 2 visits in Y. 143 00:25:09.750 --> 00:25:26.850 Lynne Jones: So, as I said, we have time windows for each of these, so you can think of them as expiring. So, the even and odd don't build up over multiple days. They expire very quickly. The U and Y, expire a little bit more slowly, so they can occasionally double up, and so we would get 6 in U. 144 00:25:27.060 --> 00:25:29.110 Lynne Jones: Or foreign and Y. 145 00:25:30.670 --> 00:25:38.529 Lynne Jones: For the EDFS field, the sequences are the same, but the cadence, the frequency, is slower to accommodate the double pointing. 146 00:25:40.340 --> 00:25:53.319 Lynne Jones: And then in ultra-deep seasons, we still have the same even-odd day sequences, but then we also add, frequent, but not everyday, sequences of 147 00:25:53.470 --> 00:25:57.290 Lynne Jones: 8 in U, 4 in G, 18 in R, 148 00:25:57.560 --> 00:26:02.420 Lynne Jones: 55 in I, 52 in Z, and 20 in Y band. 149 00:26:02.800 --> 00:26:07.280 Lynne Jones: So this is very, very red-heavy. 150 00:26:07.470 --> 00:26:12.250 Lynne Jones: And the idea is that this is looking for a high redshift supernova. 151 00:26:19.520 --> 00:26:21.810 Lynne Jones: Now we move along to the template tier. 152 00:26:21.920 --> 00:26:25.470 Lynne Jones: Please do go ahead and raise your hand if you have questions while we're going through here. 153 00:26:28.290 --> 00:26:32.289 Lynne Jones: Okay, so let's talk about tier. This is our new tier. 154 00:26:32.590 --> 00:26:34.350 Lynne Jones: In B5.3. 155 00:26:34.810 --> 00:26:42.070 Lynne Jones: We're acquiring visits separated by about 25 minutes, and good image quality for the template here. 156 00:26:42.170 --> 00:26:53.259 Lynne Jones: And you can see the names of the filters that are paired together for these pairs in the list up at the top. So we have U paired with U, G with G, G also with R, R with A, R, 157 00:26:53.660 --> 00:27:08.570 Lynne Jones: R&I. So, in general, for our standard pairs, we don't pair the same filter with itself, except for Y-band, but for the template tier, because they're, we're trying to get the U-band images under 158 00:27:09.050 --> 00:27:14.230 Lynne Jones: tighter constraints for the image quality, we do pair U with itself and G with itself. 159 00:27:15.690 --> 00:27:16.640 Lynne Jones: So… 160 00:27:17.500 --> 00:27:37.219 Lynne Jones: The template tier will only request observations when the atmospheric seeing, as we're getting the measurement from the DIMM currently, implies that the predicted seeing, full width half max, sorry, for the next visit would be better than the equivalent of, 1.2 arcseconds at zenith. 161 00:27:37.340 --> 00:27:56.450 Lynne Jones: And this is a little bit, tiny bit tricky to explain, because when I say 1.2 arcseconds at zenith, we do let that vary with declination, so I have a plot on the right of what a 1.2 full-width half max at zenith translates to over the declination range of our footprint. 162 00:27:57.500 --> 00:28:01.649 Lynne Jones: Because obviously a higher deck, you don't get as good seeing. 163 00:28:02.160 --> 00:28:11.879 Lynne Jones: And so… That the… the template tier is looking for the declination appropriate, 164 00:28:12.170 --> 00:28:22.220 Lynne Jones: predicted full-width half wax at its location. And it will also only track observations which meet those, those, full-width half-max requirements. 165 00:28:22.380 --> 00:28:34.049 Lynne Jones: There are also some hour angle limits to make sure we're pushing towards Zenith, and there are some additional constraints. Otherwise, many aspects are similar to the standard pair survey. 166 00:28:34.350 --> 00:28:42.770 Lynne Jones: The template tier is important to note, shuts off when 6 visits with the desired full-width half max are acquired. 167 00:28:42.970 --> 00:28:45.650 Lynne Jones: Or at the end of year one, whichever is soonest. 168 00:28:47.130 --> 00:29:04.799 Lynne Jones: And this is in our 5.3 configuration. This is the kind of thing, like, the details of what are… is the cutoff, at Zenith, and how many visits we need, and when should it cut off. Those are things that we'll… we'll go back and adjust as we see 169 00:29:05.560 --> 00:29:11.379 Lynne Jones: As we sync up better with, data management pipeline and requirements. 170 00:29:11.530 --> 00:29:14.390 Lynne Jones: And we see what they, what they can use. 171 00:29:17.820 --> 00:29:20.520 Lynne Jones: The template tier, so this is the… 172 00:29:20.860 --> 00:29:30.849 Lynne Jones: footprint, again, on the sky in our NDAC, and the footprint in altitude and azimuth. So what you're seeing here, that wedge shape, is the hour angle constraints. 173 00:29:31.010 --> 00:29:41.319 Lynne Jones: And then, on the right is that same plot of, like, when the observations are happening. And notice this one's much shorter in time because it only runs for the first year. 174 00:29:42.370 --> 00:29:47.519 Lynne Jones: You can also, now that there's more observations on this plot, you can see, 175 00:29:47.760 --> 00:29:55.680 Lynne Jones: A blank period here, just shortly after the start of the simulation, and that's because we have a downtime period there. 176 00:29:57.310 --> 00:29:58.879 Lynne Jones: In the simulation. 177 00:29:59.530 --> 00:30:05.379 Lynne Jones: Your Casol can notice that This is taking up most of the time of the survey. 178 00:30:07.170 --> 00:30:13.769 Lynne Jones: Not all of it, but a lot of it. And actually, now I think about it, see, if you notice this stripe going through here… oops… 179 00:30:14.210 --> 00:30:20.179 Lynne Jones: That would be because that matches up with our deep drilling fields in the previous pot. 180 00:30:20.590 --> 00:30:25.390 Lynne Jones: And when the deep drilling fields are intensely taking observations. 181 00:30:27.690 --> 00:30:28.650 Lynne Jones: Okay. 182 00:30:29.040 --> 00:30:36.520 Lynne Jones: Our next tier down is triplets, because we have a desire to get a few hour timescale follow-up. 183 00:30:36.690 --> 00:30:49.939 Lynne Jones: So, what happens here is we have a pair taken near the start of the night, which then triggers a follow-up visit two to seven hours later in one of the same filters. So the first pair is GR, RI, or IZ. 184 00:30:50.010 --> 00:31:07.579 Lynne Jones: And the, follow-up visit is in one of those same filters. The pairs come from a standard pair survey, but only runs once a night, only once every four days, so there's more time constraints. And the third visit comes from one of these scripted surveys, which says, oh, you took an observation, let me put that on my list to follow up. 185 00:31:08.680 --> 00:31:20.350 Lynne Jones: There are some hour angle constraints on the first pair, so we push it into parts of the sky which are rising, so we don't accidentally, like, make sure that we couldn't opposite reserve later. 186 00:31:21.500 --> 00:31:27.069 Lynne Jones: And then here you can see what happens. So we have the first pair. 187 00:31:27.460 --> 00:31:43.460 Lynne Jones: being pushed into the parts of the sky that are rising, and then you have the second visit of the pair, or sorry, the triplet after the pair, occurring at a wider range of positions on the sky. Because of that, it could be anywhere from 2 to 7 hours later. 188 00:31:43.520 --> 00:31:47.659 Lynne Jones: And then these are the same plots here, but this is the first part, first pair. 189 00:31:47.800 --> 00:31:50.769 Lynne Jones: So you can see it's stacked up near the start of the night. 190 00:31:50.950 --> 00:31:53.410 Lynne Jones: And only happening once per night. 191 00:31:53.620 --> 00:31:57.980 Lynne Jones: And then, the second… the triplet, sorry. 192 00:31:58.400 --> 00:32:03.930 Lynne Jones: Second survey, triplet of the pair, happening at various other times during the night. 193 00:32:05.870 --> 00:32:16.330 Lynne Jones: Okay, and now we come to our parent survey, which is fairly far down in the tiers, but this is actually the workhorse of our survey. More than 60% of the visits actually come from this tier. This is the… 194 00:32:16.810 --> 00:32:29.490 Lynne Jones: the standard pairs all over the sky, survey that we have. So this is where we're, again, we're balancing the M5 difference, the footprint, the slew times, make generally balanced choices, and then 195 00:32:29.490 --> 00:32:40.000 Lynne Jones: We add some extra basis functions to do things like make sure we get, at least 4 visits per pointing in each band per year, 196 00:32:40.480 --> 00:32:47.520 Lynne Jones: So that we don't try to take more than two visits per night at any point in the sky. The pairs are, 197 00:32:47.760 --> 00:32:50.440 Lynne Jones: The first visit of… of… 198 00:32:50.790 --> 00:32:56.969 Lynne Jones: The pair is followed by a second in a different filter, and you can see the filter combinations up at the top. 199 00:32:57.410 --> 00:32:58.290 Lynne Jones: But… 200 00:32:58.620 --> 00:33:15.029 Lynne Jones: And we… the goal revisit time for the second visit in the pair is 33 minutes, and you can see on this plot here, which is, over the whole sky, what is the typical time to coming back to the field, that we do have this good, strong peak at, 201 00:33:15.090 --> 00:33:29.609 Lynne Jones: 33 minutes. You also see this peak here, and this is just because of how this metric works, and this is from field overlaps. So when we take a visit, we're most likely to take the next visit right next to it, and then that gives us a little bit of overlap, so that has a very short 202 00:33:30.980 --> 00:33:33.520 Lynne Jones: Interval between visits in there. 203 00:33:34.580 --> 00:33:41.150 Lynne Jones: So, at 5.3, one of the new things we've done is that the visits in the pair 204 00:33:41.380 --> 00:33:51.260 Lynne Jones: The interval is trying to make 33 minutes, but it will scale that slightly depending on, the best visit time available. 205 00:33:51.360 --> 00:34:02.639 Lynne Jones: Sorry, how to best fill the time of the night. So the goal is 33 minutes, that's the most common time, but it can range, coming from the same survey, anywhere from, like, 40, 20, 206 00:34:02.840 --> 00:34:04.410 Lynne Jones: to, 207 00:34:05.260 --> 00:34:12.500 Lynne Jones: It's 40 or 45 minutes, or something like that. So we… it could be a little bit longer, depending on how much time you have in the night. 208 00:34:13.500 --> 00:34:31.080 Lynne Jones: This replaces, in our… if you were more familiar with our old survey configuration, we had this 15-minute pair and a 33-minute pair. We've consolidated them with this, dynamic time scaling. We only have this one pair survey now. So, this is good, simplifies by… 209 00:34:31.909 --> 00:34:34.949 Lynne Jones: How are these observing over the whole sky? 210 00:34:35.120 --> 00:34:36.540 Lynne Jones: Pretty much everywhere. 211 00:34:36.960 --> 00:34:52.209 Lynne Jones: And then on the right, you see this same plot of visits over time from 5.3, and notice there's very few visits in pairs in the first year, and that's because most of the time we're taking templates. And then after the template tier shuts off, we start taking, pairs. 212 00:34:52.750 --> 00:34:56.150 Lynne Jones: the standard pairs. Remember, the templates are in pairs as well. 213 00:34:57.790 --> 00:35:01.890 Lynne Jones: Alright, now we have one of our microsurvey, 214 00:35:02.540 --> 00:35:19.560 Lynne Jones: tiers, our only microsurvey tier, and this is the Twilight Near Sun microsurvey. It takes observations in RI and Z. It's trying to get low, solar elongation, nearly ecliptic, observations during twilight, so it… 215 00:35:20.120 --> 00:35:25.680 Lynne Jones: runs, it will only start if the sun altitude is, 216 00:35:25.930 --> 00:35:32.739 Lynne Jones: above minus 15 during this time period, and it does short exposures, 15 seconds. So… 217 00:35:33.620 --> 00:35:37.829 Lynne Jones: It runs in the target area. It defines a target area. 218 00:35:38.410 --> 00:35:56.900 Lynne Jones: One of these RIZ will win in that tier, and then it will try to get four images for pointing in the target area. And the area means that the total time we need to complete the whole microsurvey in, like, the morning or night of when it's triggered is about 20 minutes. 219 00:35:57.940 --> 00:36:05.000 Lynne Jones: So… These do successfully get low solar elongation visits, you can see that on the right. 220 00:36:05.360 --> 00:36:09.939 Lynne Jones: And you can also see that these are being pushed to the, 221 00:36:10.670 --> 00:36:14.269 Lynne Jones: The far edges of the, of the, 222 00:36:15.210 --> 00:36:22.310 Lynne Jones: Of the sky, and this triggers in the morning and the evening, but not every day, it's every, 4 days. 223 00:36:22.780 --> 00:36:23.440 Lynne Jones: I think. 224 00:36:23.690 --> 00:36:24.500 Lynne Jones: Yes. 225 00:36:27.210 --> 00:36:43.329 Lynne Jones: All right, and then the very last tier we have is the greedy tier. So, this tier serves as a filler. When no other survey can schedule visits, the greedy survey is there for you. It just schedules one visit at a time, and it doesn't, 226 00:36:43.600 --> 00:37:03.390 Lynne Jones: have a lot of other time constraints. It sort of is discouraged from revisiting the same part of the sky more than once in a night, but other than that, it just is going to balance what's the depth, what's the footprint, what's the sleeve time, so that it can make generally balanced choices. But there are no pairs required, there's no, 227 00:37:03.490 --> 00:37:05.879 Lynne Jones: You must finish, 228 00:37:06.070 --> 00:37:16.959 Lynne Jones: because it's only one visit, it doesn't have to consider too far into the future. And so, a lot of those other basis functions from all of the other surveys have dropped. It's simple, 229 00:37:17.150 --> 00:37:25.550 Lynne Jones: You wouldn't want to take most of your survey visits like this, because it also does things like get trapped in particular areas of the sky, but 230 00:37:26.000 --> 00:37:28.440 Lynne Jones: Yeah, this is our… this is our… 231 00:37:28.730 --> 00:37:31.650 Lynne Jones: our single visits over the sky. 232 00:37:31.770 --> 00:37:35.659 Lynne Jones: Backing up everything else. This runs in RIZNY. 233 00:37:38.730 --> 00:37:55.539 Lynne Jones: Look at that, I made it through all of the tiers. I'm actually going to talk a little bit about, like, what else went into our simulations and what we didn't know next, so if there are questions about, like, the survey configuration itself, the scheduler configuration. 234 00:37:55.780 --> 00:37:58.550 Lynne Jones: Could, take just a quick moment. 235 00:38:02.400 --> 00:38:03.420 Lynne Jones: David? 236 00:38:03.730 --> 00:38:11.679 David Schlegel: Yeah, for the wide, fast, deep survey, then, is that… that's the combination of the template survey and then the para-survey? 237 00:38:12.380 --> 00:38:18.830 Lynne Jones: So, this… this is a great question, actually. I didn't… really, 238 00:38:19.190 --> 00:38:34.840 Lynne Jones: So the… so the wide, fast, deep is more of, like, an area and goal number, of visits over the sky. So, when we define the footprint that goes into the greedy survey, or the pairs survey, or the temp… 239 00:38:35.430 --> 00:38:41.289 Lynne Jones: Not so much the template, but a little bit the template. But when we define the footprint that goes in here. 240 00:38:41.720 --> 00:38:51.290 Lynne Jones: and the greedy survey. We use our footprint over the whole sky, and so the whitefast deep footprint is encoded into… 241 00:38:51.490 --> 00:38:54.890 Lynne Jones: That information that we pass to each of these surveys. 242 00:38:55.130 --> 00:38:56.180 Lynne Jones: So… 243 00:38:57.680 --> 00:39:06.590 Lynne Jones: The Wide Fast Deep… there is not really a survey that is charged with acquiring Wide Fast Deep from the scheduler point of view. 244 00:39:07.270 --> 00:39:17.759 Lynne Jones: The… where this comes in is that we, as the survey strategy team, know what our coverage should be, and so we say, yes, that's what the footprint should look like, so that we do have a wide, fast, deep area. 245 00:39:18.040 --> 00:39:29.299 Lynne Jones: And then we put… place that into the footprint. And because we know we want pairs in the YFSD, most… we arrange things so that the pair survey gets most of those visits. 246 00:39:31.570 --> 00:39:41.689 Lynne Jones: So… From within the scheduler configuration, there really is no Wide Fast Deep versus North Ecliptic spur. 247 00:39:42.230 --> 00:39:47.160 Lynne Jones: But that all goes in as part of the information we feed into the survey. 248 00:39:47.380 --> 00:39:54.759 David Schlegel: So, sorry, just a quick follow-up. So, but it must be that things like the twilight observations wouldn't count towards that coverage? 249 00:39:55.170 --> 00:39:57.240 Lynne Jones: Yeah, so, so… 250 00:39:58.040 --> 00:40:16.579 Lynne Jones: Also a good question. This is true, because every one of these surveys that I talked about, you not only have the option to mask off parts of the sky, but you can also tell it to ignore certain kinds of observations. So there is a piece of metadata that actually gets into all of the 251 00:40:16.580 --> 00:40:29.940 Lynne Jones: information from the visits that is later available to everybody, called the scheduler note. And this is our piece of metadata that sort of tracks which of these surveys it came from, and sometimes extra information as well. 252 00:40:30.540 --> 00:40:41.380 Lynne Jones: And so, when this visit comes from the Twilight Near Sun Survey, it carries a piece of information that says, this came from the Twilight Near Sun Survey. 253 00:40:41.510 --> 00:40:42.880 Lynne Jones: And so… 254 00:40:43.310 --> 00:40:50.769 Lynne Jones: The pair survey is told, ignore those. Those are not relevant for you, you don't use that to build up the footprint. 255 00:40:51.220 --> 00:40:53.730 Lynne Jones: So… 256 00:40:53.890 --> 00:41:05.339 Lynne Jones: that's how… that's how this works. And we also tell the the par survey, for example, to ignore the TOO's observations, because they were putting dents in our footprint. 257 00:41:05.450 --> 00:41:10.269 Lynne Jones: And so there's… There's a lot of… 258 00:41:10.400 --> 00:41:14.240 Lynne Jones: Room to go in and think about, like, how can you… 259 00:41:14.440 --> 00:41:24.080 Lynne Jones: change how the survey is behaving, and this is one of the challenges, but also one of the strengths about the FBS configuration. There's usually more than one way to do a thing. 260 00:41:29.390 --> 00:41:30.070 Lynne Jones: Bye. 261 00:41:31.030 --> 00:41:32.719 Lynne Jones: So, I will… 262 00:41:33.890 --> 00:41:53.049 Lynne Jones: Unless there's other questions. I'm gonna go and talk a little bit about, like, so yesterday we talked about the V5.3 simulation, we talked about, oh, there's 10% lost visits in the 5.3, yeah, sorry, Sarah pointed out the trip list here also contributes to YFAST. There's a lot of things that contribute to WideFastD. 263 00:41:53.130 --> 00:41:54.990 Lynne Jones: And even the greedy survey does. 264 00:41:55.690 --> 00:42:01.869 Lynne Jones: So, yesterday we said there's 10% fewer visits in V5.3. 265 00:42:02.530 --> 00:42:19.750 Lynne Jones: And, I just want to take a moment to acknowledge that this… as Jocko did as well, right, we don't know what the weather is going to be. We also don't know some other things. So, the visit gap, the time between visits we talked about yesterday, 266 00:42:20.280 --> 00:42:26.099 Lynne Jones: I said it has some overhead that's for every slew that is kind of variable. 267 00:42:26.750 --> 00:42:32.299 Lynne Jones: And… at the moment, I think that variability might be, 268 00:42:32.480 --> 00:42:42.659 Lynne Jones: at least might lead to a variation in the total number of visits, that it may be that we get the number wrong by about 10%. 269 00:42:42.870 --> 00:42:45.990 Lynne Jones: That might be… not be too high right now. 270 00:42:46.330 --> 00:42:50.920 Lynne Jones: But after 6 months, I think that we should not be, like. 271 00:42:51.110 --> 00:43:03.710 Lynne Jones: incorrect by this much, and not just because we will know better, like, how the slew time is, but because the slew time itself will improve and match our model. But we don't know exactly how fast that's going to improve. 272 00:43:04.130 --> 00:43:08.739 Lynne Jones: And so, we didn't put it into the simulation. 273 00:43:08.870 --> 00:43:19.939 Lynne Jones: So, in the first… in the first period of time, our rate of acquiring visits in the simulation, V5.3, is probably a little bit too high. 274 00:43:21.180 --> 00:43:28.170 Lynne Jones: The actual engineering time needs. So, we put in 2 half-nights for the first 6 months. 275 00:43:28.420 --> 00:43:40.560 Lynne Jones: But that could be 2 full nights for the first 6 months. And so that kind of gives you that we might be as much as, 15% too high in the total number of visits in the first 6 months. 276 00:43:40.730 --> 00:43:48.259 Lynne Jones: But, after a full year, when… if we're not doing that engineering time anymore, which we… is not the 277 00:43:48.590 --> 00:43:50.010 Lynne Jones: current estimate. 278 00:43:50.230 --> 00:43:52.709 Lynne Jones: Then we might… we wouldn't be that 279 00:43:53.060 --> 00:43:56.129 Lynne Jones: incorrect. That number reduces over time, right? 280 00:43:57.200 --> 00:44:02.560 Lynne Jones: Also, it doesn't take into account that we might get science images from those engineering tests. 281 00:44:04.680 --> 00:44:15.250 Lynne Jones: Because sometimes they do run the FES during their engineering night, sometimes they run the very specific kinds of observations that are still valid observations for engineering. 