1 00:00:01,350 --> 00:00:15,190 [Music] 2 00:00:21,470 --> 00:00:19,880 how about now okay okay so thanks 3 00:00:27,980 --> 00:00:21,480 everyone for staying for the last few 4 00:00:29,560 --> 00:00:27,990 talks of the session I'm Bea I'll be 5 00:00:32,269 --> 00:00:29,570 talking to you guys today about 6 00:00:35,840 --> 00:00:32,279 polarimetry it's one cool trick that has 7 00:00:37,729 --> 00:00:35,850 moms everywhere mad and it's really not 8 00:00:39,049 --> 00:00:37,739 used as much as it should be it's 9 00:00:41,720 --> 00:00:39,059 probably something that you heard about 10 00:00:43,850 --> 00:00:41,730 while you were an undergraduate and have 11 00:00:45,140 --> 00:00:43,860 since completely forgotten about because 12 00:00:46,360 --> 00:00:45,150 most of us aren't using it in our 13 00:00:49,250 --> 00:00:46,370 research 14 00:00:52,100 --> 00:00:49,260 the idea with polarimetry is really just 15 00:00:55,880 --> 00:00:52,110 that instead of thinking of life as just 16 00:00:57,320 --> 00:00:55,890 a scalar with intensity and wavelength 17 00:00:59,780 --> 00:00:57,330 information that you think of it as a 18 00:01:01,250 --> 00:00:59,790 vector so you still have that scalar 19 00:01:04,850 --> 00:01:01,260 information but you also have 20 00:01:06,770 --> 00:01:04,860 information about your electric field 21 00:01:09,320 --> 00:01:06,780 oscillation so it's your electromagnetic 22 00:01:11,240 --> 00:01:09,330 wave having an electric field on 23 00:01:14,539 --> 00:01:11,250 oscillates up and down side aside in a 24 00:01:21,889 --> 00:01:14,549 corkscrew Plus polarimetry in terms of 25 00:01:25,069 --> 00:01:21,899 observing a planet in terms of observing 26 00:01:28,060 --> 00:01:25,079 a planet what we are going to have at 27 00:01:30,800 --> 00:01:28,070 least in an ideal case with a nice calm 28 00:01:32,630 --> 00:01:30,810 main-sequence star it's unpolarized 29 00:01:33,889 --> 00:01:32,640 incident light coming from my star and 30 00:01:37,120 --> 00:01:33,899 that's going to be scattering off a 31 00:01:39,289 --> 00:01:37,130 surface or off of an atmosphere and that 32 00:01:41,959 --> 00:01:39,299 scattering or reflection is going to 33 00:01:44,630 --> 00:01:41,969 impart a trend in the way that the 34 00:01:46,130 --> 00:01:44,640 electric field oscillates and so it's 35 00:01:49,219 --> 00:01:46,140 going to give us great contrast with our 36 00:01:51,499 --> 00:01:49,229 stars in those cases I'm talking mostly 37 00:01:54,050 --> 00:01:51,509 about habitability today but I wanted to 38 00:01:56,230 --> 00:01:54,060 touch on these other things that 39 00:01:58,370 --> 00:01:56,240 polarimetry has contributed to 40 00:02:02,779 --> 00:01:58,380 polarimetry has allowed us to constrain 41 00:02:05,359 --> 00:02:02,789 albedo of ht1 8-9 7:33 be the original 42 00:02:07,760 --> 00:02:05,369 claim detection of polarized light from 43 00:02:09,919 --> 00:02:07,770 that planet is disputed but those non 44 00:02:11,960 --> 00:02:09,929 detection that dispute that have given 45 00:02:14,650 --> 00:02:11,970 us some physical constraints on the 46 00:02:17,870 --> 00:02:14,660 nature of the planet more recently 47 00:02:20,240 --> 00:02:17,880 observations in polarized light of the 48 00:02:23,059 --> 00:02:20,250 other ha Jupiter I have up there wasp 49 00:02:26,300 --> 00:02:23,069 18b have allowed us to exclude certain 50 00:02:28,280 --> 00:02:26,310 scenarios Venus of course