282 00:44:15.410 --> 00:44:23.739 Lynne Jones: So there's… there's sort of uncertainty here about what is… what will happen with that engineering time, and 283 00:44:23.940 --> 00:44:26.339 Lynne Jones: What use it might be able to be used for. 284 00:44:26.780 --> 00:44:40.009 Lynne Jones: there's the fault downtime and timescale of improvement. So, we do have a model for faults in B5.3, which is an improvement over our earlier sims. I do think it's 285 00:44:40.550 --> 00:44:48.330 Lynne Jones: more accurate and relatively accurate, but there is a lot of variability on this, and so this, I think, is a little hard to say. 286 00:44:48.800 --> 00:44:57.960 Lynne Jones: I'm hoping we have guessed fairly right, but this is… it's hard to put a number on how accurate or not accurate, 287 00:44:58.420 --> 00:45:00.359 Lynne Jones: The values we've come up with are. 288 00:45:01.190 --> 00:45:18.599 Lynne Jones: Then we have the system contribution to seeing, and the timescale for improvement. So we're just not modeling this at present. We can look at doing that, especially during the first year, but also we don't know the timescale for that improvement, or, 289 00:45:20.300 --> 00:45:28.520 Lynne Jones: Or… or… what will happen there? Most likely, as we get more louvers, we'll see changes, and… 290 00:45:28.630 --> 00:45:33.159 Lynne Jones: That will be, will be something we track, for sure. 291 00:45:34.230 --> 00:45:51.240 Lynne Jones: But then we have the effects of cloud transparency, which we don't model at present, and dodging clouds, which we haven't… we're working on, and we actually have a couple of things in active development, but, 292 00:45:51.260 --> 00:45:55.170 Lynne Jones: There certainly is room for future improvement here, so… 293 00:45:55.710 --> 00:46:02.509 Lynne Jones: And then the last thing is the weather downtime. So, we don't have any clear indication of issues, but obviously we'll be monitoring this. 294 00:46:02.770 --> 00:46:11.750 Lynne Jones: So, As you look at smaller and smaller chunks of time out of V5.3.1, I think your uncertainty, 295 00:46:11.750 --> 00:46:25.889 Lynne Jones: is higher, right? As you look at the full 10 years, that's probably not as uncertain as if you're looking only at the first 6 months. So I think this is the main thing I wanted to say here, is just to make sure we… you understand, like. 296 00:46:26.150 --> 00:46:31.110 Lynne Jones: If you're looking at a small timescale, The uncertainty is definitely higher. 297 00:46:34.040 --> 00:46:34.930 Lynne Jones: Right. 298 00:46:35.120 --> 00:46:37.349 Lynne Jones: We took a couple questions along the way. 299 00:46:37.930 --> 00:46:42.190 Lynne Jones: But let's… if there's any questions here… and then I have… 300 00:46:42.540 --> 00:46:48.299 Lynne Jones: Taken up most of the, most of the question time. 301 00:46:48.620 --> 00:46:51.200 Lynne Jones: With the presentation up to this point, but… 302 00:46:51.300 --> 00:46:53.729 Lynne Jones: We'll move on to TOs a little bit late, maybe. 303 00:46:55.390 --> 00:46:59.700 Lynne Jones: Okay, so if there's any questions… Or comments? 304 00:47:00.170 --> 00:47:02.730 Lynne Jones: About this part, we can take them here. 305 00:47:12.150 --> 00:47:13.970 Lynne Jones: R&I, okay. 306 00:47:19.130 --> 00:47:23.550 Lynne Jones: Well, in which case… I'm on time. 307 00:47:24.940 --> 00:47:37.379 Lynne Jones: So, targets of opportunity. We have the… I talked about the target of opportunity tier, and… 308 00:47:37.500 --> 00:47:39.499 Lynne Jones: What it, 309 00:47:39.950 --> 00:47:48.049 Lynne Jones: just briefly, like, how it works. Like, we have these… this list of scripted surveys that are all in the TOO tier, 310 00:47:48.240 --> 00:47:51.780 Lynne Jones: They would compete against each other, but it's just that we don't… 311 00:47:51.920 --> 00:47:55.410 Lynne Jones: expect to get, multiple TOs at the same time. 312 00:47:58.100 --> 00:48:01.280 Lynne Jones: If we did, they would just queue up behind each other. 313 00:48:02.030 --> 00:48:07.479 Lynne Jones: Up to 3% of the survey time may be directed to TOL follow-up. 314 00:48:07.600 --> 00:48:14.719 Lynne Jones: The general plans for TO follow-up at present are well described in this, 2024 TO Workshop report. 315 00:48:15.010 --> 00:48:16.319 Lynne Jones: There… 316 00:48:16.730 --> 00:48:27.360 Lynne Jones: There is another follow-up report, so Sean McBride has been doing a lot of work with the observatory, 317 00:48:27.700 --> 00:48:29.200 Lynne Jones: To, to sort of… 318 00:48:29.440 --> 00:48:41.190 Lynne Jones: pull in the different TOL workshop report, and the very few cases that we didn't simulate, because they were over large amounts of area. 319 00:48:41.870 --> 00:48:45.040 Lynne Jones: And so… 320 00:48:45.220 --> 00:48:53.589 Lynne Jones: there is an update for this somewhere, and I have heard that there was a workshop this year that will probably be, 321 00:48:53.880 --> 00:48:58.059 Lynne Jones: Talking… looking into updating these follow-up plans as well. 322 00:48:58.280 --> 00:49:07.089 Lynne Jones: But what we have now, does match the TOL workshop, and also some… I'll find the link for the other documentation. 323 00:49:07.640 --> 00:49:11.590 Lynne Jones: We have a Rubin TO Advisory Board, 324 00:49:12.120 --> 00:49:19.020 Lynne Jones: This is a link to their documentation, their charge, and they provide guidance regarding specific TO events. 325 00:49:22.180 --> 00:49:29.340 Lynne Jones: Much of the TO process is intended to be automated, so we get an alert from an external program. 326 00:49:29.580 --> 00:49:42.500 Lynne Jones: It's evaluated by, the Rubin TOL Producer, which is a separate, not, not, not FBS scheduler, but it's a, Summit piece of software and framework. 327 00:49:42.830 --> 00:49:52.559 Lynne Jones: It evaluates the… the TOL producer evaluates the alert, and if it meets criteria, then it passes the alert information into 328 00:49:53.240 --> 00:50:00.980 Lynne Jones: the FBS, eventually. It goes through some systems, like the engineering facilities database, the EFD at the summit, and then it gets to the FBS. 329 00:50:01.800 --> 00:50:07.249 Lynne Jones: And so one of the FBS2O surveys, upon receiving that alert. 330 00:50:07.690 --> 00:50:14.410 Lynne Jones: We'll create the list of desired observations that match the predefined plan for that kind of table. 331 00:50:14.660 --> 00:50:17.720 Lynne Jones: And then… off we go. So… 332 00:50:18.210 --> 00:50:28.119 Lynne Jones: This… if the criteria are defined appropriately, this can all happen automatically and quickly without needing a human in the loop. 333 00:50:30.850 --> 00:50:40.540 Lynne Jones: The external events that are currently received by the TWOL producer include gravitational wave events, of the LVK alerts. 334 00:50:40.660 --> 00:50:47.119 Lynne Jones: It can obtain observations of potentially hazardous asteroids from JPL Scout. 335 00:50:48.400 --> 00:50:53.370 Lynne Jones: high-energy neutrinos from IceCube, and 336 00:50:53.900 --> 00:50:59.050 Lynne Jones: the galactic supernova from Super Kami Okande. 337 00:50:59.390 --> 00:51:09.989 Lynne Jones: The… there's another event producer that they're working on adding. It should be within the next year or so, but is not available yet. 338 00:51:11.380 --> 00:51:12.230 Lynne Jones: No. 339 00:51:12.740 --> 00:51:24.229 Lynne Jones: that's the automated route, but if the… if there is an alert or some kind of event that Ruben should follow, but is not one of these automated, 340 00:51:25.110 --> 00:51:31.910 Lynne Jones: sets of events. Then, the TO Advisory Board, whose members are listed here. 341 00:51:32.120 --> 00:51:40.460 Lynne Jones: will activate, and they will sort of activate that to you all, and they can provide guidance, on what to do here. 342 00:51:40.670 --> 00:51:41.760 Lynne Jones: So… 343 00:51:43.400 --> 00:51:56.880 Lynne Jones: The TO Advisory Board is intended to provide general guidance on the TO program on short timescales, like less than 24 hours for these things that don't fit into our current criteria and wouldn't match the 344 00:51:56.880 --> 00:52:04.290 Lynne Jones: automated response. You can do medium time scale response for 345 00:52:05.000 --> 00:52:08.420 Lynne Jones: Perhaps following up a multi-day, TO. 346 00:52:08.530 --> 00:52:21.149 Lynne Jones: And then they also do feedback on longer timescales, like weeks and months. And so one of the things, obviously, that we will have to do is keep track of how the TO events are… 347 00:52:21.970 --> 00:52:30.889 Lynne Jones: performing and how they're matching up with the rest of the survey, so that if we need to go and change the criteria for the automated triggering, then we can do that. 348 00:52:35.670 --> 00:52:43.290 Lynne Jones: The general TOL workflow looks like this, so we have our event… external event producers, LVK, IceCube. 349 00:52:43.430 --> 00:52:45.550 Lynne Jones: Super K JPL. 350 00:52:46.790 --> 00:52:53.080 Lynne Jones: And then that goes into SIMA. So Sima Hopscotch is where we receive the alerts from. 351 00:52:53.090 --> 00:53:07.550 Lynne Jones: Then this is part of the TOL producer, so it parses the alert for quality. Does it meet criteria, or does it meet criteria? Does it fail? If it's failed, it's just rejected. If it passes the quality criteria. 352 00:53:07.600 --> 00:53:15.590 Lynne Jones: Then it goes to the Rubin EFD. Then it goes to the Scheduler CSE, which is the framework that the FBS runs within at the summit. 353 00:53:16.080 --> 00:53:24.360 Lynne Jones: And then this scheduler creates an observing strategy. This is the FBS, creates this observing strategy, and then 354 00:53:25.120 --> 00:53:29.520 Lynne Jones: passes that back to the scheduler CSC, so Ruben executes the observation. 355 00:53:30.540 --> 00:53:39.920 Lynne Jones: And then afterwards, we have all of our processing to understand what the alert is. I pulled this, image from, Sean McBride's SBIE paper for this year, so… 356 00:53:40.620 --> 00:53:42.070 Lynne Jones: This is hot off the press. 357 00:53:43.640 --> 00:53:49.619 Lynne Jones: And of course, the TO Advisory Committee can decide to observe a non-standard TO 358 00:53:52.710 --> 00:54:03.399 Lynne Jones: Yeah. During commissioning, we did get a chance to test this workflow. It was, not as automated as some of the previous 359 00:54:05.320 --> 00:54:15.049 Lynne Jones: as the previous steps may have implied. But that was kind of on purpose, because we were in commissioning, and we didn't want to just be passing through alerts unexpectedly, so… 360 00:54:15.560 --> 00:54:23.330 Lynne Jones: every, alert that was actually passed to the FBS was done by hand, so we didn't get more than we expected. 361 00:54:24.080 --> 00:54:27.340 Lynne Jones: We tested the TWO workflow, of… 362 00:54:28.050 --> 00:54:33.810 Lynne Jones: passing the alerts through the EFD and into the FBS, on two… 363 00:54:34.840 --> 00:54:53.919 Lynne Jones: two, well, actually three, but let's… let's focus on these two, which got, more observations. So there was, 3i Atlas, and this was a very successful TOL program, and, resulted in, I think, probably the first paper coming out of, 364 00:54:54.530 --> 00:54:55.990 Lynne Jones: ribbon commissioning. 365 00:54:56.200 --> 00:54:58.380 Lynne Jones: in the SV survey over the summer. 366 00:54:58.680 --> 00:55:03.869 Lynne Jones: This was… this would definitely have been a non-standard TO, no matter what, 367 00:55:04.450 --> 00:55:13.919 Lynne Jones: But we did… we did observe it several times. You can see the, observation footprint here. This little spot here was, 368 00:55:14.030 --> 00:55:21.509 Lynne Jones: We were testing this by hand, remember? And this was not a mistake, it was just that, we obs… 369 00:55:21.820 --> 00:55:30.770 Lynne Jones: On one night, we tried to observe this field, and our masks in the FBS did their job and said, you cannot observe that field right now because it's too close to the moon. 370 00:55:31.210 --> 00:55:40.399 Lynne Jones: And so they said, okay, we still want to test the TOO procedure, so we're just going to put a different pointing center into the information we pass to the FBS. 371 00:55:40.430 --> 00:55:58.050 Lynne Jones: So we have this thing here, which we should have updated the labeling for, but we didn't, and so the commissioning, right? But I thought it was really great, because it also illustrated the FBS is doing its job with the masks, and it's making sure that we're not, 372 00:55:58.200 --> 00:56:02.989 Lynne Jones: We're not doing things that this… that the telescope is not supposed to do. 373 00:56:04.520 --> 00:56:10.910 Lynne Jones: On the right was our bigger follow-up, TO, so this was… 374 00:56:11.980 --> 00:56:16.769 Lynne Jones: Gravitational wave candidate, S251112. 375 00:56:17.060 --> 00:56:17.950 Lynne Jones: CM. 376 00:56:20.920 --> 00:56:30.500 Lynne Jones: we do have some work to do on our metadata, because it came through looking at, like, one. But we actually… we fixed that already, we just haven't had another chance to test it. 377 00:56:30.630 --> 00:56:45.889 Lynne Jones: So this TO was a gravitational wave that had a very large footprint, and it covered the whole sky, almost through… through here. This is the… what we deemed at the time to be the high priority area of the footprint. 378 00:56:45.950 --> 00:56:51.769 Lynne Jones: with some over here. So this, in this case, this was not a mistake, it was just a very far part of the footprint. 379 00:56:53.130 --> 00:56:56.620 Lynne Jones: And we observed this TO for a couple of nights. 380 00:56:56.810 --> 00:56:58.820 Lynne Jones: In G&I band. 381 00:56:59.290 --> 00:57:10.840 Lynne Jones: And so we followed this area, we did it again, we did it again. And so this was following the planned observations. One of the things about the… 382 00:57:10.840 --> 00:57:19.820 Lynne Jones: 3i Atlas being a non-standard TOO is that we had to actually put in the observations we wanted, because it didn't really, 383 00:57:21.900 --> 00:57:25.299 Lynne Jones: We had to make it look like one of the cases we expected. 384 00:57:25.750 --> 00:57:32.750 Lynne Jones: Okay, and over here, this one did, so we followed it. What we found was that there are… 385 00:57:33.880 --> 00:57:51.950 Lynne Jones: there were some details about how the FBS runs at the summit that are a little bit different than how it runs when we run it in a simulation. And so there were some things… there were definitely things we learned from this experience. It was also really good to see us follow this large area. 386 00:57:51.950 --> 00:57:59.219 Lynne Jones: I think it has proved difficult to process this without, like, production-grade templates. 387 00:57:59.450 --> 00:58:04.350 Lynne Jones: Yeah, and so we're… we'll see how that… Gentles. 388 00:58:05.990 --> 00:58:07.700 Lynne Jones: Okay. 389 00:58:10.060 --> 00:58:12.140 Lynne Jones: So, we have, 390 00:58:15.410 --> 00:58:20.250 Lynne Jones: Excuse me. We have… Children 391 00:58:20.600 --> 00:58:29.169 Lynne Jones: So, we did the gravitational wave case, and we learned things, and we're implementing updates for this in the FPS. 392 00:58:31.620 --> 00:58:37.259 Lynne Jones: And then we have questions for any of this so far. 393 00:58:43.070 --> 00:58:44.360 Lynne Jones: Roberta? 394 00:58:45.630 --> 00:58:55.059 Roberto Assef: Yes, thank you very much. Just a couple of very quick questions. So, is there, thinking… I'm thinking mostly of gravitational waves 395 00:58:55.060 --> 00:59:05.799 Roberto Assef: follow-up, is there a ramp-up, considering the number of requests towards the later years? Because I will assume that, sort of, this will keep increasing and increasing. 396 00:59:06.850 --> 00:59:09.790 Lynne Jones: It kind of goes, with the… 397 00:59:09.950 --> 00:59:13.680 Lynne Jones: With the observing seasons for, 398 00:59:15.050 --> 00:59:30.899 Lynne Jones: For LIGO, Virgo, for… so they're not actually spread evenly throughout the whole survey, and they are concentrated in… I think it's year 2. Peter might have a better answer on when exactly it is. 399 00:59:31.020 --> 00:59:38.100 Lynne Jones: They are concentrated in time. This is also something we'll have to consider, because obviously. 400 00:59:38.330 --> 00:59:48.510 Lynne Jones: we've said, okay, this is when we think that the alerts will be coming in, and we've based that time span and the rates on what came out of the TOO workshop. 401 00:59:48.750 --> 00:59:53.060 Lynne Jones: But… We don't know, for sure. 402 00:59:54.440 --> 01:00:13.109 Roberto Assef: Okay, and… and can I ask one more question? The… so, right, a lot of what we… what happened by the change to 5.3 was this… the last 10% lower on Sky time. So I'm wondering, is it too difficult to, sort of. 403 01:00:13.130 --> 01:00:30.990 Roberto Assef: after the fact, see if the images obtained for TO could fit within the strategies of the WFD and the DDFs. It could add to zero, because we don't know where the TOOs will be and when they will be, but if they add, that will help recover some of that. 404 01:00:32.130 --> 01:00:40.870 Lynne Jones: So… Potentially. The… I mean, and the… 405 01:00:41.730 --> 01:00:50.520 Lynne Jones: It's difficult because, when we're observing, like, with the PARS survey, or, all the other 406 01:00:50.710 --> 01:01:06.609 Lynne Jones: tiers that go into making our normal observing mode. We don't really have, a way to force it to say, okay, on tonight, actually really go do this part of the sky. So, you would still be activating a TOO, essentially. 407 01:01:06.930 --> 01:01:08.140 Lynne Jones: And… 408 01:01:08.480 --> 01:01:18.200 Lynne Jones: we… what it would be is maybe what we would… could do is make the TO gentler, but that's kind of the opposite of what you want for the TOO, right? 409 01:01:19.770 --> 01:01:36.559 Lynne Jones: So… so there… yes, there is this tension between, like, following up the TOO as it… as it ideally would be, and as quick as it would be, versus, like, doing it in a way that might just look like the normal survey. 410 01:01:37.210 --> 01:01:44.559 Lynne Jones: And… the… looking like the normal survey is… I'm not… 411 01:01:46.190 --> 01:02:04.999 Lynne Jones: Yeah. We did have… we… the reason we… so, originally, when we made TOs, we counted them towards the… the footprint for the pairs survey, but, what we found was that disturbs the cadence we're trying to get with the pairs as well. So, it's kind of like they… 412 01:02:05.020 --> 01:02:11.530 Lynne Jones: Don't go together super well, but certainly, you know, if this turns out to be a really big 413 01:02:11.720 --> 01:02:22.280 Lynne Jones: problem that we really have many more TOs than we… that we need to follow up than we can accommodate. This would be something we could go and revisit, but it… it is difficult. 414 01:02:23.450 --> 01:02:25.690 Lynne Jones: And I'm not sure it'd be successful. 415 01:02:27.170 --> 01:02:27.870 Roberto Assef: Thank you. 416 01:02:29.370 --> 01:02:30.380 Lynne Jones: Bindu? 417 01:02:31.480 --> 01:02:44.719 Bindu Rani: Yeah, hi, Lynn. Really quick, is there a fixed amount of time assigned for the TO observations? And, if it is, is there a plan, like, you know, in case if that time has not been used, 418 01:02:45.020 --> 01:02:46.710 Bindu Rani: How that time will be used. 419 01:02:46.950 --> 01:02:47.880 Bindu Rani: Otherwise. 420 01:02:48.450 --> 01:02:53.650 Lynne Jones: Yeah, good question. It's not… there is a fixed cap… well. 421 01:02:54.070 --> 01:03:05.430 Lynne Jones: in theory, a fixed cap is… we don't enforce it in the FBS. To enforce the cap on the TOs, it would have to come into, like, the criteria for triggering on the TOs. 422 01:03:05.750 --> 01:03:13.830 Lynne Jones: So… The TUL program is expected to use up to 3% of the total survey time. 423 01:03:14.520 --> 01:03:31.369 Lynne Jones: there's nothing that, like, if they… there are no TOOs, it's not like we're not observing. We just don't observe a TOO, and we do observe all the normal stuff we would observe, so all of the other tiers lower in the scheduler just would activate. 424 01:03:31.570 --> 01:03:46.380 Lynne Jones: And, like I was saying yesterday, our footprint is just a ratio, so if we have more time, we just get more observations distributed over the footprint, and if we have less time, we just get less observations distributed over the footprint. 425 01:03:46.630 --> 01:03:47.280 Bindu Rani: I still think. 426 01:03:47.280 --> 01:03:53.830 Lynne Jones: So, it just… if we… if we didn't have any TOs, we would have a little bit more time 427 01:03:54.280 --> 01:03:58.640 Lynne Jones: That would go into everything else in the survey, and if we had more TOOs. 428 01:03:59.080 --> 01:04:01.250 Lynne Jones: Then it takes the time. 429 01:04:02.900 --> 01:04:03.460 Bindu Rani: Thanks. 430 01:04:06.680 --> 01:04:07.650 Lynne Jones: Rachel? 431 01:04:09.870 --> 01:04:17.370 Rachel Mandelbaum: Yeah, hi, Lynn. Just to… to add to that and make sure I've understood properly, especially given an answer you gave to another question. 432 01:04:17.510 --> 01:04:27.969 Rachel Mandelbaum: Is it correct that, like, you know, since We do anticipate that The number of gravitational wave… 433 01:04:28.270 --> 01:04:30.680 Rachel Mandelbaum: Events will depend on, like, weather. 434 01:04:31.050 --> 01:04:35.870 Rachel Mandelbaum: whether there's, like, a LIGO ROGO CAGRA observing run on or not. 435 01:04:36.120 --> 01:04:36.580 Lynne Jones: They're. 436 01:04:36.580 --> 01:04:43.649 Rachel Mandelbaum: There might be some years where the TOO time could exceed the 3%, and the 3% is more across the whole survey. 437 01:04:43.870 --> 01:04:44.300 Lynne Jones: Yeah. 438 01:04:46.890 --> 01:05:04.580 Lynne Jones: Yeah, the… I mean, we do expect it to be variable, because most of the time in the TOs is for these very large events, which are not as frequent, so they will be bunched up. Sorry, not bunched up, but the TO time overall will be bunchy. 439 01:05:05.400 --> 01:05:09.810 Lynne Jones: I don't think we have a… 440 01:05:10.340 --> 01:05:16.210 Lynne Jones: cap on how much TOL time can be used within a particular time frame. 441 01:05:16.380 --> 01:05:21.079 Lynne Jones: And that… that is something that I think the SEOC have… 442 01:05:21.340 --> 01:05:30.740 Lynne Jones: decided to think about, but it is hard to make progress on that without understanding what the actual, 443 01:05:31.480 --> 01:05:35.500 Lynne Jones: event rate is going to be, because there's… there's uncertainty on it, so… 444 01:05:36.690 --> 01:05:45.689 Lynne Jones: And it's also hard, because it is hard then also to say, okay, what effect will that have on the rest of the observations? So… 445 01:05:46.290 --> 01:05:54.570 Lynne Jones: Yeah, I do think this is a thing that we need to think about, because it would go back to the, 446 01:05:55.030 --> 01:06:10.820 Lynne Jones: to the TO Advisory Board, and they would say, hey, this… this time is being used too… too quickly, and we should… we should change the criteria. Igor, and you are on the, TO Advisory Board, so hopefully you can say a few words. 447 01:06:10.990 --> 01:06:17.739 Igor Andreoni: Yeah, maybe just complimenting a little bit, all you've said was in response to Rachel. 448 01:06:18.160 --> 01:06:19.190 Igor Andreoni: the… 449 01:06:19.760 --> 01:06:31.860 Igor Andreoni: We have tried to rally up the community, bringing it together to discuss and develop strategies and come up with realistic budgets. 450 01:06:32.050 --> 01:06:36.700 Igor Andreoni: for TU observation requests. So this was done in 2024. 451 01:06:36.870 --> 01:06:44.269 Igor Andreoni: And we are doing it again right now. Hopefully, we will have the new documents published by the end of July. 452 01:06:44.390 --> 01:06:46.430 Igor Andreoni: So, I would suggest… 453 01:06:46.790 --> 01:06:54.749 Igor Andreoni: If you want to have, like, a preview, you can check on the archive. We have put the report from 2024. 454 01:06:54.860 --> 01:07:00.400 Igor Andreoni: I think if you search the Rubin TO program on ADS, should be the first thing that comes up. 455 01:07:00.730 --> 01:07:05.870 Igor Andreoni: Otherwise, waiting a month, you will have more solid numbers. 456 01:07:06.080 --> 01:07:15.759 Igor Andreoni: These numbers that we've come up with, try to be more or less within 3% over the course of the whole survey. 457 01:07:15.970 --> 01:07:21.110 Igor Andreoni: We are trying to be very, mindful of, 458 01:07:21.600 --> 01:07:34.260 Igor Andreoni: minimizing disruption, of course, and when I say we, I really mean everyone who is interested in TOs, from gravitational waves to other types of messengers, to, potentially hazardous asteroids. 459 01:07:34.850 --> 01:07:36.649 Igor Andreoni: In addition. 460 01:07:37.080 --> 01:07:54.649 Igor Andreoni: at the moment, the go-to policy is whenever a counterpart we're searching for is found, we stop observations, so that the other telescope with a smaller field of view can perform the follow-up if they're available. So there are… 461 01:07:54.920 --> 01:07:57.780 Igor Andreoni: I think… 462 01:07:58.620 --> 01:08:11.529 Igor Andreoni: There are ways we're actually perform… gonna perform the observations that are maybe not fully encapsulated in the simulations, because again, they're so… honestly, so difficult to predict. 463 01:08:11.690 --> 01:08:16.240 Igor Andreoni: But my hope is that the… 464 01:08:16.810 --> 01:08:20.969 Igor Andreoni: We will use the time well in a very efficient manner. 465 01:08:21.220 --> 01:08:27.159 Igor Andreoni: Possibly all the… what's available, and if not, observation will go towards 466 01:08:27.330 --> 01:08:34.739 Igor Andreoni: The minimum… all the meaningful science that can be achieved with the regular survey. 467 01:08:35.050 --> 01:08:51.330 Igor Andreoni: And all of this keeps changing. The rates, for example, for gravitational wave sources keep changing as more and more light runs are performed. And at the same time, new ideas for interesting science cases are brought up by the community. So we… 468 01:08:51.330 --> 01:09:02.239 Igor Andreoni: Every couple of years, we'll try to rethink a little bit how to structure the program and try to make it as effective and efficient as possible. 469 01:09:09.229 --> 01:09:10.109 Lynne Jones: Thanks, Igor. 470 01:09:10.539 --> 01:09:13.309 Lynne Jones: I'm glad you… I'm glad you, got a… 471 01:09:13.429 --> 01:09:16.949 Lynne Jones: Though we got to hear from somebody from the TO Advisory Board. 472 01:09:17.439 --> 01:09:18.329 Lynne Jones: Yay. 473 01:09:18.839 --> 01:09:21.839 Lynne Jones: Alright. 474 01:09:22.879 --> 01:09:27.659 Lynne Jones: And now we can move… oh, sorry, go ahead, Rob. We can take one more question here. 475 01:09:29.460 --> 01:09:43.779 Saurabh Jha: Yeah, I just wanted to follow up on, a little bit on Roberta's question. One of the things about the TOs, and I just checked in with Peter about this, was, some of the observations are using non-standard visits, so the exposure times might go up to 120 seconds in the TOOs. 476 01:09:44.180 --> 01:09:55.970 Saurabh Jha: And so, you know, whether those could be included in what becomes Wide Fast Deep, yeah, I mean, maybe, probably, but, you know, they are a little bit different than the other observations in the survey, or can be. 477 01:10:02.470 --> 01:10:12.859 Lynne Jones: Alright, excellent. And, let's move on to talking about the templates and the templates here. Eric… 478 01:10:13.060 --> 01:10:16.419 Lynne Jones: Are you… Were you, 479 01:10:17.580 --> 01:10:33.699 Lynne Jones: Oh, great. Okay. I… I… I didn't… I wasn't quite sure where to put in your slides. I was just going to say a little bit about our new option for the template tier, and then, hand… hand over to you for that. 480 01:10:33.700 --> 01:10:35.930 Eric C Bellm: That's fine, how much time do you want me to spend? 481 01:10:40.120 --> 01:10:48.399 Lynne Jones: You… you said you didn't want very long, so… I'm thinking you can… somewhere between 5 and 10 minutes. 482 01:10:48.720 --> 01:10:50.269 Eric C Bellm: Okay, that sounds fine. 483 01:10:51.190 --> 01:10:54.799 Lynne Jones: And some of that might be questions, if that works better. 484 01:10:55.130 --> 01:10:55.980 Lynne Jones: Okay. 485 01:10:56.100 --> 01:11:03.300 Lynne Jones: So, some of this I… Eric is gonna just say yes or no about, but basically. 486 01:11:03.450 --> 01:11:18.049 Lynne Jones: One of the issues we have is good template creation requires at least 5 to 6 visits, with the full-width half mics and transparency, required for the template co-add, and that's… 487 01:11:18.790 --> 01:11:25.789 Lynne Jones: Awesome. So they… so they… these are declination-dependent and band-dependent values. 488 01:11:26.650 --> 01:11:43.410 Lynne Jones: Now, the other thing is, why can't we just create bad templates and keep going? Well, bad templates are bad, because, replacing templates is bad for the… it adds offsets in the magnitudes of the alerts, so the template continuity over time is strongly preferred. 489 01:11:44.340 --> 01:11:59.090 Lynne Jones: And then the other thing is bad templates make more alerts, which then make even more alerts because of how, alert… the alert, prompt processing pipeline works, and this basically just loads up the prompt processing database with noise. 490 01:11:59.630 --> 01:12:00.500 Lynne Jones: And… 491 01:12:00.810 --> 01:12:09.850 Lynne Jones: So, we don't want to just make bad templates and keep going, so we want to make good templates, and then the problem is, if we don't 492 01:12:10.270 --> 01:12:20.599 Lynne Jones: set up the FBS to sort of have a specific push to acquire the 5 to 6 visits with good image quality and good transparency. 493 01:12:20.750 --> 01:12:34.199 Lynne Jones: at each point on the sky per band, there is a high likelihood that we would not acquire those necessary visits within year one. And this is not just a high likelihood, but almost certain in UNG with our… without the template here. 494 01:12:35.170 --> 01:12:39.999 Lynne Jones: So, this is why we added the template tier to the baseline surveys, so that we meet this need. 495 01:12:40.130 --> 01:12:50.109 Lynne Jones: Now, the… the thing we immediately did was we just put in templates… a template tier which… which acquired visits and singles, but because there's so many visits in this 496 01:12:50.280 --> 01:12:52.300 Lynne Jones: Tier in year one. 497 01:12:52.480 --> 01:13:00.680 Lynne Jones: Singles were not a good choice, so I keep saying we acquire the templates in pairs, because that actually was an important consideration. 498 01:13:05.190 --> 01:13:22.389 Lynne Jones: The next question is, can we improve on the template acquisition? Because there is still a risk that we would not complete the templates over the whole… the template inputs, we don't make the templates, that we would not get enough template inputs over the whole sky at the end of year one. 499 01:13:23.540 --> 01:13:37.990 Lynne Jones: So we have, a simulation called Faster Templates. This is in our V5.3 set of simulations. And the idea here is we need epics with dithering for the pixel coverage. 500 01:13:38.380 --> 01:13:54.149 Lynne Jones: Individually, they could be shallower, potentially, although they shouldn't be worse quality full-width half max, but because they are good quality full-width half max, perhaps they can just be a little bit shorter exposures, and it doesn't make them that much, shallower in depth. 501 01:13:55.390 --> 01:14:03.139 Lynne Jones: So… This simulation poses a question, what if we take the template image, the template visits. 502 01:14:03.520 --> 01:14:09.770 Lynne Jones: As 20-second images, increasing the number of epics, 503 01:14:09.970 --> 01:14:23.109 Lynne Jones: As… versus what we would have if we just took them as 30-second visits. Now, so, U-band is special, as always, because U-band is 38 seconds in a standard visit, and it would go down to 25 seconds in these shorter visits. 504 01:14:24.540 --> 01:14:39.610 Lynne Jones: Now, this is not just for us to say, because there's lots of impacts to everybody else, so we have an RFC, a request for comment, in progress within Ribbon to evaluate the possibility and impacts of making this change. 505 01:14:41.070 --> 01:14:57.969 Lynne Jones: And I will just note that 70% of the first-year images in the simulation are acquired with the template tier. So, when we say, oh, you can just take some 20-second images, we actually mean the majority of the images in year one would be these shorter images. 506 01:15:01.780 --> 01:15:19.580 Lynne Jones: the impacts on our metrics. So, if you remember this grid from yesterday, we have the high-level, metrics across a bunch of different science areas. So, these are, at the bottom, are the, SRD metrics, and we have things that go into, 507 01:15:19.710 --> 01:15:23.099 Lynne Jones: Cosmology, and then time domain. 508 01:15:23.650 --> 01:15:33.149 Lynne Jones: static science of galaxies and solar system objects. And this is all normalized to, be 5.3. 509 01:15:33.400 --> 01:15:41.200 Lynne Jones: And at the… here we have what happens if we go to these 20-second templates, so the 20-second fast template simulation. 510 01:15:44.100 --> 01:15:54.200 Lynne Jones: some things get better, some things get worse. It's not obvious we've completely captured the effect in our metrics, but one thing that is for sure is that 511 01:15:54.300 --> 01:16:01.139 Lynne Jones: On the right here, what we have is the night that you have captured a given amount of area. 512 01:16:01.410 --> 01:16:12.390 Lynne Jones: while getting, at least 4 visits per band onto, silicon. So… This is math. 513 01:16:12.550 --> 01:16:17.439 Lynne Jones: Evaluating the camera footprint on our visit bore sites. 514 01:16:18.150 --> 01:16:25.020 Lynne Jones: Which is not quite the same as how, as I mentioned yesterday, as how data management would count 515 01:16:25.640 --> 01:16:33.730 Lynne Jones: whether the… detector was usable to go into the co-add, because they have, 516 01:16:34.280 --> 01:16:41.860 Lynne Jones: probably different constraints on the edges and things like that. So, this is our estimate, but it's not the final answer. 517 01:16:42.270 --> 01:17:00.899 Lynne Jones: So this is… if we have this deck-dependent seeing limit, and we chose… we said it's a limit of 1.2 arcseconds at zenith, and how many, how much area would you have where you got 4 visits onto silicon and… per band? 518 01:17:01.500 --> 01:17:15.570 Lynne Jones: And so what you see is this is the total area of the survey, and if… with, with the Comp Survey V5.3, that's the one where we used the old downtime, so we don't have our extra downtime. It's blue. 519 01:17:15.750 --> 01:17:25.209 Lynne Jones: The green line here that's lower is our baseline 5.3. So this is the effect of not having as many visits in year one. 520 01:17:26.270 --> 01:17:40.339 Lynne Jones: And then the red line is what happens if we, take those visits and make them shorter. So we… with a shorter visit, we do have a little bit less duty cycle on the sky, but we still end up with more visits, and so… 521 01:17:41.600 --> 01:17:53.240 Lynne Jones: If we were to do that, and all of the things, like the visit gaps remain the same, then we would push back up to, the same number of visits as we would have had without the extra downtime. 522 01:17:53.670 --> 01:17:58.249 Lynne Jones: And, so this is… this is close to you. This is… 523 01:17:58.360 --> 01:18:03.329 Lynne Jones: Essentially getting templates over the sky by the end of year one. 524 01:18:04.180 --> 01:18:15.360 Lynne Jones: Now, like I said, this is uncertain. You know, you can't say, oh, if we don't do this, we won't close the sky for the templates, and if we do, then we will, but that's… 525 01:18:15.450 --> 01:18:26.259 Lynne Jones: And if you said instead of 4 per year, you said 5… sorry, 4 per band, you said 5 per band, the difference between these would scale similarly, but, 526 01:18:26.600 --> 01:18:31.800 Lynne Jones: It's true that the overall Area would be slightly different. 527 01:18:34.110 --> 01:18:39.370 Lynne Jones: Right, so from the… that's our… from the point of view of metrics. Now, is this… 528 01:18:39.720 --> 01:18:46.590 Lynne Jones: So now I'm going to hand it over to Eric to talk about actual templates, and did you have slides of your own that you wanted to talk about? 529 01:18:46.590 --> 01:18:47.649 Eric C Bellm: Yeah, I can share. 530 01:18:47.650 --> 01:18:50.250 Lynne Jones: I put this one in because I wasn't quite sure. 531 01:18:50.440 --> 01:18:56.299 Eric C Bellm: Yeah, I'll… I'll put them into the shared slide deck after I talk. I just didn't have the link in time. 532 01:18:56.710 --> 01:18:58.149 Lynne Jones: Perfect, yeah, sorry about that. 533 01:18:58.490 --> 01:19:00.269 Lynne Jones: I'm gonna stop sharing a hand to you. 534 01:19:01.590 --> 01:19:06.260 Eric C Bellm: Alright, so I'm just gonna spend a few minutes talking about, 535 01:19:06.870 --> 01:19:15.730 Eric C Bellm: templates from the data management perspective. So I, I think it's worth, 536 01:19:16.050 --> 01:19:28.930 Eric C Bellm: saying up front, you know, kind of distinguishing in our minds two separate questions. One is thinking about what we're aiming for at the end of year one, as the… for the inputs into DR1. 537 01:19:28.930 --> 01:19:52.219 Eric C Bellm: which has been kind of targeted as our source of, you know, good all-Sky templates, and so that's, I think, especially driving some of the questions around the template tier that Lynn is describing. You know, how do we get to an endpoint where we have enough inputs of good quality over the whole footprint that we can co-add. Separately, you know, of course. 538 01:19:52.220 --> 01:20:06.089 Eric C Bellm: I, like all of you, am extremely excited to get alert science going, early in the survey, in this first year, and so for that, we need to be even more, sort of, aggressive in getting templates deployed. 539 01:20:06.180 --> 01:20:19.509 Eric C Bellm: how do we manage… how do we maximize that sort of science ahead of DR1? And so there, I think it's clear, as you're gonna see in a minute, you know, we have to… we have to accept some compromises of some kind, and it's just a question of 540 01:20:19.510 --> 01:20:29.959 Eric C Bellm: It's kind of an engineering and science trade-off of where do we cut the corners, because it's… we don't have as many images as we'd like, and we have to kind of figure out what to do about that. 541 01:20:30.340 --> 01:20:50.750 Eric C Bellm: All right, there are kind of two technical constraints that really, influence what we do on template generation. The one is for alert production. There's a database we call the APDB, the Alert Production Database, which serves as sort of the core of the association and light curve generation, sort of. 542 01:20:50.880 --> 01:21:15.719 Eric C Bellm: For alerts, and it's very sensitive to, false positive rate. If we… if we pump it full of junk sources, it will… it will break down. It will… it will reach capacity and not function. We have approached that on a few occasions and, learned from the process, but, you know, we have to be thoughtful about it. And I would say, probably as science users, you also don't want just 543 01:21:15.720 --> 01:21:40.669 Eric C Bellm: cascades of bad detections either. There's lots of knobs we're learning to tune here, you know, both in things like Real Bogus and how we configure image subtraction, but I just want to put out front that this is something that we really do care about a lot, and as you'll see in a minute, templates are a major source of false positives. So, the other challenge is that it is not as easy 544 01:21:40.670 --> 01:22:03.500 Eric C Bellm: as either it sounds, or we'd like it to be to change the templates frequently. The processing takes a while, frankly, and so it's not easy to do a big template run and just update things. I also think, scientifically, most users don't actually want that, because when you change the templates, all the… 545 01:22:03.850 --> 01:22:09.870 Eric C Bellm: All the different slight curves are gonna shift. You get different amounts of contamination from 546 01:22:09.870 --> 01:22:30.859 Eric C Bellm: transients in the… in the template for supernovae and things like that, and for variables. So, all of that just says that, like, you know, we will change templates over time, but we're not gonna thrash them, especially in the first year. So, we're trying to do the best job we can, you know, put templates on and keep them there for, you know, of order a year. 547 01:22:31.760 --> 01:22:55.759 Eric C Bellm: All right, so since we can't update the templates a lot, we want to try to minimize gaps where we can, because if you have a hole in the template, you can't fill it for a while, you get no alerts from there at all. The fill factor of the camera, in terms of, when you project it into the template space, it's about 88%, and so if you just use single images, then you're gonna just have 548 01:22:55.760 --> 01:22:57.940 Eric C Bellm: 12% holes. So… 549 01:22:58.280 --> 01:23:17.839 Eric C Bellm: So we want multiple inputs, and what is the very minimum? If you think of these as just uncorrelated and ask, you know, how many, how many, what area doesn't have any pixels on it, you only need sort of 2 or 3, and you get real close to 100% fill factor. So that's, like, kind of the minimum. 550 01:23:17.920 --> 01:23:30.060 Eric C Bellm: like, baseline to if you want to avoid holes. There are some other image quality and image subtraction issues, which we'll discuss there, but in terms of, like. 551 01:23:30.170 --> 01:23:39.209 Eric C Bellm: What's… what is the bare minimum for year one if… if we accept that we don't want to just leave giant holes in the survey, then… then there's a few images to input? 552 01:23:39.750 --> 01:23:44.200 Eric C Bellm: And again, those should be good quality images, they shouldn't have clouds in them, things like that. 553 01:23:45.000 --> 01:23:48.510 Eric C Bellm: As we add images, we do better. 554 01:23:48.550 --> 01:24:06.869 Eric C Bellm: with 3 or more images, we can do something, we can do artifact rejection. We have some algorithms that, especially work nicely when you get lots of images, where we… it's, able to reject, footprint… detection footprints that only show up in a configurable fraction of the inputs. 555 01:24:06.870 --> 01:24:10.690 Eric C Bellm: As you can see, on the right here, the difference between 556 01:24:10.690 --> 01:24:28.380 Eric C Bellm: sort of, you know, mean and sigma clip coads and this, what we call compare warp rejection, which is great for getting rid of things like satellite trails and glints and so on. So, this is, what we, you know, why we push for more inputs when we have them. 557 01:24:29.360 --> 01:24:42.029 Eric C Bellm: So again, we're trying to get to that sort of greater than 3 images, and that's where we sort of talked to Lynn about, can we get to 5, 6 sort of images to, to get inputs. 558 01:24:42.410 --> 01:24:59.630 Eric C Bellm: All right, what have we done so far? We have DP2 coming, later this year, and that is, based on commissioning images from last year, which got, especially this wide trance that you see here in the ecliptic plane and crossing through, sort of, the galactic center region. 559 01:24:59.870 --> 01:25:10.660 Eric C Bellm: We… this is the, a view of the HIPS maps from the Deepco ad. The template selections are very slightly different and a little smaller, but it's useful for illustration. 560 01:25:10.660 --> 01:25:34.220 Eric C Bellm: And when you zoom down at this level, it looks great, and you're like, okay, we got templates on all that area. It's not quite that simple. When you zoom in in the middle somewhere, you see that, yes, indeed, it is pretty well covered. But at the edges, you can see, that, you know, these are sort of single epochs that have big chip gaps in them. Don't pay too much attention to the interpolation here, but you can see the… 561 01:25:34.270 --> 01:25:36.379 Eric C Bellm: The chip structure of the camera. 562 01:25:36.830 --> 01:25:46.859 Eric C Bellm: This is U-band for comparison, and in U-band, for instance, there's even larger holes, even in the middle of this… of this footprint. 563 01:25:47.200 --> 01:26:03.899 Eric C Bellm: So as Lynn, showed, we have deployed these DP2 templates in addition to the existing drilling templates. There's a dashboard that's been circulated, and we're keeping updated as we add new ones. We added a few more, from, 564 01:26:03.900 --> 01:26:07.310 Eric C Bellm: From a few weeks ago, and are continuing to do so. 565 01:26:07.310 --> 01:26:11.380 Eric C Bellm: And so our alert volumes have accordingly increased. 566 01:26:11.490 --> 01:26:17.780 Eric C Bellm: What I do want to say, and this, again, impacts the… sorry, darn it. Let me… 567 01:26:18.140 --> 01:26:21.070 Eric C Bellm: Rapidly edit this. 568 01:26:21.170 --> 01:26:22.609 Eric C Bellm: Meant to make that a… 569 01:26:22.870 --> 01:26:42.160 Eric C Bellm: animation. We do see that even the DP2 templates have some challenges. So this is a pattern of alerts that we've sent out in the last few days, and you can see there's a pretty strong grid structure in some regions of this, of the sky. And this is, we have tracked down due to, 570 01:26:42.280 --> 01:26:54.660 Eric C Bellm: when we have co-added even, you know, a relatively small number of images in this wide area, there's a wide enough range of PSF sizes that when you have chip gaps. 571 01:26:54.800 --> 01:27:07.820 Eric C Bellm: Sometimes the PSF that results in the COAD is printing through has some pretty strong spatial variations, which you can see on the right for a patch here. I apologize, the full width half max here is in pixel units. 572 01:27:07.820 --> 01:27:26.319 Eric C Bellm: Which is, you know, multiplied by 0.2, but you can kind of see how these structures, you know, have the imprint of the focal plane in full width, half max space. And so image differencing has a fair bit of trouble right now. It's sort of managing, you can't… 573 01:27:26.320 --> 01:27:31.030 Eric C Bellm: The kernel is not able to handle such rapid changes, and so you get 574 01:27:31.030 --> 01:27:42.500 Eric C Bellm: an excess of false positives. We have a number of ideas about how to deal with this, both at the vetting side and in template construction, image differencing, and so on. 575 01:27:42.500 --> 01:27:56.850 Eric C Bellm: But I guess I would just, you know, highlight the point that, you know, it's not quite as simple as, you know, just take, take in image, you know, take two images and add them and everything will be fine. It really does… we do see problems. 