was famously 51 00:02:29,839 --> 00:02:28,290 observed and polarized like many times 52 00:02:32,690 --> 00:02:29,849 and that allowed us to determine what 53 00:02:35,569 --> 00:02:32,700 the cloud species was dominant in that 54 00:02:38,929 --> 00:02:35,579 atmosphere that that was not a nice 55 00:02:41,270 --> 00:02:38,939 jungle planet right next door to us in 56 00:02:43,640 --> 00:02:41,280 the case of Titan polarimetry was used 57 00:02:45,979 --> 00:02:43,650 to give us the first indication that 58 00:02:48,110 --> 00:02:45,989 this was a cloudy hazy world and that 59 00:02:51,020 --> 00:02:48,120 unusual photometry that we saw from that 60 00:02:53,030 --> 00:02:51,030 was not because we had snow all over the 61 00:02:54,860 --> 00:02:53,040 surface that's a really interesting 62 00:02:58,069 --> 00:02:54,870 paper by the way if you look it up 63 00:03:01,129 --> 00:02:58,079 Illinois 1973 very recently we've had 64 00:03:03,649 --> 00:03:01,139 observations of solar oblate notes from 65 00:03:05,360 --> 00:03:03,659 rapidly rotating stars even seeing stars 66 00:03:07,849 --> 00:03:05,370 reflecting each other's light in 67 00:03:09,470 --> 00:03:07,859 polarized light and we've had a lot of 68 00:03:11,780 --> 00:03:09,480 characterization of the interstellar 69 00:03:15,440 --> 00:03:11,790 medium which is a really vital component 70 00:03:16,640 --> 00:03:15,450 to studies of exoplanets the polarized 71 00:03:17,509 --> 00:03:16,650 light that's something that we need to 72 00:03:30,110 --> 00:03:17,519 take into account 73 00:03:33,920 --> 00:03:30,120 oh is it thanks okay that sounds better 74 00:03:36,649 --> 00:03:33,930 yeah all right so as we have a planet 75 00:03:39,080 --> 00:03:36,659 that's moving through its phases around 76 00:03:40,969 --> 00:03:39,090 its star we're going to see these key 77 00:03:43,099 --> 00:03:40,979 features come up in polarized light 78 00:03:46,369 --> 00:03:43,109 coming from glint off an ocean if it has 79 00:03:47,719 --> 00:03:46,379 a rainbow from other optical effects 80 00:03:50,330 --> 00:03:47,729 from clouds and from Rayleigh scattering 81 00:03:51,890 --> 00:03:50,340 and depending out what wavelengths are 82 00:03:53,899 --> 00:03:51,900 looking at different features we'll be 83 00:03:55,550 --> 00:03:53,909 dominant so that allows us to 84 00:03:57,860 --> 00:03:55,560 characterize the exoplanets around their 85 00:03:59,629 --> 00:03:57,870 star there's also some stuff that you 86 00:04:01,369 --> 00:03:59,639 can do as far as bio signatures looking 87 00:04:02,809 --> 00:04:01,379 for chiral molecules so I'm not really 88 00:04:04,490 --> 00:04:02,819 going to talk about that today but I 89 00:04:07,670 --> 00:04:04,500 just wanted to leave it up to remind 90 00:04:09,500 --> 00:04:07,680 people to look it up so one of the 91 00:04:11,479 --> 00:04:09,510 strengths of this as I have touched on 92 00:04:13,670 --> 00:04:11,489 before is that you can naturally know 93 00:04:15,559 --> 00:04:13,680 that star if it's a calm star you're 94 00:04:17,629 --> 00:04:15,569 going to create natural contrast with it 95 00:04:20,420 --> 00:04:17,639 so you don't necessarily need to use 96 00:04:21,830 --> 00:04:20,430 something like a coronagraph you don't 97 00:04:23,390 --> 00:04:21,840 necessarily need your planet to be 98 00:04:25,640 --> 00:04:23,400 transiting the star for you to be able 99 00:04:27,650 --> 00:04:25,650 to characterize it 