576 01:27:56.850 --> 01:28:07.429 Eric C Bellm: I mean, the good news is these are not such large, bogus volumes that it's overwhelming the APDB, but it is something where we feel like we need to take some corrective action. 577 01:28:08.180 --> 01:28:12.430 Eric C Bellm: All right, so we're looking ahead to incremental templates with, 578 01:28:12.480 --> 01:28:26.180 Eric C Bellm: with pre-LSST images, as well as the previous input inputs. Lynn hasn't seen these, because I just got them done this morning. So these are plots of basically all of the Rubin science images subject to some cuts. 579 01:28:26.200 --> 01:28:45.109 Eric C Bellm: And… and sort of looking where we… where we could start building incremental templates now, and so this is band by band. I'll call your attention mainly to the green boxes, which are tracks that have complete coverage of at least 3 input images, and so that would be kind of a good place to start. 580 01:28:45.430 --> 01:28:54.949 Eric C Bellm: So this is U-band, there's some, you know, maybe, I guess it's labeled here. 42 tracks are maybe plausible. 581 01:28:54.950 --> 01:29:14.720 Eric C Bellm: G, a little wider. The white areas already have templates deployed, either from the DDFs or from DP2. R-band, a little bit of coverage, sort of, in the south. It remains patchy. This… there's a region, here that maybe we could explore. 582 01:29:14.720 --> 01:29:23.750 Eric C Bellm: Iban, there's these big stripes that were taken during OES commissioning, which we can build templates in, so those are a natural place for us to start. 583 01:29:23.880 --> 01:29:30.220 Eric C Bellm: Zband, I think, is in some ways the best. There are some really large areas here that have quite a bit of coverage. 584 01:29:30.310 --> 01:29:47.160 Eric C Bellm: And then Y band a little less. So, I think we do have a bit of a head start building templates over a reasonable but not overwhelming area, but we need to sort of understand, some of the issues we're seeing with the DP2 templates. 585 01:29:47.160 --> 01:29:56.710 Eric C Bellm: In order to make sure that we're making the right choices there as we deploy them. So, happy to… I don't know if we're going to questions here, Lynn, but that's all I have for the moment. 586 01:29:59.770 --> 01:30:11.090 Lynne Jones: Yep, it was, just questions, and then we… we back up to the break next. So, actually, that was awesome, Eric, thank you so much. And all of that new stuff, very fascinating. 587 01:30:11.090 --> 01:30:25.110 Lynne Jones: I wanted to make the comment that when we know that we can build a template in a particular area of the sky, we will be able to load that into the template tier survey, so that they know that, like, okay, yeah, we… 588 01:30:25.290 --> 01:30:37.260 Lynne Jones: You may not know about those observations, because we're going to wipe its memory clean when we start the survey, but we can tell that, yes, there are already templates available for this part of the SCA. 589 01:30:38.240 --> 01:30:40.320 Lynne Jones: Alright, David. 590 01:30:41.100 --> 01:30:46.880 David Schlegel: Yeah, these DP2 template observations, are that all the range of rotation angles? 591 01:30:47.620 --> 01:30:58.659 Eric C Bellm: Yeah, that's right. It's getting the… maybe Lynn can speak better to it, but my understanding is those are widefast, deep-style dithers in rotation and translation. 592 01:30:59.340 --> 01:31:12.869 Lynne Jones: Yeah, the… so the… the stripe across the sky in the ecliptic area was mostly wide-fast-y, style. It was mostly coming from, our Paris survey. 593 01:31:12.970 --> 01:31:19.879 Lynne Jones: tier, but… The… because of the fact that, it's a smaller area on the sky. 594 01:31:19.990 --> 01:31:24.889 Lynne Jones: We… the repeat rate was a little bit higher, and 595 01:31:26.010 --> 01:31:32.259 Lynne Jones: Yeah, but other than that, it would be like our normal survey observations. 596 01:31:45.540 --> 01:31:46.870 Lynne Jones: Alright, wow. 597 01:31:47.170 --> 01:31:50.849 Lynne Jones: I really thought everybody would have questions for you, Eric, because of the… 598 01:31:51.130 --> 01:32:04.350 Lynne Jones: I'm really fascinated to see the, you know, where we can go with incremental templates, and what we might be able to do even before we start the survey, because these are really 599 01:32:04.570 --> 01:32:10.999 Lynne Jones: big questions, like, what are we going to try to do in the first year regarding templates? 600 01:32:17.530 --> 01:32:22.289 Lynne Jones: I… nobody has asked, but I'm gonna ask, because… 601 01:32:22.620 --> 01:32:27.700 Lynne Jones: I get asked, how soon can you have templates for a particular area of the sky? 602 01:32:27.930 --> 01:32:37.789 Lynne Jones: And I know from watching that there's a… can be a significant lag, because as you said, it's quite labor-intensive. 603 01:32:38.730 --> 01:32:45.580 Lynne Jones: Do you… do you want to say a few words on, like, the rate of, like, once we cover the sky, or, like… 604 01:32:46.000 --> 01:33:00.890 Eric C Bellm: Yeah, I had this in a slide and kind of brushed past it. My estimate right now is that the delta between, we know we have enough images here, and we could get this into production, is about a month. 605 01:33:01.090 --> 01:33:15.690 Eric C Bellm: And a lot of that is human steps, you know, either shepherding data through, or looking… vetting the data before we deploy it, or getting it deployed. I hope that can come down over time as we streamline 606 01:33:15.690 --> 01:33:22.509 Eric C Bellm: You know, our metrics and learn to trust, you know, what we're looking at. 607 01:33:22.550 --> 01:33:28.450 Eric C Bellm: you know, again, we sort of started with the DDFs, which have a very different sort of… 608 01:33:28.680 --> 01:33:46.470 Eric C Bellm: behavior when you co-add them, versus some of these wider areas. So, you know, that's… that's my estimate right now, is it takes a month, and I hope that it improves over time. It kind of needs to, but, I don't… I don't think that's… that's happening quickly, so… 609 01:33:50.560 --> 01:33:51.440 Lynne Jones: John? 610 01:33:52.950 --> 01:34:00.260 John Gizis: So I guess I… I guess I don't quite follow the big picture case for, sort of, taking a major part of the first 611 01:34:00.540 --> 01:34:06.829 John Gizis: year and turning it into a 20-second survey, right? I mean, if there's one-month delays anyway on templates. 612 01:34:07.240 --> 01:34:10.460 John Gizis: The alert, you know, volume is so large. 613 01:34:10.590 --> 01:34:22.890 John Gizis: you know, in the long run, of course, you can… you will have templates and can go backwards in time, so it's just about alert production. Doesn't it seem like there'll be enough alerts that maybe you should just stick with the 30-second? Like, what's the big picture? Like. 614 01:34:23.890 --> 01:34:27.809 John Gizis: Like, you really won't be able to generate alerts even after one year. 615 01:34:28.220 --> 01:34:29.080 Lynne Jones: So… 616 01:34:29.080 --> 01:34:33.289 John Gizis: Over the whole sky? In every filter? Is that the problem? Like… 617 01:34:33.290 --> 01:34:34.450 Lynne Jones: Oh. 618 01:34:34.450 --> 01:34:36.919 John Gizis: Understand what drives such a big change. 619 01:34:37.470 --> 01:34:39.789 Lynne Jones: Yeah, I don't… I don't… okay, so Eric, I saw Eric… 620 01:34:40.300 --> 01:34:45.819 Lynne Jones: You put up your hand, so I'm gonna say maybe you… if you have something to say about this, go ahead. 621 01:34:45.820 --> 01:34:55.250 Eric C Bellm: Okay, sure, we can take two turns. I think the advantage to 20-second exposures is that it gives you more images 622 01:34:55.730 --> 01:35:03.990 Eric C Bellm: you know, more… a larger number of images at any given position and filter in the sky at the end of year one. And… 623 01:35:03.990 --> 01:35:17.529 Eric C Bellm: If those are… especially if those are preferentially taken in better conditions, that increases the odds that you have a good set of inputs that you can, reject artifacts, you know. 624 01:35:17.570 --> 01:35:31.159 Eric C Bellm: you know, dither out chip caps, etc. So, you're sort of sacrificing a little bit of depth in exchange for kind of an absolute image quality improvement. It's less about, in my mind, it's less about 625 01:35:31.200 --> 01:35:41.139 Eric C Bellm: Getting alerts out in year one, and more about, do you have enough, you know, what is the quality and aerial coverage of templates at the end of, at the end of year one? 626 01:35:41.140 --> 01:35:59.050 Eric C Bellm: I will say, you know, Lynn didn't say, but, you know, we have been discussing in data management, like, can we support 20-second images? Are there concerns we need to worry about? Largely, the answer is no, with one exception. There is some concern that the active optics system 627 01:35:59.050 --> 01:36:22.450 Eric C Bellm: instead of being able to correct, sort of, every, you know, 2 images later would be then at 3 images later correction because of the shorter, sort of, cycle time. And that is a significant concern that they worry that the image quality will suffer, and that may be, you know, maybe a showstopper. And there's some discussion, I don't know if Bob or others want to comment, you know, we should just test this. 628 01:36:22.560 --> 01:36:31.350 Eric C Bellm: But I think that's maybe the biggest concern that I'm aware of with the 20-second exposures outside of the survey strategy question. 629 01:36:31.670 --> 01:36:41.530 John Gizis: And could I ask a related question? My metric actually seemed to survive, because the, you know, the extra images probably makes up for anything you lose, so it's, it's, you know, it's all fine. 630 01:36:41.610 --> 01:36:56.269 John Gizis: But I heard a lot, I think, in previous workshops of the need for really high-quality, G-band and R-band images, that it was important to get, you know, sort of deep, good-seeing images there. 631 01:36:56.360 --> 01:36:58.139 John Gizis: And it sort of seems like that might… 632 01:36:58.680 --> 01:37:09.480 John Gizis: be a real problem to what I heard, you know, repeatedly in a lot of documents, that that was sort of really a priority for the 10-year static case. Maybe it's all in the wash, since it's only 1 tenth. 633 01:37:09.800 --> 01:37:14.239 John Gizis: But, has that… is there any comments about that? 634 01:37:15.110 --> 01:37:31.670 Lynne Jones: This is… this is a good point, because I think that this is one of the things that's not necessarily well captured in the metrics that we have, like, how… and… and what it goes into is, how well can you de-blend things like stars and galaxies, is my understanding. 635 01:37:32.060 --> 01:37:35.360 Lynne Jones: Yeah, so… 636 01:37:36.340 --> 01:37:44.120 Lynne Jones: That might be an issue. I think it certainly is one of the things we would have to go and consider. 637 01:37:44.320 --> 01:38:00.989 Lynne Jones: It also, after 10 years, it does kind of probably come out in the wash, but the question is, do you need that at the end of year one? Which I think was actually their request, that you have those at the end of year one. That said, they also didn't have a large number of these 638 01:38:01.390 --> 01:38:09.129 Lynne Jones: you can sort of think of them as Pathfinder, like, they're the, like, that's pin to blending based on these, like, really deep, good-seeing images. 639 01:38:09.320 --> 01:38:10.430 Lynne Jones: And… 640 01:38:11.210 --> 01:38:25.630 Lynne Jones: it's not obvious you wouldn't have that anyway, even with the slightly shallower depths, because they are in good conditions, so that you naturally get a slightly deeper depth. So I think that's something to also look at, for sure. 641 01:38:25.690 --> 01:38:32.020 Lynne Jones: It's also true that it may be a showstopper based on the AOS, 642 01:38:32.110 --> 01:38:34.500 Lynne Jones: So, we'll see. There's, there's… there's… 643 01:38:35.510 --> 01:38:40.210 Lynne Jones: This is still very much in the, we're going to… 644 01:38:40.450 --> 01:38:43.899 Lynne Jones: Have to think about this a little bit more, maybe test some data on the sky. 645 01:38:44.160 --> 01:38:48.030 Lynne Jones: The other… there wasn't another… 646 01:38:50.250 --> 01:38:58.879 Lynne Jones: there's maybe some concern about U-band, and maybe we would have to leave U-band at 38 seconds, just because, 647 01:38:59.570 --> 01:39:11.410 Lynne Jones: getting even further… getting back into the read noise, which is what would start to happen with the 25-second exposure, might be bad. Alright, here's… this is the other thing I was gonna say, though. 648 01:39:12.190 --> 01:39:23.780 Lynne Jones: it may not be that we have… then… if I didn't say, oh, it's so that we can get templates over the whole sky and we can close the sky, but if instead I said, and this might hold up DR1, 649 01:39:24.120 --> 01:39:26.160 Lynne Jones: Does that change your opinion? 650 01:39:28.020 --> 01:39:39.710 Lynne Jones: Because that… not having… not being able to make templates over the whole sky might actually mean, like, oh, we're gonna wait a little bit longer until we get those images so we can make them as part of DR1. 651 01:39:40.810 --> 01:39:48.160 Lynne Jones: That is not my decision to make, obviously, and it's… it's not a for-sure thing, but, like, that would be a possibility. 652 01:39:48.470 --> 01:39:52.860 Lynne Jones: So… Damn. 653 01:39:55.340 --> 01:40:04.510 Dan Taranu: Yeah, so you showed this plot that had the number of… or the area covered versus the number of nights, or the various scenarios, and it kind of looked like 654 01:40:05.380 --> 01:40:11.429 Dan Taranu: The slope from the baseline after you reach around 15,000 square degrees was just about the same. 655 01:40:11.870 --> 01:40:21.119 Dan Taranu: I was wondering, are those the same 15,000 square degrees? Are you envisioning a scenario where you do 20 seconds for, like, 200 days and then switch over, or… 656 01:40:21.710 --> 01:40:24.040 Lynne Jones: This one… this one here, you mean? 657 01:40:24.310 --> 01:40:25.040 Dan Taranu: Yeah. 658 01:40:27.820 --> 01:40:44.339 Lynne Jones: Yes, sorry, after… so this would only be 20-second visits coming from the template tier. Any other tier would just do normal 30-second visits. However, like I said, in the first year, and the template tier switches off after the first year, right? So in the first year, 659 01:40:44.740 --> 01:40:50.420 Lynne Jones: On the order of 70% of the visits would be the shorter visits coming from the template tier. 660 01:40:53.910 --> 01:40:57.210 Lynne Jones: So yeah, after this point, it looks… 661 01:40:57.620 --> 01:41:04.880 Lynne Jones: It will become fairly similar, but that's also… the template here isn't trying to acquire any visits after that point. 662 01:41:06.160 --> 01:41:08.700 Dan Taranu: Right. Well, what I meant was after about 663 01:41:08.840 --> 01:41:14.680 Dan Taranu: Knight 300, the slope of the green line looks basically the same as red, right? 664 01:41:16.310 --> 01:41:20.779 Dan Taranu: So, if you were to switch over from 20 seconds to 30 seconds after, like. 665 01:41:20.960 --> 01:41:23.009 Dan Taranu: I don't know, 250 nights? 666 01:41:25.010 --> 01:41:25.830 Lynne Jones: I'm… 667 01:41:27.690 --> 01:41:35.690 Lynne Jones: So, okay, Peter can say something more about this if he wants, because he made this plot, but I'm gonna guess that that's… 668 01:41:36.030 --> 01:41:38.989 Lynne Jones: Not just because of, 669 01:41:40.190 --> 01:41:49.729 Lynne Jones: A lot of that has to do with how much area is new and appearing on the sky, maybe rather than quite so much as, 670 01:41:50.770 --> 01:41:58.429 Lynne Jones: the rate of acquiring just enough. I'm not sure, yeah. Peter, do you have anything to say about that? 671 01:41:58.430 --> 01:42:08.540 Peter Yoachim: I bet that rapid rise is that we observed some area at the start of the survey, but didn't get enough to get templates, and so it's come back around, and so now we're able to rapidly, you know. 672 01:42:08.750 --> 01:42:13.240 Peter Yoachim: One image gets us to the threshold, and so that's why there's that rapid rise. 673 01:42:13.630 --> 01:42:14.010 Lynne Jones: Yeah. 674 01:42:14.010 --> 01:42:18.419 Peter Yoachim: Yeah, it's… it's area that's coming back around that… that now we can complete. 675 01:42:21.370 --> 01:42:31.539 Lynne Jones: Yeah, that makes sense. So, it's… it's because we did… we did part of the sky that we're observing here, we did it back here, but we didn't reach 4. 676 01:42:32.460 --> 01:42:33.010 Peter Yoachim: Yeah. 677 01:42:36.150 --> 01:42:36.900 Lynne Jones: Okay. 678 01:42:41.330 --> 01:42:48.230 Lynne Jones: I'll pause for a minute if there's any more questions. We are into our break, so… But also I think that… 679 01:42:49.090 --> 01:42:57.080 Lynne Jones: these are all really good questions, and I really appreciate hearing about the templates and the current plans. So thank you, Eric. 680 01:43:03.260 --> 01:43:03.920 Lynne Jones: Alright. 681 01:43:04.800 --> 01:43:14.999 Lynne Jones: I don't see any more questions. Remember, you can ask questions on Slack, or on Community if you have a more general question. That's great, a great place as well. 682 01:43:15.560 --> 01:43:16.400 Lynne Jones: Alright. 683 01:43:17.450 --> 01:43:25.289 Lynne Jones: Actually, this is the time for our break, so we'll come back at, in 20 minutes at 10 o'clock. 684 02:03:01.450 --> 02:03:02.480 Lynne Jones: All right. 685 02:03:02.830 --> 02:03:05.600 Lynne Jones: Here we are, 10 o'clock, 686 02:03:06.960 --> 02:03:12.029 Lynne Jones: Hopefully everybody comes back from the break now. Okay, so… 687 02:03:12.260 --> 02:03:24.060 Lynne Jones: Next, we have, two more specific areas to cover, rolling cadence and options around rolling cadence, and Leanne Guy's gonna talk a little bit, with us about 688 02:03:24.490 --> 02:03:30.029 Lynne Jones: uniformity in coads and data management processing for DRP. 689 02:03:30.590 --> 02:03:38.039 Lynne Jones: As well, to go with that. And then we're going to talk about the DESE survey options. And then we have some time for general discussion. 690 02:03:38.190 --> 02:03:39.620 Lynne Jones: As, as we need it. 691 02:03:40.390 --> 02:03:41.340 Lynne Jones: Okay. 692 02:03:43.010 --> 02:03:44.040 Lynne Jones: So… 693 02:03:44.830 --> 02:04:00.340 Lynne Jones: rolling cadence. So, if you remember, this is what we do so that we can boost the cadence, for time domain in certain areas of the sky, at the expense of in other seasons that has slightly lower cadence. So. 694 02:04:00.730 --> 02:04:12.719 Lynne Jones: When a part of the sky is in active rolling cadence, the… the gap between, nights of visits is… is sort of 2. 695 02:04:12.910 --> 02:04:24.829 Lynne Jones: On average. And in a low cadence season, the gap between coming back to the same, part of the sky, the same pointing on the sky, is about 7 nights. 696 02:04:25.200 --> 02:04:27.270 Lynne Jones: So it does vary, and then… 697 02:04:27.430 --> 02:04:37.909 Lynne Jones: In between, in our seasons, which are just, like, normal, uniform cadence, like in the first year, the gap between revisits is actually, 698 02:04:38.380 --> 02:04:45.310 Lynne Jones: Medium value of 3, you know, obviously there's a little bit more scatter in there, so… 699 02:04:45.560 --> 02:04:55.819 Lynne Jones: So, if you look at the whole survey, and don't look at individual seasons of rolling, you mostly… and you're just measuring something like the 700 02:04:55.940 --> 02:05:08.009 Lynne Jones: the gap between visits. You mostly see the uniform seasons, and it sort of washes out that increase from rolling and the decrease from the, low activity rolling errors. But. 701 02:05:08.330 --> 02:05:13.650 Lynne Jones: If you are looking at something like how much… how well you're recovering particular light curves. 702 02:05:13.760 --> 02:05:21.620 Lynne Jones: That will be influenced by the details of the observations in a particular season or year, and so you'll notice that a little bit more. 703 02:05:21.740 --> 02:05:26.830 Lynne Jones: So that's one of the things that, depending on how you're… 704 02:05:27.230 --> 02:05:33.380 Lynne Jones: Looking at what you're looking at when you're trying to evaluate impacts of 705 02:05:34.170 --> 02:05:38.120 Lynne Jones: just the visit spacing on time domain. 706 02:05:38.310 --> 02:05:42.839 Lynne Jones: metrics. You do have to consider whether you're 707 02:05:43.180 --> 02:05:50.730 Lynne Jones: Sensitive to the changes in a given year of rolling, or if you're sort of washing out over the whole survey. 708 02:05:51.850 --> 02:05:53.799 Lynne Jones: So, that said… 709 02:05:54.070 --> 02:05:59.180 Lynne Jones: That makes some of the metrics a little tough to interpret when you're looking at 10-year metrics. 710 02:05:59.900 --> 02:06:00.690 Lynne Jones: And rip. 711 02:06:01.610 --> 02:06:15.940 Lynne Jones: what we have is, in baseline V5.3, we start rolling after year one. This is the standard. We don't want to roll inside of year one, because we want fairly uniform coverage at the end of year one, so that we can do 712 02:06:15.970 --> 02:06:23.400 Lynne Jones: Calibration and photometric and astrometric catalogs over the whole sky with something that's, 713 02:06:23.800 --> 02:06:26.530 Lynne Jones: That has the number of visits and is fairly uniform. 714 02:06:26.950 --> 02:06:29.759 Lynne Jones: Now, if we're still acquiring visits. 715 02:06:30.090 --> 02:06:49.720 Lynne Jones: needed for the input templates, instead of starting rolling right after year 2, or right at the start of year two, at the end of year one, we could delay the start of rolling until after year two, because there is, a reasonable argument to be made that you should not start rolling when you don't have templates yet. 716 02:06:49.730 --> 02:06:58.649 Lynne Jones: Because, the templates are needed to fully leverage the time domain, and the time domain is the reason for going into the rolling cadence. 717 02:07:00.120 --> 02:07:04.690 Lynne Jones: Now, it is also too early yet to know if this is a problem. 718 02:07:04.970 --> 02:07:22.660 Lynne Jones: And the decision can wait while we're investigating options on whether we should start rolling at the end of year one, or whether we should start rolling at the end of year two. So, some of the things we're talking about here in the various simulations that we have are questions of 719 02:07:23.460 --> 02:07:28.419 Lynne Jones: things to think about, we don't… we won't be making the decision today. 720 02:07:28.720 --> 02:07:31.220 Lynne Jones: Or… or immediately, anyway. 721 02:07:32.760 --> 02:07:46.780 Lynne Jones: This series of plots over here on the right is the number of visits in IBAND, so I chose just a single band, after year one. So, year one is a time… 722 02:07:47.030 --> 02:07:54.279 Lynne Jones: deadline, not a season. So remember, this is just the… the end of year one. We would have this many visits in IBAN. 723 02:07:54.710 --> 02:08:01.329 Lynne Jones: At the end of year two, our coverage would look like this, because we've started rolling during year two. 724 02:08:02.210 --> 02:08:11.439 Lynne Jones: At the end of year three, it looks like this, because we've started rolling, but also we've started the opposite rolling, but you still see all of this signature rolling. 725 02:08:11.550 --> 02:08:21.949 Lynne Jones: And then we have a season for the rolling cadence, where instead of doing a high activity or low activity, it has an average, so the medium. 726 02:08:22.180 --> 02:08:31.730 Lynne Jones: Or normal uniform activity. And so that lets the sky catch up and, equalize, and so at the end of year four. 727 02:08:31.840 --> 02:08:40.570 Lynne Jones: we have what looks like a fairly uniform coverage on the sky. Now, I did make these plots, removing any of the special surveys. 728 02:08:41.120 --> 02:08:46.420 Lynne Jones: Because that… then this lets us see exactly how uniform, 729 02:08:46.780 --> 02:08:53.139 Lynne Jones: Things like the… the pair survey, and our normal wide, fast, deep kind of observations would look. 730 02:08:54.120 --> 02:09:12.439 Lynne Jones: If we delay the start of rolling until after year two, what this basically means is we're shuffling the high and low activity and uniform seasons so that the end of year two is uniform, so instead of being here at the end of year four, year 2 would be uniform. 731 02:09:12.680 --> 02:09:18.539 Lynne Jones: And then 3 and 4 would be non-uniform, because we've just shuffled that order. 732 02:09:19.920 --> 02:09:20.780 Lynne Jones: Okay. 733 02:09:22.060 --> 02:09:24.320 Lynne Jones: So, we have some simulations. 734 02:09:24.500 --> 02:09:27.840 Lynne Jones: That illustrate 735 02:09:28.450 --> 02:09:36.280 Lynne Jones: different options. So if we go with the baseline, normally at the end of year four, we have a uniform data release. 736 02:09:36.520 --> 02:09:42.449 Lynne Jones: And I'm gonna keep saying uniform with quotes because, this is part of the things that 737 02:09:42.570 --> 02:09:44.589 Lynne Jones: that Leon is going to talk about. 738 02:09:45.070 --> 02:09:49.410 Lynne Jones: Well, we'll talk about a little bit more in a minute. 739 02:09:50.100 --> 02:10:03.499 Lynne Jones: So at the end of year four, normally we would have a uniform data release, but if we reshuffle and delay the start of rolling, that year 4 uniform data release disappears, and it moves into year 2. So these are… 740 02:10:03.520 --> 02:10:22.969 Lynne Jones: Two other options. This is if we just delay the start of rolling, or we don't change anything else. So you can see year four, so across in this plot is all year four, for different simulations. Down in these series of images is different years, so it's 4, 5, and 7, not 6. I skipped a year, but… 741 02:10:23.370 --> 02:10:24.470 Lynne Jones: There. 742 02:10:24.760 --> 02:10:35.669 Lynne Jones: So this is… on the left is the baseline, year 4, 5, and 7. And the second row is just a simple… we'll delay the start of rolling for one year. 743 02:10:35.960 --> 02:10:46.420 Lynne Jones: So this is what we… the simulation we're calling Roll Mash, 5.3. So it goes… this is, again, your 4, 5, and 7, and you can see your 7… 744 02:10:46.570 --> 02:10:55.279 Lynne Jones: Because we only shuffled some of these rolling seasons early in the survey, year 7 looks very similar. So you have year 7 in the baseline, year 7 in Roll Mash. 745 02:10:55.450 --> 02:10:58.370 Lynne Jones: That's our uniform data release year. 746 02:10:59.450 --> 02:11:06.660 Lynne Jones: And then, if we not only reshuffle the, seasons of uniform rolling, 747 02:11:06.830 --> 02:11:17.310 Lynne Jones: in the first year… sorry, in year 2 and 3 and 4, if we also shuffle them in later years, we can move that uniform data release that was in year 7 748 02:11:17.640 --> 02:11:22.939 Lynne Jones: into your 5. And so this is roll U5, V5.3. 749 02:11:24.060 --> 02:11:29.629 Lynne Jones: So this one… in this U5 simulation, we also delayed the start of rolling for a year. 750 02:11:30.210 --> 02:11:42.150 Lynne Jones: But instead of taking the uniform season, right before the year 7 data release, we've moved it up in time, and so we have a uniform data release at year 5 instead. 751 02:11:42.450 --> 02:11:53.210 Lynne Jones: So in both of these simulations, because we wait, we have a uniform data release in year 1, year 2, and then this would be year 7, and year 10, and this would be year 5, and year 10. 752 02:11:54.760 --> 02:11:59.089 Lynne Jones: So, if we delay… This started rolling. 753 02:11:59.350 --> 02:12:08.189 Lynne Jones: We inevitably lose uniform data release at year 4, but then we can have a choice about if it's year 7 or year 5. 754 02:12:11.060 --> 02:12:15.999 Lynne Jones: And of course, year 10 in all of these simulations is the same. 755 02:12:18.550 --> 02:12:24.199 Lynne Jones: So… Because at the end of 10 years, you've done the same… 756 02:12:24.330 --> 02:12:35.239 Lynne Jones: number of visits, and the simulation is generally the same. Just reshuffling the seasons when you're doing rolling cadence and when you're not should be… 757 02:12:35.700 --> 02:12:38.989 Lynne Jones: really have a minimal impact on those Year 10 metrics. 758 02:12:39.220 --> 02:12:50.870 Lynne Jones: And so this is our metric grid again. It's, here's V5.1, the baseline, and so this is what everything is normalized to, and these are these high-level summary metrics. 759 02:12:51.640 --> 02:12:54.990 Lynne Jones: Now… Role… 760 02:12:55.170 --> 02:13:06.689 Lynne Jones: Year 2, U7 is, like, we have… wait until year 2, this is the roll mash, sorry, it's renamed. This is one reason why, in general, we discourage people from renaming, but I did it anyway. 761 02:13:08.580 --> 02:13:15.429 Lynne Jones: And this is the one where it was… the uniform data release was shuffled into year 5 instead of year 7. 762 02:13:15.880 --> 02:13:18.530 Lynne Jones: And you can see it's not exactly the same. 763 02:13:19.100 --> 02:13:23.760 Lynne Jones: The changes are pretty minimal, so this… note the scaling here, this is, 764 02:13:24.930 --> 02:13:30.829 Lynne Jones: 10% into the… into the red, or 10% into the… into the blue. 765 02:13:31.040 --> 02:13:39.009 Lynne Jones: And these are all generally a few percent, except for some. There's… there are some of these time domain metrics which seem a little bit more sensitive. 766 02:13:39.040 --> 02:13:56.500 Lynne Jones: And it may be that what we're actually seeing here is noise, rather than actually something, real in the changes of the metrics, because really, these impacts should be minimal, but it is possible that as we change things around. 767 02:13:56.790 --> 02:13:59.630 Lynne Jones: There's some unintended effects. 768 02:14:00.090 --> 02:14:06.229 Lynne Jones: So it's worth looking at, but it is also possible that… Not that significant. 769 02:14:08.090 --> 02:14:20.369 Lynne Jones: So this is the thing we should think about, like, what do we do about, if we did delay the start of rolling, which we don't know we would do yet, but it is a possibility, especially if we can't. 770 02:14:20.520 --> 02:14:24.710 Lynne Jones: Complete templates around the sky at the end of year one. 771 02:14:25.010 --> 02:14:31.500 Lynne Jones: Then what do we do about later years, and down the road, do we shift some of these uniform data releases around? 772 02:14:35.030 --> 02:14:46.150 Lynne Jones: Now, I also wanted to talk a little bit about uniformity and what that means, because we talk a lot about, hey, let's have a uniform data release. 773 02:14:46.640 --> 02:14:51.779 Lynne Jones: But, that's not really very well defined. 774 02:14:52.490 --> 02:14:58.619 Lynne Jones: And… It's not obvious, what's the best way to support that? 775 02:14:58.770 --> 02:15:04.890 Lynne Jones: There's some uniformity we can enforce, we can try to gain from survey strategy. 776 02:15:05.210 --> 02:15:13.859 Lynne Jones: By not letting our… our number of epochs or depths get too uneven across the sky. 777 02:15:13.980 --> 02:15:22.019 Lynne Jones: And an example of trying to manage that uniformity is with this uniform season in the rolling cadence. 778 02:15:23.470 --> 02:15:42.339 Lynne Jones: There's also an aspect, like, you could enforce uniformity later in the processing chain at data management, although if we do that there, it necessarily means dropping visits to gain uniformity, so you're not dropping visits completely, but not including them in the coads. 779 02:15:43.030 --> 02:15:49.270 Lynne Jones: So… This raises questions, how could or should we achieve 780 02:15:49.400 --> 02:15:54.490 Lynne Jones: uniformity in the coads and the catalogs that come from the coads. 781 02:15:54.570 --> 02:16:14.260 Lynne Jones: What does that mean? There is some natural variation due to weather, that will lead to variations in the coated depth across the low dust, wide, fast, deep region, but is it that we want less than the magnitude of variation in the estimated coated depth, the number of epochs? 782 02:16:14.360 --> 02:16:20.140 Lynne Jones: Is it a different number on the… on the RMS of the coated depth? 783 02:16:20.580 --> 02:16:25.720 Lynne Jones: And what does it mean for visits which are not included in the co-ads? 784 02:16:25.970 --> 02:16:44.380 Lynne Jones: So these are all good questions, that I had, and then the plots here show us the co-ed depth and I-band, if you do include all of the special surveys, versus if you don't. So even if we don't have a question about, like, what do we do with rolling cadence, what do we do with DESI, 785 02:16:44.629 --> 02:16:52.719 Lynne Jones: anything, we already have non-uniformity due to things like the TOs, and other special surveys. 786 02:16:53.790 --> 02:16:57.799 Lynne Jones: So… Leanne, are you there? 787 02:16:59.260 --> 02:17:00.490 Leanne Guy (Rubin): I am here. 788 02:17:00.620 --> 02:17:12.929 Lynne Jones: Excellent, excellent. I was going to hand this over to you to talk a little bit about, some of the things we chatted about the other day, like, what happens to visits that don't get included in co-ads and things like that? 789 02:17:13.850 --> 02:17:30.650 Leanne Guy (Rubin): Yeah, okay, thanks, Lynn, thanks for introducing us. So, I've sort of just come along at the last minute at Lynn's request to support this meeting. I have nothing prepared, I have no answers for you, but I am here to take a lot of questions and to think about how we can address some of the open topics and questions. 790 02:17:30.969 --> 02:17:46.130 Leanne Guy (Rubin): What happens to visits that are not included in COADs? They will still be perfectly valid single visit images, and there will be catalogues of detections in those single visit images, and they will be included in a data release. They just won't have gone into a COAD. 791 02:17:46.580 --> 02:17:58.249 Leanne Guy (Rubin): You'll already see this, in fact, with Data Preview 2, which is coming up sometime in the July to September timeframe. We have a region of DP2 which has co-ads. 792 02:17:58.250 --> 02:18:12.709 Leanne Guy (Rubin): And then we have a lot of other visits scattered across a very large area of the sky. So the co-added region is roughly 3,000 square degrees, although there's variation of co-added depth within that 3,000 square degrees. And then you can get out to another sort of, I think it's about 12,000 or so 793 02:18:12.830 --> 02:18:23.079 Leanne Guy (Rubin): degrees, with just single visit images taken at various positions on the sky. So, some of the positions on the sky will only actually have one visit, maybe some will have two, but none of these were co-added. 794 02:18:23.709 --> 02:18:28.149 Leanne Guy (Rubin): So, you'll already see how that looks in the Data Preview 2 release. 795 02:18:29.730 --> 02:18:38.829 Leanne Guy (Rubin): So the term throw out is a bit strong, maybe. We will throw them out of the co-add, but we will not throw them out of the release, provided they meet other quality criteria. 796 02:18:44.620 --> 02:18:48.419 Lynne Jones: Sorry for my thrashing there as I tried to unmute myself. 797 02:18:49.190 --> 02:18:59.980 Lynne Jones: Yeah, and those… the catalogs from the single visit images are calibrated in the same way, like, against, the full astrometric and photometric calibration, etc. 798 02:18:59.980 --> 02:19:19.579 Leanne Guy (Rubin): In a data release, yes. Like, single visit images in the prompt, nightly processing, no, have a, I think, more fast approximate calibration, but in data release, yes, they are fully calibrated, single-visit images. It's… they're processed in exactly the same way as every other single visit image, irrespective of whether it goes into a co-add or not. 799 02:19:20.690 --> 02:19:32.559 Lynne Jones: So if we were able to make a goal on the uniformity of the co-edit depth, so that when we make catalogs from the co-edit images. 800 02:19:32.709 --> 02:19:34.230 Lynne Jones: that the… 801 02:19:34.360 --> 02:19:41.939 Lynne Jones: Depth in those catalogs is fairly uniform across the sky, and obviously there's a limit to how much you can do there. 802 02:19:42.170 --> 02:19:53.410 Lynne Jones: But if we were to do that, you would still have all of the single visit measurements well-calibrated, so you could do light curve analysis, 803 02:19:53.740 --> 02:19:59.599 Lynne Jones: On all of the visits, and it would just be that your, co-edited visit 804 02:19:59.880 --> 02:20:04.090 Lynne Jones: Co-edited catalog would be more uniform and more shallow. 805 02:20:04.850 --> 02:20:16.130 Leanne Guy (Rubin): Yeah, I mean, the co-added images that are created would be shallower, they would be missing some images, and that would, of course, have an impact on detection in co-ads, which is what goes into the object catalogue, so… 806 02:20:16.170 --> 02:20:32.349 Leanne Guy (Rubin): let's say, quite simply, they wouldn't have the same depth. Let's… if we… if we remove some, you'd lose some depth, so then you might not have, you might have fewer objects detected in those coads, or their parameters might not be measured with the same sort of accuracy or characterization. There might be more uncertainty around them. 807 02:20:32.610 --> 02:20:37.640 Leanne Guy (Rubin): Yep, I think that answers the question. 808 02:20:39.800 --> 02:20:42.740 Lynne Jones: Let's see if, there are questions from… 809 02:20:42.990 --> 02:20:49.410 Lynne Jones: the people listening. Or comments on, like, what the… the impact of this uniformity or not is. 810 02:20:49.840 --> 02:20:50.880 Lynne Jones: Roberta? 811 02:20:52.740 --> 02:20:55.980 Roberto Assef: Yeah, one question, is it… 812 02:20:56.350 --> 02:21:14.589 Roberto Assef: Would it be feasible in any way to sort of think of doing the full code, and then produce a good enough error model, so that at the catalog space, you could add those sort of additional uncertainties to homogenize your catalog at whatever level you want to. 813 02:21:15.220 --> 02:21:16.679 Roberto Assef: To do that. 814 02:21:17.170 --> 02:21:28.880 Leanne Guy (Rubin): I think so, yes, but as Dan's on there, and Dan's more deeply embedded in the pipelines than me, he might have a response to that, but I don't think, in principle, that would be a problem. I'm not sure if it's part of our current processing 815 02:21:29.020 --> 02:21:30.140 Leanne Guy (Rubin): Pipelines. 816 02:21:30.810 --> 02:21:31.460 Roberto Assef: Okay. 817 02:21:32.290 --> 02:21:33.739 Leanne Guy (Rubin): Dan, do you want to throw something in? 818 02:21:34.600 --> 02:21:36.160 Dan Taranu: Well, I was gonna say that… 819 02:21:36.270 --> 02:21:43.549 Dan Taranu: the image we do detection on doesn't necessarily have to be the same as the coeds we do measurement on, and 820 02:21:44.940 --> 02:21:51.240 Dan Taranu: The simplest example is we could do detection on a multivand image, and that has been tested, but not 821 02:21:51.690 --> 02:21:57.879 Dan Taranu: Fully implemented and… The impact hasn't really been measured yet, but it is a possibility. 822 02:21:58.810 --> 02:22:12.139 Leanne Guy (Rubin): Can I throw… can I add something just quickly to that? If we were to do this, though, consistently across the entire widefasted for a data release, that would involve producing two coads, essentially, for every position on the sky, right? To do detection on… 823 02:22:12.290 --> 02:22:15.579 Leanne Guy (Rubin): The deepest, and then measurement on the uniform. 824 02:22:17.990 --> 02:22:27.579 Dan Taranu: Yeah, but I mean, we are already making template coads, for DP2. We have also added the pretty co-ads that we're making images out of, so… 825 02:22:28.360 --> 02:22:38.229 Dan Taranu: I mean, yeah, there is a storage question. If this is… the thing we do detection on is something we persist as a product separately from the other coads, but I don't think it's out of the question. 826 02:22:39.110 --> 02:22:45.709 Leanne Guy (Rubin): So, so technically it's not out of the question, but there is a non-zero question of storage cost plus processing time plus 827 02:22:45.920 --> 02:22:47.200 Leanne Guy (Rubin): etc. 828 02:22:47.460 --> 02:22:59.190 Leanne Guy (Rubin): The short of it is, I can't tell you we can do that right now, because it's got budget involved, and I'd have to go back and talk to other people as well, but it's good to understand that the scientific and technical side doesn't necessarily pose any problems. 829 02:22:59.190 --> 02:23:12.549 Lynne Jones: And my understanding from previous questions about this was that it was… it probably did… was out of scope, especially once you included all the catalogs that you would generate from that, as well as the co-ed itself. 830 02:23:12.720 --> 02:23:14.980 Lynne Jones: But yeah, that, I mean… 831 02:23:15.460 --> 02:23:17.610 Lynne Jones: Those are really good questions, like. 832 02:23:17.610 --> 02:23:26.539 Leanne Guy (Rubin): I mean, there's also going to be provenance questions as well, and keeping track of all this, and what was done on what, so there's all sorts of, you know, data wrangling that has to go in as well. 833 02:23:26.880 --> 02:23:29.300 Leanne Guy (Rubin): Yeah. 834 02:23:31.110 --> 02:23:33.109 Leanne Guy (Rubin): Like, it's not just a flip-the-switch thing. 835 02:23:33.110 --> 02:23:33.430 Roberto Assef: Good. 836 02:23:33.430 --> 02:23:35.950 Leanne Guy (Rubin): There is work involved, but it's not, 837 02:23:36.240 --> 02:23:38.840 Leanne Guy (Rubin): It's… it's not, what's the word? 838 02:23:39.540 --> 02:23:42.410 Leanne Guy (Rubin): Well, we would know how to do it, like, yeah. 839 02:23:42.410 --> 02:23:45.959 Lynne Jones: But this does raise the point that somebody else could do it, too. 840 02:23:46.520 --> 02:23:54.429 Leanne Guy (Rubin): Indeed. But then it… that also raises the point of, you know, how do we define our data releases as our, sort of, flagship product? 841 02:23:54.920 --> 02:23:58.410 Leanne Guy (Rubin): That's… yeah, sorry, we're interrupting Rachel. 842 02:24:02.280 --> 02:24:05.860 Rachel Mandelbaum: You can't interrupt someone who hasn't started talking. 843 02:24:06.930 --> 02:24:10.010 Rachel Mandelbaum: so, I just… 844 02:24:10.640 --> 02:24:16.770 Rachel Mandelbaum: I… it could be that I… that I… that I missed something, but the way this slide and some of the discussion was framed. 845 02:24:16.880 --> 02:24:36.310 Rachel Mandelbaum: It seems like there may be a lack of awareness that there's been a lot of work on desk in, you know, defining metrics of sufficient uniformity in COAGs, and, quite a few people, you know, Boris Leistat, Renee Losec, me, a few others, put a lot of time and effort into getting metrics into MAF. 846 02:24:36.640 --> 02:24:39.089 Rachel Mandelbaum: So that they could be 847 02:24:39.290 --> 02:24:52.780 Rachel Mandelbaum: you know, run on the simulations and use to assess them. They cover, a subset of the questions one cares about with uniformity, so if there's a strategy that, for example, the metrics currently assume that if 848 02:24:52.890 --> 02:25:07.320 Rachel Mandelbaum: you know, RI and Z band are uniform-ish than the others are, so if there's a simulation for which that assumption is false, they won't catch that. But, you know, a lot of work went into that, and I wanted to advocate for those being included by default. 849 02:25:07.410 --> 02:25:20.160 Rachel Mandelbaum: and used, at least in part, to address this. I also want to say that I recognize that, you know, there are other science cases besides the Cosmology ones and desk for which uniformity matters, and it could be that 850 02:25:20.220 --> 02:25:32.069 Rachel Mandelbaum: for example, for galaxies, maybe the criteria are a bit different, but… but I do think that having some metrics is better than having no metrics, so I wanted to flag that, and I'll put a link in the, in the Slack 851 02:25:32.270 --> 02:25:35.660 Rachel Mandelbaum: Channel for this workshop, as well, to the, to the paper. 852 02:25:36.030 --> 02:25:51.680 Lynne Jones: Yeah, thank you, Rachel. I mean, you have a very good point, and I will apologize, because we did not run these metrics on the current set of simulations. We had missed including this in the automatic processing, and it turns out 853 02:25:51.770 --> 02:26:01.029 Lynne Jones: when we went back to look at it, there… we… we actually… there's a, NumPy upgrade-related issue with… with… 854 02:26:01.200 --> 02:26:02.430 Lynne Jones: Running it. 855 02:26:02.740 --> 02:26:16.980 Lynne Jones: So, we'll… we will look at that, we will work with you guys to make sure we're fixing it in a way that is consistent with your, outputs. I think what I'm missing, and maybe this is already in the metric, and I'm just missing it, is… 856 02:26:17.810 --> 02:26:29.679 Lynne Jones: I thought that the metrics indicated which simulations were better than others, and not necessarily gave the guidance that would be, if data management was setting out. 857 02:26:29.680 --> 02:26:40.239 Lynne Jones: to make a uniform co-add, what is their specific goal? And maybe I just missed it, and that's, like, on my part for not understanding what the metric is telling me. 858 02:26:41.660 --> 02:26:49.019 Lynne Jones: But I didn't know if there was a number on, like, this is the uniformity requirement at the end. 859 02:26:51.020 --> 02:26:56.840 Rachel Mandelbaum: So, we might want to talk offline about that. I think the short answer is that 860 02:26:57.280 --> 02:27:12.600 Rachel Mandelbaum: For one of the metrics, there is essentially a criterion one can apply, and, you know, we used it that way in the paper. But I do want to say that, you know, the reason that people have found it kind of slippery is, you know, is this uniform enough? 861 02:27:12.820 --> 02:27:16.020 Rachel Mandelbaum: Because the answer is that when it's not uniform. 862 02:27:16.240 --> 02:27:33.189 Rachel Mandelbaum: one has to try to mitigate that with, you know, like, how you do the analysis. So, you know, in principle, if it's really non-uniform, but maybe, you know, people spend, like, years putting together new analysis methods, technically, yes, they… maybe they could do cosmology, but, like. 863 02:27:33.320 --> 02:27:37.839 Rachel Mandelbaum: I'm not sure that's what we should be aiming for. 864 02:27:37.960 --> 02:27:42.710 Rachel Mandelbaum: So, the metrics generally are about, you know, with existing analysis methods. 865 02:27:42.920 --> 02:27:59.620 Rachel Mandelbaum: you know, which still take quite a while, lots of work and validation to apply to, you know, a large imaging survey, you know, is this, is this, uniform enough? And we can talk details offline, maybe, but, I wanted to just share the… 866 02:28:00.190 --> 02:28:05.400 Rachel Mandelbaum: the… the basic thought process behind, those metrics. 867 02:28:12.080 --> 02:28:13.120 Lynne Jones: Sora? 868 02:28:14.100 --> 02:28:22.109 Saurabh Jha: Yeah, I think, you know, I second everything Rachel just said. Just one part of it, which, and I'm really glad to hear from Leanne and Dan that, you know. 869 02:28:22.110 --> 02:28:38.540 Saurabh Jha: possibilities are, you know, not really off the table. It's not exactly the message that we'd sort of internalized a while ago, and so I think that's a very positive development. I think part of it was this philosophical idea, right? If you have, you know, quote-unquote, good visits in some part of the sky. 870 02:28:38.540 --> 02:29:01.049 Saurabh Jha: in time for a data release, are you going to deliberately not include them in a co-add? And I think the… there was at least a philosophical bent, at least coming from, you know, some portions of the community that said, no, you would have to include them in a data release. And so then, you know, we'd be talking about two separate coads, a uniform one and a full one. 871 02:29:01.050 --> 02:29:19.679 Saurabh Jha: But, you know, I think from DESC, I think also Galaxies, as I recall, had this as their highest, priority scientifically, is that for the coads and the catalogs that are made from those coads to be as uniform as possible. And of course, you know, those first two questions, you know, what does it actually mean? What does uniformity mean? I think that's a totally valid question. 872 02:29:19.680 --> 02:29:26.019 Saurabh Jha: But if it is possible to do something like that, where we know that those visits, you know, even if they're there. 873 02:29:26.250 --> 02:29:33.549 Saurabh Jha: They've been sitting on disk for a few months, and now is the time for the new data release, and they're gonna be treated just as single 874 02:29:33.550 --> 02:29:58.460 Saurabh Jha: visits, and they will show up in the COAD in the next data release, or in the final data release. I think that would be a huge scientific win if we could have some sort of, you know, definition of what a uniform co-ad and catalog means. That's up to the scientific community. But as that, as the main product of a data release, is something closer to uniform, I think that would be a huge scientific win. So I'm all in support 875 02:29:58.460 --> 02:30:07.600 Saurabh Jha: of trying to make that, you know, technically feasible and have the science drive the, you know, technical and budgetary requirements. 876 02:30:09.420 --> 02:30:10.930 Lynne Jones: Yeah, and, and… 877 02:30:11.520 --> 02:30:28.700 Lynne Jones: I know Desk did do this analysis of, like, how much depth you would lose if you were just correcting for rolling cadence all the time. And it was a significant amount of depth, so it is also possible that what we end up looking at is, some kind of… 878 02:30:28.820 --> 02:30:47.089 Lynne Jones: hybrid, where we do decide, okay, these will be uniform data releases, these may not, just based on the rolling cadence, but then there is this aspect of, like, we will have non-uniformity from the TOs, from the special surveys, from other things, like, if we include those stripes that Eric showed earlier. 879 02:30:47.190 --> 02:30:49.600 Lynne Jones: Right, that were the engineering data. 880 02:30:49.930 --> 02:30:58.460 Lynne Jones: That is very non-uniform. So, what do we do with all of this, and when do we want to, 881 02:30:58.560 --> 02:31:03.860 Lynne Jones: ensure we have uniform data releases. So I think these are all really good questions, and it's… 882 02:31:03.990 --> 02:31:09.280 Lynne Jones: there's… there's things we can do at Survey Strategy to make it, 883 02:31:09.430 --> 02:31:17.690 Lynne Jones: make it a good place to start from, but I do think that we can't make it all uniform from survey strategy at the end of the day. 884 02:31:18.800 --> 02:31:32.849 Saurabh Jha: Yeah, I agree, and I was focusing specifically on the uniform checkpoints that are, you know, in either one, you know, 14710 or 12510, you know, whatever it ends up being, those four checkpoints where we think it's going to be roughly uniform. 885 02:31:33.260 --> 02:31:36.989 Lynne Jones: Yeah, I think that's a great approach. Leanne? 886 02:31:38.480 --> 02:31:54.869 Leanne Guy (Rubin): Yeah, so I put my hand up to say something, and I'm going to respond, though, to a few of the points that came up. So, Saurabh, yes, you're right. In the past, there was sort of more of a… I wouldn't say it was a message, but it was maybe a bit of a reluctance for us to pivot our strategy to make uniform coeds during the construction period. 887 02:31:54.870 --> 02:32:00.430 Leanne Guy (Rubin): We had, the DM Science team, had a lot of discussions with Rachel and other people on the desk about this. 888 02:32:00.830 --> 02:32:03.250 Leanne Guy (Rubin): At the time, though, it wasn't so much that 889 02:32:03.250 --> 02:32:28.250 Leanne Guy (Rubin): we'd rejected the idea, but just that there were other… there were other avenues to explore, with the survey, and with trying to, you know, with trying to work this into the survey and not having to make duplicate sets of data products, and not having to make two sets of data products. So we wanted to explore all those avenues first, before we actually got to the point of doing work, which would, you know, have to go into our system to make these extra data products, to curate them, to have provenance, to search 890 02:32:28.250 --> 02:32:35.389 Leanne Guy (Rubin): of them, etc. And to pay the, you know, it is a non-zero cost increase to serve up an extra set of coads and do this work, so… 891 02:32:35.790 --> 02:32:46.180 Leanne Guy (Rubin): it wasn't off the table, it's just we wanted to explore all the other easier options first about, about, you know, getting this into the baseline survey cadence. So that's more what that was about. 892 02:32:49.960 --> 02:33:02.670 Leanne Guy (Rubin): let's see, what did you… you said it was… it would be a scientific win if we could have something like this, but it… doesn't that really depend on what science people are doing? Because uniform coads does sacrifice depth. 893 02:33:02.830 --> 02:33:17.189 Leanne Guy (Rubin): And my recollection from… I forget who did the paper, someone on the desk, was it was something like 10% over 10 years, was it? Or maybe it was a bit less than that on that sort of order, I can't remember, but… I mean, you do sacrifice depth, and it is, like, not including data, so… 894 02:33:18.430 --> 02:33:25.750 Leanne Guy (Rubin): I guess it doesn't… it just doesn't it depend on what science people are trying to do as to whether it's a scientific gain or not? 895 02:33:26.710 --> 02:33:51.410 Saurabh Jha: Yeah, yeah, for sure. I mean, I was sort of, maybe responding maybe too eagerly to the idea that there would be two sets. One would be a full, and one would be a uniform, and so you wouldn't have… it wouldn't be such a trade-off. I think, you know, for a lot of time domain, that's going to be a lot of single-visit science anyway. We have this separate issue about nightly co-ads or monthly co-ads, and you know, like, there are all these other time scales you could consider for other science cases. 896 02:33:51.410 --> 02:33:54.609 Saurabh Jha: So I didn't want to open that discussion. 897 02:33:54.610 --> 02:33:56.430 Leanne Guy (Rubin): Yeah, I… 898 02:33:56.430 --> 02:34:07.589 Saurabh Jha: I fully agree, yeah, different science cases will have different requirements, but, you know, for Desk and Galaxy, certainly having catalogs as uniform as possible across the sky is a big scientific… 899 02:34:07.590 --> 02:34:15.059 Leanne Guy (Rubin): So if we could set up the two sets of data products, the depth-optimized COAD and the, uniform-optimized COAD. 900 02:34:15.300 --> 02:34:19.120 Leanne Guy (Rubin): together. Yes, that would be a science game for everyone. 901 02:34:19.980 --> 02:34:32.190 Leanne Guy (Rubin): I guess I should probably go back and try to cost that now, given that we've gotten to this point. Cost in terms of actual dollars and cost in terms of people, time, effort, you know, all the rest of it. 902 02:34:33.750 --> 02:34:38.699 Leanne Guy (Rubin): Okay, so what I did put my hand up to ask about, unless, Rachel, you want to say something about what I just mentioned? 903 02:34:39.130 --> 02:34:40.610 Leanne Guy (Rubin): I have a different question. 904 02:34:41.370 --> 02:34:44.329 Rachel Mandelbaum: It is… it is kind of about what you… you just mentioned. 905 02:34:44.330 --> 02:34:45.000 Leanne Guy (Rubin): Go ahead. 906 02:34:45.000 --> 02:34:51.380 Rachel Mandelbaum: kind of the costs and the trade-offs in these different things you were just talking about. So, 907 02:34:51.620 --> 02:34:54.130 Rachel Mandelbaum: It could be this isn't quite what you meant, but… 908 02:34:54.530 --> 02:34:55.100 Rachel Mandelbaum: like. 909 02:34:55.610 --> 02:35:07.419 Rachel Mandelbaum: when we see, some of the depth maps where, for example, the TO observations are included together with everything else, and leading to some splotchiness, you know, at year 10, 910 02:35:07.580 --> 02:35:09.560 Rachel Mandelbaum: I had thought that that… 911 02:35:09.930 --> 02:35:23.429 Rachel Mandelbaum: could actually be more effort than a typical co-add, because, like, some of the exposures might have different exposure times. Like, it might actually be harder to throw the TOOs in than it is to, like, exclude them, and so it's felt like an… 912 02:35:23.580 --> 02:35:28.000 Rachel Mandelbaum: like, the cost trade-off isn't just that the uniform co-add is, you know. 913 02:35:28.000 --> 02:35:28.350 Leanne Guy (Rubin): Yeah. 914 02:35:28.350 --> 02:35:32.070 Rachel Mandelbaum: extra effort, but it could be I'm not totally… 915 02:35:32.370 --> 02:35:32.920 Lynne Jones: Yeah. 916 02:35:32.920 --> 02:35:34.249 Leanne Guy (Rubin): Lynn wants to say something. 917 02:35:34.250 --> 02:35:39.240 Lynne Jones: A little hard to find all the things and not hit my slides, sorry. 918 02:35:40.280 --> 02:35:58.140 Lynne Jones: Yes, and then there's also the question that, like, the TO observations may be at higher air mass, and they could be under, like, non-optimal conditions because the timing is the constraint. There will be visits that are not included in the coads because they don't meet quality. 919 02:35:58.200 --> 02:36:14.220 Lynne Jones: constraints. So we're already going to be not including some visits into the co-ads, and so this is maybe, like, adding an extra level of intentionally excluding visits, which could otherwise have been included, I think is one way to look at it. 920 02:36:15.610 --> 02:36:26.289 Lynne Jones: I am gonna say, we should move along to Desi, but we do have extra discussion time after DESI to cover any questions that have come up, throughout… 921 02:36:26.310 --> 02:36:36.030 Lynne Jones: all of this area. And I also do think this is very good preparation for when we talk about the DESI stuff, because that does also introduce some non-uniformity. 922 02:36:36.200 --> 02:36:41.259 Lynne Jones: But I'm gonna… if you have something to wrap up here real quick, Leanne. 923 02:36:41.260 --> 02:36:49.499 Leanne Guy (Rubin): Yeah, very, very quickly, but we can come back to this discussion. You've got a good starting set of questions there. A couple of others that I'd throw into it are. 924 02:36:49.500 --> 02:37:13.229 Leanne Guy (Rubin): And very importantly, how do we select which images to not include in the co-ad? And there's a whole lot of criteria. You know, we already have quality cuts on images to include in coads like seeing, for example. But, you know, does, for example, the time distribution of images throughout a co-add have any impact on the science people want to do? So that's also a really important one that I think data management cannot decide. 925 02:37:13.550 --> 02:37:21.440 Leanne Guy (Rubin): And we need some sort of algorithm, we need some sort of selection process agreed by the community across all sciences as to how 926 02:37:21.540 --> 02:37:23.230 Leanne Guy (Rubin): Optimally, to decide. 927 02:37:23.430 --> 02:37:34.189 Leanne Guy (Rubin): you know, what are the criteria that you want to cut on, and how do you combine those criteria to satisfy all the different sciences? That's just another important question I want to throw in there. 928 02:37:36.010 --> 02:37:37.040 Lynne Jones: Yeah, that… 929 02:37:37.390 --> 02:37:41.450 Lynne Jones: I didn't… I didn't write that, but that is definitely a good one. How do you pick the visits? 930 02:37:41.950 --> 02:37:42.850 Lynne Jones: Okay. 931 02:37:43.630 --> 02:37:45.330 Lynne Jones: So, 932 02:37:45.670 --> 02:38:03.450 Lynne Jones: I'm going to give a really brief overview on, what we did for the DESI simulations and how that contrasts to how we would be acquiring visits, otherwise. And then I'm going to hand this over to David, who will tell you all about the great, synergies that come out of, 933 02:38:03.810 --> 02:38:09.820 Lynne Jones: What could be enabled by the… this change in the survey strategy? 934 02:38:10.550 --> 02:38:13.729 Lynne Jones: So the basic idea in the request is, 935 02:38:14.140 --> 02:38:31.020 Lynne Jones: to take this about 5,000 square degree area that is shown here in the yellow and purple areas, and sort of accelerate the coverage of that area to get to a depth of 30 to 40 visits in each of you, GRIZY, by the end of year 4. 936 02:38:33.360 --> 02:38:40.399 Lynne Jones: And the initial, like, sort of question was, could we get to the yellow portion of that footprint by the end of year two? 937 02:38:40.650 --> 02:38:49.669 Lynne Jones: On the left, what I have is the median number of visits over the sky in the baseline survey. So this is a median, and it's over… 938 02:38:50.090 --> 02:38:58.229 Lynne Jones: Just without any, any, influence, and as you've seen before, rolling cadence does start to influence things after 939 02:38:59.610 --> 02:39:01.500 Lynne Jones: After you… when you get to year two. 940 02:39:01.810 --> 02:39:07.980 Lynne Jones: But this is… this is sort of median number of visits that we would have over the sky, and you can see 941 02:39:08.500 --> 02:39:17.209 Lynne Jones: in RISY in the redder bands, we would get to that, or close to that depth at the end of year 3. 942 02:39:17.490 --> 02:39:28.369 Lynne Jones: And then UNG are where we have the problem with this goal, because at year 3, we're still very far back at, like, 10 and 16 visits. 943 02:39:28.860 --> 02:39:39.230 Lynne Jones: Note that our template tier has already accelerated U and G in year one, to get to the number of visits we need for the templates. 944 02:39:39.970 --> 02:39:49.819 Lynne Jones: And we don't actually reach 30 visits in these bands until year 6 or year 8, if we go with a natural cadence. 945 02:39:50.410 --> 02:40:06.659 Lynne Jones: So that's the primary problem. What you see, if you look at, like, our band, is that year 4, so after the… year four would be the end of the, the request, can you cover this footprint to your 946 02:40:06.760 --> 02:40:20.230 Lynne Jones: to this number of visits by year 4. At year 4 in G-Band, the dizzy footprint is very obvious, because it's ahead of the rest of the sky, and at year four, in our band, it's not really very obvious. 947 02:40:21.430 --> 02:40:25.360 Lynne Jones: Which just matches what we see from the number of visits per year. 948 02:40:26.730 --> 02:40:32.720 Lynne Jones: The other thing to consider with this is that… within the DESE footprint. 949 02:40:32.750 --> 02:40:52.390 Lynne Jones: So this is the number of… the night, and the number of visits we've acquired to that… to… up to that night. And so, in year one, we really… because we have this template tier, because we're pushing hard to get all the visits for the template, there isn't really that much of a change. Whether you're in the DESI footprint or outside the DESE footprint, we're doing the same thing in year one. 950 02:40:52.950 --> 02:40:58.110 Lynne Jones: But… After… after year one, 951 02:40:58.280 --> 02:41:06.020 Lynne Jones: if in the DESE simulations, we sort of switch over to, like, okay, let's try and get the, the visits for this 952 02:41:06.180 --> 02:41:10.290 Lynne Jones: footprint. You can see that it, accelerates. 953 02:41:10.460 --> 02:41:20.629 Lynne Jones: And so we get up to, this is a part in the year 2 footprint, so the yellow area. So you can see we get up to, 954 02:41:22.270 --> 02:41:25.260 Lynne Jones: Maybe not. Okay, sorry, it's not vibe. 955 02:41:25.820 --> 02:41:32.280 Lynne Jones: So we get, we get a lot of visits in, UGRIZ, 956 02:41:32.820 --> 02:41:50.679 Lynne Jones: because of the being in the Desi footprint, but then after you get that number of visits, because now you're very far ahead in this part of the sky, you get very few visits for a very long time, and then eventually the rest of the sky catches up to you, and so you say… so the scheduler 957 02:41:50.930 --> 02:41:57.749 Lynne Jones: Says, okay, great, now we're… we're balanced in the footprint, and we can… we should start taking visits here again. 958 02:41:57.870 --> 02:41:59.480 Lynne Jones: And so you see this… 959 02:41:59.720 --> 02:42:10.049 Lynne Jones: acceleration, and then a weight until you take more visits. And that's not as strong in the rider bands, because those are more on par with the rest of the sky. 960 02:42:10.280 --> 02:42:13.600 Lynne Jones: And then outside of the DESI footprint. 961 02:42:13.900 --> 02:42:27.130 Lynne Jones: So this is a much lower declination that's outside of that footprint. You see that you get a little bit of suppression in that period where it's… the scheduler is concentrating on DESI, and then you… you start 962 02:42:27.410 --> 02:42:29.619 Lynne Jones: Recovering visits after that. 963 02:42:33.440 --> 02:42:42.619 Lynne Jones: And of course, we can look at our metrics. The metrics here… so this is DESI, and we have two simulations for the DESI footprint. We… 964 02:42:43.170 --> 02:43:00.480 Lynne Jones: oops, sorry, we have two simulations to date for the DESI footprint. DESI yearly does that yellow band and blue band completing by year 2 and Year 4, and the DESI 3040, actually tries to complete the whole thing by year 2, which I'm sure Desi loves. 965 02:43:00.480 --> 02:43:04.739 Lynne Jones: But this does have more of an impact on, 966 02:43:04.760 --> 02:43:08.909 Lynne Jones: When you'll see that delay in the footprint. 967 02:43:09.070 --> 02:43:21.200 Lynne Jones: It's kind of a much stronger effect than we actually intended. So, the DESI yearly completes the request by year 2 and Year 4 on the relevant parts of that footprint. 968 02:43:21.630 --> 02:43:22.480 Lynne Jones: And… 969 02:43:23.770 --> 02:43:33.110 Lynne Jones: It's not clear to me that our current metrics, especially when we evaluate at the end of year 10, that they really capture, any… 970 02:43:33.660 --> 02:43:48.050 Lynne Jones: potential benefits, or the, you know, full impact for this. So, I think you need, you know, we take this with a grain of salt. There certainly are some metrics which don't seem to be impacted by the end of year 10, which, as you would expect, the co-added depth 971 02:43:48.160 --> 02:43:55.709 Lynne Jones: If… if you have static science that only cares about co-added depth, at the end of year 10, the co-added depths are very similar. 972 02:43:55.950 --> 02:43:59.089 Lynne Jones: You didn't gain or lose by having 973 02:43:59.200 --> 02:44:01.969 Lynne Jones: This reshuffling of the observation cadence. 974 02:44:02.580 --> 02:44:14.050 Lynne Jones: And for some time domain, this will be an impact, and it's not obvious that when we look at the impact at the end of year 10, that we've… we've captured this properly or not. 975 02:44:15.850 --> 02:44:29.919 Lynne Jones: And then I was gonna say, we do have one simulation that we've not made yet, but that we will look at, which… it's not clear it will make a huge difference, but, the idea is instead of covering 976 02:44:30.140 --> 02:44:41.899 Lynne Jones: the whole footprint by year 4. Instead, we split it up into smaller chunks and let the last chunk sort of hang off the end, so it's at the end of year 5. And so. 977 02:44:42.080 --> 02:44:59.900 Lynne Jones: this is not necessarily the order you would do this, but I made a little plot to give the idea. So the different colors on the right are, like, doing 1,000… about 1,000 square degrees at the end of year two, another by the end of year 3, and so then you end up with… 978 02:45:00.110 --> 02:45:05.870 Lynne Jones: the final… 1,000 square degrees being completed at the end of year 10. 979 02:45:06.000 --> 02:45:06.880 Lynne Jones: Five. 980 02:45:07.420 --> 02:45:14.930 Lynne Jones: And… It's… it's worth noting, like, this… one thing that would happen here is that after year 3, 981 02:45:15.320 --> 02:45:21.830 Lynne Jones: And maybe even during year 3, you wouldn't be accelerating any of the redder bands. So… 982 02:45:22.080 --> 02:45:35.230 Lynne Jones: the redder band cadence would only be disturbed in two of these bands, but the bluer visits, like U and G, would still be disturbed in all of the band passes, and it's just… 983 02:45:35.800 --> 02:45:41.430 Lynne Jones: It might not be quite as strong of an effect, but it would still be there, and you would still… 984 02:45:41.660 --> 02:45:47.929 Lynne Jones: if you completed to 30 visits here, you're 5. You… oop, sorry. 985 02:45:48.040 --> 02:45:51.759 Lynne Jones: You would still be sort of waiting until about, 986 02:45:52.440 --> 02:46:03.649 Lynne Jones: your 7 or 8 until you started picking up more visits in this area. Unless we do something else again, like, add more visits in UNG to this part of the sky. 987 02:46:04.560 --> 02:46:09.229 Lynne Jones: Which is yet another variation on the survey strategy, and it's not… 988 02:46:09.450 --> 02:46:21.659 Lynne Jones: super clear, given that we've lost 10% of… lost. Since we… since we've updated our forecasts to be slightly fewer visits overall, what exactly the impact of that is? 989 02:46:22.830 --> 02:46:32.589 Lynne Jones: So now I'm going to turn it over to David to tell you about all of the good things that come out of this. Oh, sorry, Kathy, you have a quick question? 990 02:46:33.760 --> 02:46:38.810 Kathy Vivas: Yeah, my question, Lynn, is, how do you see… 991 02:46:38.960 --> 02:46:43.730 Kathy Vivas: This strategy will combine with running cadence. 992 02:46:45.530 --> 02:46:54.210 Lynne Jones: Yeah, so… so the original request was actually quite smart, because in… it doesn't… 993 02:46:54.340 --> 02:47:11.060 Lynne Jones: quite line up, now we've changed the start of the survey, but in the original version of the survey strategy, which… where we had started this simulation on November, this year 2 and Year 4 did align with the rolling cadence, so it was kind of like. 994 02:47:11.300 --> 02:47:12.970 Lynne Jones: Building on the rolling cadence. 995 02:47:13.110 --> 02:47:21.409 Lynne Jones: When we changed the start of the survey, we changed which part, like, the part of the sky, and so there's some changes about whether we're in a… 996 02:47:21.560 --> 02:47:34.739 Lynne Jones: up deck band or a down deck band, and so it doesn't quite align anymore, but that's something we could reinstate, and certainly, when you look at something like this, we could arrange these to be more smartly aligned with the rolling cadence. 997 02:47:36.160 --> 02:47:47.790 Lynne Jones: All right, I do want to make sure that David gets to tell you about the good aspects here. So, I'm actually going to cut off questions, and we can come back and discuss this more afterwards. 998 02:47:48.730 --> 02:47:50.550 Lynne Jones: David, is that okay? Are you… 999 02:47:50.550 --> 02:47:54.649 David Schlegel: Yeah, no, that's good, yeah. If I could share also. 1000 02:47:54.650 --> 02:47:55.480 Lynne Jones: Oh, sorry. 1001 02:47:55.480 --> 02:48:10.980 David Schlegel: Yeah, let me start with Lynn. It's… yeah, it's been wonderful working with this SCOC group, very responsive, and we are trying to, you know, approach this in a way that we're making minimal impact on, group and observing. 1002 02:48:13.810 --> 02:48:15.550 David Schlegel: Okay, 1003 02:48:16.490 --> 02:48:33.330 David Schlegel: This is my one slide about what is DESI. Hopefully you've heard of DESI before. It's really the most wonderful multi-object spectrograph on the planet right now. Over the past 5 years, it's mapped 47 million galaxies, 20 million stars. 1004 02:48:33.510 --> 02:48:45.359 David Schlegel: This is a fully, 100% DOE-funded, operation, so we're making use of the Noir Lab, telescope at Kit Peak. 1005 02:48:45.890 --> 02:48:54.690 David Schlegel: And then here's just the, the basic stats on this, where it's, it's 5,000, robotic fibers. 1006 02:48:54.910 --> 02:49:02.180 David Schlegel: Broad wavelength range, and the, data quality is just wonderful. 1007 02:49:02.670 --> 02:49:15.229 David Schlegel: Partly because every observation, we get simultaneously 100 standard stars, 600 skies, so we can really produce, excellent Poisson Limited spectra. 1008 02:49:16.360 --> 02:49:29.879 David Schlegel: Okay, these are just, representative spectrum. These are truly representative of what the DESI main survey has been doing, because we do these dynamic exposures where we adjust 1009 02:49:29.970 --> 02:49:45.470 David Schlegel: the open shutter time according to seeing, sky brightness, transparency. And I do want to know what you're talking about, uniformity. We're now operating DeckCam in exactly this mode. 1010 02:49:45.690 --> 02:50:05.579 David Schlegel: It's not too late for Ruben, and here's some quotes here, like, what do people say about dynamic exposures? All good things. From my perspective, one of the best things is we actually get a faster survey, because on good nights, we collect about twice as much data as you might expect. 1011 02:50:05.830 --> 02:50:11.010 David Schlegel: So we really do a lot of catching up on the Prime nights. 1012 02:50:12.040 --> 02:50:17.500 David Schlegel: So, you know, you're talking about, you want to get 10% back? You could easily get 10% back. 1013 02:50:20.250 --> 02:50:27.010 David Schlegel: Okay, starting… actually, I think it's tonight, Desi begins mapping 1014 02:50:27.240 --> 02:50:33.320 David Schlegel: Further south, so we've expanded the, DESI Run 1 footprint, 1015 02:50:33.430 --> 02:50:46.220 David Schlegel: this is the expanded footprint for DESE, that we'll be doing over the next couple years, and I just want to note this because this new area fully overlaps, the Rubin 1016 02:50:46.750 --> 02:50:47.780 David Schlegel: footprint. 1017 02:50:50.900 --> 02:50:58.250 David Schlegel: Okay, what we're interested in enabling here, though, is what we're calling DESI Run 2. 1018 02:50:58.480 --> 02:51:08.290 David Schlegel: So this will be the next phase of the DESI project starting in January 2029. Most of the dark time is focused on a cosmology 1019 02:51:08.500 --> 02:51:21.949 David Schlegel: experiment at redshifts 2 to 3.5 over this, 5,000 square degree equatorial footprint that Lynn was just showing you, and we chose this footprint, 1020 02:51:22.040 --> 02:51:37.279 David Schlegel: Not because this is necessarily our best footprint, it's a little too far south for us, but again, we're trying to minimize our impact on Rubin, so we're fitting this in on the northernmost good sky that Ruben was already planning on observing. 1021 02:51:40.390 --> 02:51:51.480 David Schlegel: Okay, so we have a proposed data exchange between Desi and Ruben, so this is following the policies of both collaborations. 1022 02:51:51.630 --> 02:52:09.770 David Schlegel: Where what we're asking from Ruben is, this, early imaging when necessary over this equatorial footprint, and that's what we'll be using for target selection, for DESIRUN2. So, you know, obviously we need this 1023 02:52:09.890 --> 02:52:16.160 David Schlegel: before Desi run 2, just so we can select the targets. And then… 1024 02:52:16.280 --> 02:52:29.270 David Schlegel: In return on this data exchange, what we've put on the table is, what we call 250 effective dark hours. What that corresponds to is four and a half months 1025 02:52:29.360 --> 02:52:45.150 David Schlegel: of DESI time? And, you know, what can be done with four and a half months of DESI time? Well, if you're talking about the kind of data we've been collecting typically for the last five years, that would be 4 million spectra. 1026 02:52:46.170 --> 02:52:56.930 David Schlegel: Or one can do deeper observations, so, you know, hundreds of thousands of spectra deeper, or some combination of all of these. 1027 02:52:57.040 --> 02:53:12.549 David Schlegel: Another point here is that the data are fully reduced, typically by the time I'm having coffee in the morning, and I get up early, so these data, they're spooled over to NERSC during the night, and 1028 02:53:12.550 --> 02:53:18.700 David Schlegel: you know, we'd say typically available within 12 hours. If you're impatient, they're actually available faster than that. 1029 02:53:22.040 --> 02:53:36.400 David Schlegel: Okay, these observations would be coordinated, between the two projects so that we make, you know, best use of this time. Examples of what could be done that, 1030 02:53:36.600 --> 02:53:50.820 David Schlegel: you know, this, DESI Rubin Working Group has been looking at so far are primarily based on observations in the two deep drilling fields that are available to both telescopes. 1031 02:53:50.820 --> 02:54:01.779 David Schlegel: So we could go quite deep in these deep drilling fields for, PhotoZee catalogs in these footprints. 1032 02:54:01.910 --> 02:54:09.029 David Schlegel: And also, we could be observing transients, within a day of discovery. 1033 02:54:09.030 --> 02:54:25.079 David Schlegel: And in practice, we can do these in such a way that we do observations where you're doing both simultaneously. So you're observing these deep fields, you're picking up new transients, and then you accumulate signal-to-noise on fainter objects at the same time. 1034 02:54:27.960 --> 02:54:42.250 David Schlegel: Desi's already measured about a quarter million redshifts in these two deep drilling fields already. These footprints, they're essentially the same size as the Rubin footprints. The field of view of both instruments is about the same. 1035 02:54:42.250 --> 02:54:55.589 David Schlegel: This just shows you the density of targets that we've already published, and just, you know, you can see the scale here, 50 arcseconds. So very high density of targets that we've already observed. 1036 02:54:55.780 --> 02:55:00.900 David Schlegel: So it's kind of a down payment of what's available in these deep drilling fields. 1037 02:55:02.360 --> 02:55:07.609 David Schlegel: We've also demonstrated, that we can go, 1038 02:55:07.730 --> 02:55:25.380 David Schlegel: quite a bit deeper, so we've taken data up to about 5 hours and demonstrated that we can get Poisson-level spectroscopy. So these are objects where we've observed 1039 02:55:25.570 --> 02:55:31.550 David Schlegel: Well, 3 or 4 hours, 24th, 25th magnitude, spectra. 1040 02:55:32.180 --> 02:55:33.829 David Schlegel: So this is all published. 1041 02:55:35.620 --> 02:55:53.799 David Schlegel: We also have a pretty good understanding of, redshift success rate as a function of integration time, so this is also something that was just published a couple months back, so this is looking at that success rate versus exposure time. It's actually very dependent on the 1042 02:55:53.820 --> 02:56:08.180 David Schlegel: you know, magnitude and colors of objects. So there are parts of color space where, you know, we're already doing this right now. We're observing, for example, luminous red galaxies at redshift of 1 in 15 minutes. 1043 02:56:08.180 --> 02:56:14.139 David Schlegel: Just because it's a color space where we know we can very quickly get a successful redshift. 1044 02:56:17.160 --> 02:56:28.100 David Schlegel: Okay, timeline, so we really need the first bit of, the Rubin imaging. 1045 02:56:28.150 --> 02:56:36.070 David Schlegel: available prior to the start of this Desi Run 2 in January 2029. And we could… 1046 02:56:36.110 --> 02:56:49.869 David Schlegel: you know, it'd be great if we could have all of this prior to 2029, but we're, you know, we're willing to work with Rubin and space this out over a few years, just so that the Rubin imaging is… 1047 02:56:50.000 --> 02:56:54.109 David Schlegel: You know, still prior to each footprint that we're observing with DESE. 1048 02:56:54.890 --> 02:57:03.630 David Schlegel: And then for this, data trade, so the DESI spectroscopy, this could be provided early. 1049 02:57:03.690 --> 02:57:17.379 David Schlegel: And or it could be cadence throughout the DESI Run 2 going through 2034. So, in other words, what we're imagining is, early in DESI Run 2, we would do 1050 02:57:17.380 --> 02:57:25.300 David Schlegel: Some deep observations in these deep drilling fields, and then over the course of, you know, maybe the next 4 or 5 years. 1051 02:57:25.380 --> 02:57:30.660 David Schlegel: You know, do, transient follow-up in those, in those fields. 1052 02:57:30.930 --> 02:57:38.270 David Schlegel: Okay, and then let me just end with DESI has no plans to coordinate with any other surveys, so it really is just… 1053 02:57:38.450 --> 02:57:42.599 David Schlegel: The Ruben that we're trying to coordinate with us on this. 1054 02:57:43.270 --> 02:57:47.109 David Schlegel: Okay, so that's… That's actually all I had to show. 1055 02:57:48.460 --> 02:58:00.409 David Schlegel: And I should note, there are some other DESE folks on as well. We tried to not overwhelm your call, but, but who could answer questions here? 1056 02:58:02.600 --> 02:58:03.410 Lynne Jones: Alright. 1057 02:58:03.810 --> 02:58:06.000 Lynne Jones: Thank you, David. That's, 1058 02:58:06.860 --> 02:58:13.489 Lynne Jones: That's a… that's a great demonstration of what… what we gain from the… from… from doing this. 1059 02:58:13.980 --> 02:58:17.919 Lynne Jones: Yeah, let's go with questions now. Dan? 1060 02:58:20.270 --> 02:58:25.359 Dan Taranu: When you say you don't have plans to coordinate with other surveys, do you mean imaging surveys, or also… 1061 02:58:25.560 --> 02:58:33.440 Dan Taranu: upcoming spectroscopics, I'm thinking of… Subaru PFS is definitely gonna target deep fields. 1062 02:58:35.470 --> 02:58:39.910 Dan Taranu: Foremost, I guess, is not really overlapping, but, 1063 02:58:40.410 --> 02:58:47.899 Dan Taranu: And I don't think they've asked for anything specific, but could you not also make the argument, well, we should also prioritize covering, like, the waves? 1064 02:58:48.090 --> 02:58:49.380 Dan Taranu: foremost. 1065 02:58:49.790 --> 02:58:53.110 Dan Taranu: Fields in a similar fashion. 1066 02:58:55.170 --> 02:58:59.569 David Schlegel: Sorry, that Desi should be coordinating with Waves, or what… 1067 02:59:00.180 --> 02:59:04.019 Dan Taranu: No, so, for the first part. 1068 02:59:04.540 --> 02:59:08.600 Dan Taranu: Are you coordinating at all with Subaru PFS? 1069 02:59:09.260 --> 02:59:11.690 Dan Taranu: In the deep drilling fields, for example. 1070 02:59:12.180 --> 02:59:31.329 David Schlegel: Yeah, so we don't have any coordination. So the only other coordination we have is we are obtaining other imaging that we need for DESI Run 2 from several different telescopes. We're running those imaging surveys within DESE. These are medium-band imaging surveys. 1071 02:59:31.400 --> 02:59:39.119 David Schlegel: So that is our other coordination. That's just internal, as For other spectroscopic projects. 1072 02:59:39.310 --> 02:59:43.300 David Schlegel: we're really far ahead on DESI, and it's… it's kind of… 1073 02:59:43.440 --> 02:59:51.520 David Schlegel: the question gets turned on its head of, you know, these other projects shouldn't repeat what DESI has already done. 1074 02:59:57.430 --> 02:59:59.290 Lynne Jones: Rachel? 1075 03:00:01.760 --> 03:00:05.569 Rachel Mandelbaum: Yeah, I have a comment and a question, if that's okay? 1076 03:00:05.680 --> 03:00:08.649 Rachel Mandelbaum: So the, the comment, 1077 03:00:09.190 --> 03:00:15.710 Rachel Mandelbaum: is more on the earlier part of the presentation. There was a statement that the metrics… you know. 1078 03:00:15.900 --> 03:00:17.660 Rachel Mandelbaum: For impact of… of… 1079 03:00:17.850 --> 03:00:31.410 Rachel Mandelbaum: these strategies on the science, may not capture, you know, the full impact. They may not be designed for that. I want to actually strengthen that to say that several of the desk metrics definitely 1080 03:00:31.510 --> 03:00:35.729 Rachel Mandelbaum: Do not capture the impact of this change in strategy, because they make assumptions about 1081 03:00:35.910 --> 03:00:41.780 Rachel Mandelbaum: the coverage in each band tracking each other in a way that these simulations violate, so I think it's a stronger statement that 1082 03:00:41.980 --> 03:00:48.740 Rachel Mandelbaum: you know, we'll likely need to update the metrics. But then, to ask my actual question, 1083 03:00:49.210 --> 03:01:07.900 Rachel Mandelbaum: One other timeline question that I wanted to understand is, when would a decision have to be made about doing this? Like, at what point would the Rubin strategy need to start to deviate from what it would otherwise be? Because that feels like a pretty important and relevant factor to understand. 1084 03:01:07.900 --> 03:01:12.030 Lynne Jones: Yeah, that is a great question. 1085 03:01:12.210 --> 03:01:16.970 Lynne Jones: I don't actually have a super good answer for you, except for the fact that I would say. 1086 03:01:17.600 --> 03:01:25.449 Lynne Jones: when we did run these simulations with the DESI survey, like, the DESI 3040 and the DESI yearly. 1087 03:01:25.620 --> 03:01:32.990 Lynne Jones: There was no change inside of year one, because the template tier, was put in at a higher priority. 1088 03:01:33.090 --> 03:01:35.440 Lynne Jones: I'm assuming, that's right. Is that right, Peter? 1089 03:01:37.690 --> 03:01:39.040 Peter Yoachim: Yep, that's right. 1090 03:01:39.040 --> 03:01:49.059 Lynne Jones: Yeah, so the templates being a higher priority meant that the templates were trying to get their visits, and because the templates take up most of year one, it just basically means there's no… 1091 03:01:49.250 --> 03:02:01.060 Lynne Jones: actual impact. So yes, we should decide as soon as possible, in practice, if our priority is actually first getting templates, which I think it should be. 1092 03:02:01.060 --> 03:02:09.669 Lynne Jones: But that's my opinion, of course. But then, then… then we have, then we have some time in practice. 1093 03:02:10.040 --> 03:02:20.489 Lynne Jones: we should definitely decide before… I mean, ideally, we decide as soon as possible, because it makes a difference for funding, for various things, right? But, 1094 03:02:21.140 --> 03:02:23.900 Lynne Jones: In practice, if we… 1095 03:02:24.530 --> 03:02:34.180 Lynne Jones: had a strategy in place, like, a decision in place 6 months from now, I think that that would… it would not really impact what we're actually doing on Sky. 1096 03:02:35.140 --> 03:02:50.069 Rachel Mandelbaum: Yeah, and to be clear, it's not like I wanted to push to wait until the latest possible moment. It was more trying to understand, is this, like, a right now decision, or, you know, we should do this within a couple of months, and the time will fly, so, 1097 03:02:50.230 --> 03:02:51.660 Rachel Mandelbaum: Thank you for clarifying. 1098 03:02:52.340 --> 03:02:59.119 David Schlegel: Yeah, I mean, let me just say, from the DESI side, though, we're eager to get to a decision point 1099 03:02:59.380 --> 03:03:10.789 David Schlegel: quickly, even if this isn't perturbing Rubin observations for another year. And that's just, you know, you can imagine that this could blow up the DESE Run 2 1100 03:03:10.920 --> 03:03:11.710 David Schlegel: Planning. 1101 03:03:15.620 --> 03:03:18.250 Lynne Jones: Yeah, definitely. That's good. 1102 03:03:18.680 --> 03:03:19.810 Lynne Jones: Roberto? 1103 03:03:22.470 --> 03:03:33.750 Roberto Assef: Yeah, so, there were… we discussed this a little bit on the impact on the AGN science collaboration in the latest telecom, and there were a couple of questions that, so I… 1104 03:03:34.160 --> 03:03:41.639 Roberto Assef: that I think were very interesting that came up. So, one was, is the DESE2 footprint fixed? 1105 03:03:41.760 --> 03:03:49.139 Roberto Assef: And if so, do you know how much does it overlap with Euro Cedar, at least the German part of Eurosida? 1106 03:03:51.510 --> 03:03:56.129 David Schlegel: Oh, that's a good question. I don't have that right in front of me, but maybe… 1107 03:03:56.870 --> 03:04:05.299 David Schlegel: Maybe one of my collaborators can figure this out quickly, but it's, I mean, you can look at it, it must be a fair amount of overlap, because we're… 1108 03:04:05.900 --> 03:04:09.829 David Schlegel: you know, we're overlapping LSST, which has a fair amount of overlap. 1109 03:04:12.870 --> 03:04:14.649 David Schlegel: So sorry, I don't pull that offhand. 1110 03:04:14.650 --> 03:04:20.480 Roberto Assef: That's fine. And the other question was, 1111 03:04:21.170 --> 03:04:40.270 Roberto Assef: So, right, currently the offer, right, is for the exchange to 250 dark time hours. One of the questions was, would it be instead, or, you know, with some partition, access to all the DES spectra taking over the… 1112 03:04:40.270 --> 03:04:42.280 Roberto Assef: LSSD footprint. 1113 03:04:43.250 --> 03:05:02.750 David Schlegel: So all of the DESI spectra, they are made public on some timescale, and in fact, the DESI DR1 release, which goes back a year now, most of that is actually over the Rubin footprint, in fact, just because we started 1114 03:05:03.000 --> 03:05:15.010 David Schlegel: Or it must be more than half, because we started kind of equatorial with, DESI. So we… we've… we've not discussed that. I… I… 1115 03:05:15.330 --> 03:05:21.220 David Schlegel: The DESE director's on, maybe he would like to respond to that. 1116 03:05:24.210 --> 03:05:25.140 David Schlegel: Michael? 1117 03:05:27.500 --> 03:05:29.330 Michael Levi: I'm sorry, what was the question? 1118 03:05:29.330 --> 03:05:30.150 David Schlegel: Oh. 1119 03:05:30.150 --> 03:05:31.080 Michael Levi: No, sorry. 1120 03:05:31.610 --> 03:05:33.029 David Schlegel: Do you want to just repeat your question? 1121 03:05:33.030 --> 03:05:37.860 Roberto Assef: Sure, sure. So, the question that came up was, would it be, would… 1122 03:05:38.050 --> 03:05:48.039 Roberto Assef: could there be access to the private DESE data, DESE2 data, on the regions that overlap the LSST footprint? 1123 03:05:48.040 --> 03:05:55.260 Michael Levi: Well, the 250 hours that we're talking about, I think the answer is yes, because you would be defining what those are. 1124 03:05:57.050 --> 03:05:59.020 Roberto Assef: Oh, right, but not… okay. 1125 03:05:59.350 --> 03:06:05.140 Roberto Assef: Okay, so I think the question was, instead of the 250 hours, access to all the spectra. 1126 03:06:06.980 --> 03:06:11.899 Roberto Assef: But, I mean, I see what you mean, right? So we could coordinate to make sure that it's reconciled. 1127 03:06:11.900 --> 03:06:14.429 Michael Levi: So, no, this is not an offer to open up the… 1128 03:06:14.580 --> 03:06:20.220 Michael Levi: proprietary, all of the proprietary, DESI data, I mean, that would be… 1129 03:06:20.380 --> 03:06:24.040 Michael Levi: It's possible for, you know, you as an individual 1130 03:06:24.320 --> 03:06:38.309 Michael Levi: to come in to DESE as an external collaborator with a particular scientific project to work with one of our other collaborators within DESE, to work with us on a topic where then you would have access to some of that information. 1131 03:06:38.500 --> 03:06:46.580 Michael Levi: So that's technically possible. You know, a broader… if you're asking a question, well, what about a collaboration between 1132 03:06:47.040 --> 03:06:52.209 Michael Levi: Desi and E. Rosita, you know, that's probably out of context for this meeting, but… 1133 03:06:52.210 --> 03:06:53.020 Roberto Assef: Yeah, absolutely. 1134 03:06:53.140 --> 03:06:57.370 Michael Levi: So, I think that's, you know, it would be a different format than what we're talking about here. 1135 03:06:57.880 --> 03:06:59.250 Roberto Assef: Okay. Thank you. 1136 03:07:00.950 --> 03:07:01.830 Lynne Jones: Toronto? 1137 03:07:03.070 --> 03:07:27.179 Saurabh Jha: Yeah, David, I just wanted to understand a little better, the DESI Run 2 needs, and maybe this is probably in some document, and I apologize if I have not read the appropriate document. But the example spectra you showed, like, even the long exposure ones, were getting down to, you know, 23rd, 24th magnitude, and I guess I understand that the DESI Run 2 is targeting somewhat higher redshift, so maybe, maybe slightly fainter is the goal, but… 1138 03:07:27.180 --> 03:07:50.389 Saurabh Jha: That was a surprising number a little bit to me, because if you're requesting 4-year-ish Rubin depth, that seems a lot deeper. So, you know, even in one visit, you're getting to close to 24th magnitude in U, 24.5 in G, so it feels like in a few visits, I know maybe you need signal and noise of 10 or 50 in the images, so maybe you just need very high, 1139 03:07:50.390 --> 03:08:02.159 Saurabh Jha: fidelity photometry, but it seems like in 4 years of Rubin, you get down to, like, 26th magnitude, and so is it possible that you can do the target selection with less data from Rubin? 1140 03:08:02.800 --> 03:08:14.469 David Schlegel: Yeah, we started with a request that was even deeper, and then dialed that back after some studies. The, the reason is, you know, these are the high-rich 1141 03:08:14.730 --> 03:08:25.899 David Schlegel: galaxies for which we can most efficiently and quickly, get a redshift. So they're not typical redshift 3 galaxies, they're the ones that we can 1142 03:08:26.030 --> 03:08:45.749 David Schlegel: get a redshift up. So the, primarily, you should think of these as the U-dropout galaxies, where if you want an efficient selection of… it's just the brightest U-dropout galaxies, you need about these 30 visit depths. 1143 03:08:45.890 --> 03:08:50.000 David Schlegel: The other objects that we're looking at, it's, 1144 03:08:50.300 --> 03:09:03.870 David Schlegel: It's these Lyman Alpha emitters, where their broadband photometry is really quite faint, because they're objects where we've picked them up as a 25th magnitude object. 1145 03:09:05.140 --> 03:09:15.510 David Schlegel: In medium band imaging, and then the broadband depth is deeper than that, but we still want the broadband color to distinguish those from interlopers. 1146 03:09:15.690 --> 03:09:20.489 David Schlegel: So, you know, we've looked pretty carefully at these depth requirements. 1147 03:09:22.470 --> 03:09:31.099 Julien Guy: Maybe to complement that, we, we have run target selection with random forest, assuming different depths of LSST. 1148 03:09:31.480 --> 03:09:35.910 Julien Guy: And, for four-year depths, which is equivalent to what we're discussing here. 1149 03:09:36.490 --> 03:09:43.740 Julien Guy: we get a purity of only, 55%. So, we really need that depth to, 1150 03:09:44.010 --> 03:09:46.700 Julien Guy: To get an efficient survey afterwards. 1151 03:09:48.400 --> 03:09:49.250 Saurabh Jha: Thanks. 1152 03:09:54.190 --> 03:09:55.390 Lynne Jones: John? 1153 03:09:58.860 --> 03:10:01.509 John Gizis: Oh, sorry, I didn't realize my camera was off. 1154 03:10:01.680 --> 03:10:20.289 John Gizis: So I guess, so my science case, it doesn't make any difference in the long run, you know, when you move the filters around, particularly the blue filters. But I do want to ask, because I've spent a lot of time lately hearing about Roman, it seems like this preferentially moves U and G observations out of Roman overlap. 1155 03:10:20.720 --> 03:10:25.929 John Gizis: In the upcoming years, and since we now believe it will really launch in August. 1156 03:10:26.180 --> 03:10:34.250 John Gizis: It seems like this is a very high impact on the American astronomical community, to lose 1157 03:10:34.570 --> 03:10:40.860 John Gizis: that potential science case, where presumably Roman can't observe U and G, so it was really adding something to the… 1158 03:10:41.030 --> 03:10:53.300 John Gizis: How will the SCOC, I don't think it's a question for David, address, you know, those sorts of concerns? What the views of other, communities that aren't necessarily LSST-centric? 1159 03:10:53.410 --> 03:10:56.420 John Gizis: dude. 1160 03:10:56.760 --> 03:10:59.819 John Gizis: So it's a question to raise a big issue, I guess. 1161 03:11:03.650 --> 03:11:05.100 Lynne Jones: So… 1162 03:11:05.860 --> 03:11:16.829 Lynne Jones: I don't think this is a question for me to answer, as I'm a ex-officio member of the SEOC. However, Fed is not actually, with us today, unfortunately, due to personal information. 1163 03:11:16.830 --> 03:11:20.539 Zeljko: in Ubers, so there may be too much background noise, I apologize. 1164 03:11:20.850 --> 03:11:21.360 Lynne Jones: There we go. 1165 03:11:21.360 --> 03:11:28.939 Zeljko: But, as Lynn said, we want SEOC to focus on scientific impact and cadence change. 1166 03:11:29.430 --> 03:11:37.070 Zeljko: And other aspects of this proposal will be considered elsewhere. There are, of course, many other aspects to it. 1167 03:11:37.520 --> 03:11:50.960 Zeljko: SCOC is in the best position to assess what would be impacts on MSSD science cases if we followed the strategy that we already simulated in response to this. 1168 03:11:51.770 --> 03:11:55.029 Zeljko: That is the main goal for this committee. 1169 03:11:55.310 --> 03:12:00.599 Zeljko: Those other aspects that are valid and that we need to consider, they will be addressed elsewhere. 1170 03:12:01.330 --> 03:12:04.299 John Gizis: Yeah, so overlap with external, 1171 03:12:04.780 --> 03:12:10.939 John Gizis: surveys is out of bounds, but a purely LSST consideration of the impact. 1172 03:12:11.420 --> 03:12:12.440 John Gizis: Is… Right. 1173 03:12:12.590 --> 03:12:15.679 John Gizis: That's very helpful for us to understand. Thank you so much. 1174 03:12:16.750 --> 03:12:18.540 Zeljko: Okay, sorry for the noise. 1175 03:12:21.570 --> 03:12:30.640 Lynne Jones: I think it is… it is certainly a goal in general of the SELC to consider as many aspects as possible of 1176 03:12:30.750 --> 03:12:37.360 Lynne Jones: of survey strategy changes as they come up. There is always, of course, the limitation that, 1177 03:12:38.700 --> 03:12:50.830 Lynne Jones: our knowledge within the project and our knowledge from… coming from the science collaborations will be imperfect. And so, if this comes up through the science collaborations, that they say, oh, you know, one of the… 1178 03:12:50.830 --> 03:13:02.140 Lynne Jones: things that I'm now concerned about is, like, how LSST survey coverage is… is going to impact my other science. It's true, that's a little bit, 1179 03:13:03.790 --> 03:13:16.390 Lynne Jones: It's a bit of a question that's, like, out of bounds for what the LSSD is, because the priority of the SEOC has to remain, the LSSD science, but it certainly is something that they can… can think about. 1180 03:13:16.970 --> 03:13:20.720 Lynne Jones: Nobody's going to say that you… they couldn't consider something. 1181 03:13:23.070 --> 03:13:27.340 Lynne Jones: But yeah, it… there are always… 1182 03:13:27.770 --> 03:13:33.850 Lynne Jones: There are always, unfortunately, things that we're gonna miss, of course, but… 1183 03:13:34.150 --> 03:13:38.359 Lynne Jones: at the end of the day, we are here to try to make the best LSST. 1184 03:13:39.000 --> 03:13:42.180 Lynne Jones: And, let's see. 1185 03:13:43.470 --> 03:13:59.600 Lynne Jones: We have… we do have some more time here for questions. We can talk about, Desi, and we can talk about other questions from other… other parts of the… the session. I do want to make sure, if we have things we didn't want to circle back to from the rest of the… 1186 03:14:00.030 --> 03:14:05.810 Lynne Jones: the workshop, that we… that we cover those as well. But… so damn. 1187 03:14:07.890 --> 03:14:11.130 Dan Taranu: Yeah, sorry, I had a lingering question from before, and I… 1188 03:14:11.430 --> 03:14:15.569 Dan Taranu: Missed the discussion about the DDFs earlier, but looked at… looked at the slides. 1189 03:14:18.210 --> 03:14:36.439 Dan Taranu: Do you have a lot of metrics for specifically optimizing the radial dithering in the… or translational dithers in the DDFs? Is it basically trading off the area that gets full coverage versus the larger area that might get less coverage on the outer skirts, and… 1190 03:14:37.100 --> 03:14:43.630 Dan Taranu: Does that one failed detector that's very near the edge of the focal plane, but not quite, does that change things at all, or… 1191 03:14:44.610 --> 03:14:51.890 Lynne Jones: Okay, so this is… This is a good question that touches along a lot of, 1192 03:14:52.000 --> 03:14:55.619 Lynne Jones: On a particular math aspect as well. 1193 03:14:55.850 --> 03:14:59.409 Lynne Jones: With math, what we do is, 1194 03:15:00.550 --> 03:15:04.880 Lynne Jones: We do imprint the camera footprint when we're calculating our metrics. 1195 03:15:05.000 --> 03:15:09.540 Lynne Jones: We don't necessarily have the resolution to really say this is the… 1196 03:15:10.420 --> 03:15:21.119 Lynne Jones: We don't usually run our metrics at super high resolution, so we don't… we represent the chip gap statistically, but not necessarily exactly, for example. 1197 03:15:21.120 --> 03:15:34.770 Lynne Jones: That said, we should take our camera footprint and take out the… because we do have the chip gaps in our camera footprint. We haven't taken out the missing detector, and we should do that, and that's a very good point. 1198 03:15:34.820 --> 03:15:39.160 Lynne Jones: So I don't know if the missing detector makes a difference or not. 1199 03:15:39.320 --> 03:15:49.559 Lynne Jones: The metrics we have for the deep drilling fields and the dithering really do just, as you say, look at the trades between as you get wider. 1200 03:15:49.640 --> 03:16:03.390 Lynne Jones: bigger dithers, you decrease the cadence, so we do have things that are looking at, like, what is the… essentially, what is the cadence within the deep drilling fields, and you do, decrease the coated depth. 1201 03:16:03.480 --> 03:16:13.849 Lynne Jones: Because you're spreading that over more area. I don't know specifically we look at, like, what happens with the roll-off, but as you… towards the edges of the dinner, but we, 1202 03:16:14.540 --> 03:16:23.100 Lynne Jones: We definitely… that is the primary driver for having smaller jitters, is you get a better cadence, and you get deeper depths. 1203 03:16:25.570 --> 03:16:26.970 Lynne Jones: That's a problem. 1204 03:16:27.400 --> 03:16:51.980 Saurabh Jha: Yeah, just to follow up on that, so yeah, it's true that the metrics don't always capture that for the DDFs, but this is something we put in the DDF task force of the SCOC we posed to the science collaborations, and basically, you know, you can imagine you have this umbra of the DDF, and then you have this penumbra, which gets bigger the more you dither, and you could imagine some science cases would like, you know, basically you're making your effective area of a deep drilling field just bigger. 1205 03:16:51.980 --> 03:17:01.210 Saurabh Jha: But it turns out, in terms of, like, external synergies for the DDFs and, like, you know, space-based imaging and stuff, that the Rubin footprint is already big. 1206 03:17:01.210 --> 03:17:22.599 Saurabh Jha: Right? Compared to the size of these fields. And so, increasing that area was not generally a science win across the board for the science collaborations. And so, from the science collaborations point of view, keeping that as small as possible, like maybe just dithering over chip gaps, that would be the ideal. And then that would improve the cadence, just as Lynn said, and get the highest co-added depth. 1207 03:17:22.600 --> 03:17:29.029 Saurabh Jha: So basically, the dithering we would want to do with EDFs is as little as possible that DM says is okay. 1208 03:17:33.650 --> 03:17:46.570 Lynne Jones: And it does seem like we've, moved on to other questions, so I'm gonna make sure we thank all of the DESI people for joining us. Of course, like, please stay on so that in case we come back to more DESI questions, but thank you for… 1209 03:17:47.030 --> 03:17:49.589 Lynne Jones: For your presentation and joining us. 1210 03:17:49.690 --> 03:17:51.920 Lynne Jones: Neal? 1211 03:17:53.570 --> 03:18:09.800 William Nielsen Brandt: Yeah, sorry, I just did want to ask one other just point of clarification, just to be sure I didn't miss something along the way. So, if the DESE plan were implemented, what would you anticipate the effects upon the deep drilling fields, if anything, material, to be? 1212 03:18:09.960 --> 03:18:18.960 William Nielsen Brandt: I presume, we would still maintain truly excellent time domain coverage in any of the deep drilling fields that are also in that footprint. 1213 03:18:19.220 --> 03:18:25.959 William Nielsen Brandt: That would… that's obviously very important, and it's key to the nature of the deep drilling field, you know, in terms of the U and G bands. 1214 03:18:26.170 --> 03:18:31.440 William Nielsen Brandt: But are there other effects you could anticipate there that we should be thinking about? 1215 03:18:32.630 --> 03:18:35.750 Lynne Jones: I have. 1216 03:18:35.750 --> 03:18:49.980 David Schlegel: Let me jump in for a sec. I mean, I don't see why this would affect Ruben at all, but we do have the opportunity on the DESI side. We don't have any other cadencing requirements or anything like that, so if, you know, if the request 1217 03:18:50.380 --> 03:18:59.299 David Schlegel: for this data exchange from DESE said, hey, you know, we really want to do the DESI follow-up on the following days, or, you know, just 1218 03:18:59.460 --> 03:19:07.069 David Schlegel: you know, more of a triggered response, you know, we could do that, so that… I think we'd certainly see that on the DESE side. 1219 03:19:08.060 --> 03:19:12.360 William Nielsen Brandt: Thanks. Yes, I'm mostly interested in the Rubin side here. 1220 03:19:12.740 --> 03:19:16.369 William Nielsen Brandt: So, Lynn, did you have any insights there? I mean. 1221 03:19:17.120 --> 03:19:31.950 Lynne Jones: So it's true, I haven't specifically looked to see in the Desi Sims, did we change the deep drilling coverage? However, I would guess we did not, and so Rob is shaking his head. 1222 03:19:31.950 --> 03:19:39.460 Lynne Jones: Because of the fact that, the deep drilling fields are programmed separately, and they're in a higher tier, so they should… 1223 03:19:39.710 --> 03:19:49.050 Lynne Jones: continue as, as previously planned, and we didn't, like, decrease the DDF coverage because we were getting this other coverage as well. 1224 03:19:50.550 --> 03:19:51.250 Lynne Jones: That's wrong? 1225 03:19:51.250 --> 03:19:51.930 William Nielsen Brandt: Okay. 1226 03:19:53.330 --> 03:20:01.560 Saurabh Jha: Yeah, I was gonna say the same thing, that the DFs are not affected. It's really the WFD visits in that northern part of the sky that get shipped. 1227 03:20:01.790 --> 03:20:06.979 William Nielsen Brandt: Very good. I just wanted to be sure there wasn't some second-order effect that I wasn't appreciating, but thank you. Okay. 1228 03:20:08.010 --> 03:20:17.150 Lynne Jones: No, in fact, it's usually the other way around, that the DDFs affect the coverage of the rest of the sky, because they are in this higher priority tier. 1229 03:20:17.460 --> 03:20:29.790 Lynne Jones: And this was, for example, one of the reasons we had to move the ultra-deep season of EDFS out of year one, because we were already a little stretched thin in that part of the sky. 1230 03:20:29.990 --> 03:20:39.310 Lynne Jones: And so… and with, like, assuming a higher fault rate and lower efficiency at the start of the survey, it made things a little bit too tight. 1231 03:20:39.870 --> 03:20:48.920 Lynne Jones: So… Yeah, the deep drilling fields are… Or… Very strongly, 1232 03:20:49.650 --> 03:20:52.280 Lynne Jones: defined, I guess, is one way to put it. 1233 03:20:53.030 --> 03:20:59.489 Lynne Jones: All right, do we have other questions? We have about… 10 more minutes. 1234 03:20:59.990 --> 03:21:01.060 Lynne Jones: Yeah, Rachel. 1235 03:21:02.840 --> 03:21:05.250 Rachel Mandelbaum: Yeah, so this is a question for… 1236 03:21:05.370 --> 03:21:15.650 Rachel Mandelbaum: Rubin Leadership, so looking at who's on the call, maybe Phil or Jelco? So… For the, 1237 03:21:16.130 --> 03:21:28.929 Rachel Mandelbaum: Does the observing time that would come out of this exchange? Like, does Rubin leadership have an idea for a model for how to allocate that to maximize the benefit to the Rubin community? 1238 03:21:32.290 --> 03:21:37.550 Phil Marshall (SLAC/Rubin): I would say… Not yet, but we have some… 1239 03:21:37.780 --> 03:21:40.239 Phil Marshall (SLAC/Rubin): I've already done some thinking about, 1240 03:21:41.160 --> 03:21:47.399 Phil Marshall (SLAC/Rubin): other in-kind contributions of telescope time and so on. So… 1241 03:21:47.710 --> 03:21:56.119 Phil Marshall (SLAC/Rubin): we would look at what we've done there with the, you know, contributions from Subaru and other places, and think about whether we could 1242 03:21:56.270 --> 03:22:05.479 Phil Marshall (SLAC/Rubin): treat this, you know, the DESI time or the DESI data in a similar way. I mean, we're trying to be… 1243 03:22:06.400 --> 03:22:19.159 Phil Marshall (SLAC/Rubin): even-handed in our support of the RSST science community, and YLAB has, you know, open skies policies that we're trying to observe as well. So, we would try and make sure that the… 1244 03:22:19.390 --> 03:22:23.729 Phil Marshall (SLAC/Rubin): that the benefits of any data exchange with DESI were… were shared around. 1245 03:22:25.680 --> 03:22:32.399 Phil Marshall (SLAC/Rubin): it may well be that some parts of the RSSD science community would benefit more from this than others. 1246 03:22:32.530 --> 03:22:34.660 Phil Marshall (SLAC/Rubin): and… You know, we would… 1247 03:22:34.820 --> 03:22:46.539 Phil Marshall (SLAC/Rubin): we would try and take that into account as well, but, I mean, there would… there would be something significant to work out here in terms of how best to use these data. I mean, the… 1248 03:22:46.740 --> 03:22:50.600 Phil Marshall (SLAC/Rubin): I think… I suppose there's some hope that, 1249 03:22:51.390 --> 03:23:11.149 Phil Marshall (SLAC/Rubin): that there could be simple ways, and I think David was highlighting these in his slides, simple ways for… for using DESI spectra, kind of synoptically, similar to the LSST survey itself, so looking for applications that already serve multiple science cases, and PhotoZ training is one of those, for example. 1250 03:23:12.810 --> 03:23:30.839 Nathalie Palanque-Delabrouille: Yeah, so I'm just reiterating what David showed, but with just a one-slight summary of topics that we've discussed for collaboration between DESI, Spectra, and LSST, and in the deep billing fields in particular, we can really contribute to the DSST science, the Rubin science. 1251 03:23:30.840 --> 03:23:35.040 Nathalie Palanque-Delabrouille: By providing the spectra of live transients, or a supernovae host. 1252 03:23:35.040 --> 03:24:00.030 Nathalie Palanque-Delabrouille: And for the weak lensing science, we can also significantly support that science by providing the very deep spectra for, photocalibration. We've, tested, up to a few hours, but we've shown that with the instrumentation upgrade that we're planning for this second phase of DESI, we could actually, stack up to 80 1253 03:24:00.030 --> 03:24:04.040 Nathalie Palanque-Delabrouille: hours of Spectra, and so that would really provide very deep, 1254 03:24:04.040 --> 03:24:21.400 Nathalie Palanque-Delabrouille: spectra for calibration of photos Zs, and so this is an example of what we've been discussing so far, but of course, this is not set in stone, and we can definitely continue to identify what would be the best, outcome of this data exchange. 1255 03:24:23.920 --> 03:24:24.890 Phil Marshall (SLAC/Rubin): Thanks, Natalie. 1256 03:24:39.940 --> 03:24:40.600 Lynne Jones: Wow. 1257 03:24:41.180 --> 03:24:45.409 Lynne Jones: I think we've, we've… Covered a lot, and we've had a lot to think about. 1258 03:24:45.630 --> 03:24:48.520 Lynne Jones: I don't see any more questions or hands coming up. 1259 03:24:49.120 --> 03:24:50.180 Lynne Jones: So… 1260 03:24:50.390 --> 03:24:56.609 Lynne Jones: I'm going to say thank you all very much for coming and sharing and, talking with us today. 1261 03:24:57.170 --> 03:25:12.679 Lynne Jones: And all of the… all of you community members and all of the SCOC members, thank you, as well. It's been, a lot to go through and to talk about, and I hope we all have some good ideas of how the survey will start. 1262 03:25:13.180 --> 03:25:21.790 Lynne Jones: What we're doing in terms of the strategy, and where we might be going for the next year or two, as well as over the 10 years of the survey. 1263 03:25:23.730 --> 03:25:33.620 Lynne Jones: you know what, I think we can be done. We can have a few minutes back out of your day, and thank you all for coming. We do have Monday coming up, and, I'm… 1264 03:25:34.250 --> 03:25:45.920 Lynne Jones: hoping that Fed will be back to, help us coordinate for that, but otherwise, we'll be reaching out to the science collaborations to organize feedback. Monday is a little bit more for 1265 03:25:46.180 --> 03:25:50.619 Lynne Jones: feedback from you in the science collaborations to the SEOC. 1266 03:25:51.870 --> 03:25:53.410 Lynne Jones: So, thanks very much. 1267 03:25:53.530 --> 03:25:55.910 Lynne Jones: We'll talk to you on Monday. 1268 03:25:58.240 --> 03:25:58.970 Phil Marshall (SLAC/Rubin): Excellent.