100 00:04:29,960 --> 00:04:27,660 another benefit is that you can derive 101 00:04:32,360 --> 00:04:29,970 orbital parameters even for planets that 102 00:04:34,640 --> 00:04:32,370 do not transit there start your 103 00:04:37,040 --> 00:04:34,650 inclination is going to change the shape 104 00:04:38,330 --> 00:04:37,050 of your polarized light curve not just 105 00:04:39,800 --> 00:04:38,340 the intensity but the shape of your 106 00:04:43,310 --> 00:04:39,810 polarized light curve so that can be 107 00:04:46,129 --> 00:04:43,320 figured out using this method polarized 108 00:04:47,570 --> 00:04:46,139 light really lends itself to confirming 109 00:04:49,520 --> 00:04:47,580 the presence of clouds as well and 110 00:04:52,100 --> 00:04:49,530 possibly to characterizing them if you 111 00:04:54,170 --> 00:04:52,110 can get enough data for that so I'm 112 00:04:57,250 --> 00:04:54,180 going to show you a few models most of 113 00:04:59,810 --> 00:04:57,260 these models are going to be based on 114 00:05:02,540 --> 00:04:59,820 chemically evolved models from and 115 00:05:04,159 --> 00:05:02,550 ruling house keys 2018 papers so he was 116 00:05:06,680 --> 00:05:04,169 looking at the Trappist one system and 117 00:05:10,580 --> 00:05:06,690 the kind of archetype planets that we 118 00:05:11,689 --> 00:05:10,590 might find there so in these graphs that 119 00:05:13,580 --> 00:05:11,699 I'm going to show you in a little bit 120 00:05:15,230 --> 00:05:13,590 we're going to be taking a few of these 121 00:05:15,680 --> 00:05:15,240 archetypes and comparing them to each 122 00:05:18,080 --> 00:05:15,690 other 123 00:05:19,700 --> 00:05:18,090 maybe including things like varying 124 00:05:21,560 --> 00:05:19,710 types of clouds and adding cloud cases 125 00:05:24,230 --> 00:05:21,570 we're not going to talk about services 126 00:05:27,230 --> 00:05:24,240 in too much detail but the question was 127 00:05:28,879 --> 00:05:27,240 if we have this information from the 128 00:05:30,770 --> 00:05:28,889 scalar components things like the albedo 129 00:05:34,760 --> 00:05:30,780 of these different surfaces and the 130 00:05:37,159 --> 00:05:34,770 behavior in scalar light of atmospheres 131 00:05:38,900 --> 00:05:37,169 and of different types of clouds what 132 00:05:41,420 --> 00:05:38,910 more can we know by looking at this in 133 00:05:43,640 --> 00:05:41,430 polarized light so we have that for 134 00:05:46,100 --> 00:05:43,650 comparison in scalar light we also have 135 00:05:47,990 --> 00:05:46,110 very different behavior of surfaces in 136 00:05:49,779 --> 00:05:48,000 polarized light different surfaces 137 00:05:53,360 --> 00:05:49,789 polarized light in different ways and 138 00:05:55,640 --> 00:05:53,370 even different types of ices can 139 00:05:57,350 --> 00:05:55,650 polarize light in slightly different 140 00:06:00,650 --> 00:05:57,360 ways which could be vital in the far 141 00:06:03,230 --> 00:06:00,660 future for characterizing some types of 142 00:06:04,820 --> 00:06:03,240 exoplanets but is immediately useful for 143 00:06:08,659 --> 00:06:04,830 characterizing the icy moons in our own 144 00:06:11,270 --> 00:06:08,669 solar system for the plots I'm about to 145 00:06:13,969 --> 00:06:11,280 show you this is just a dummy plot I 146 00:06:15,860 --> 00:06:13,979 just wanted to point out that the x-axis 147 00:06:17,420 --> 00:06:15,870 it's typically going to be just half of 148 00:06:20,779 --> 00:06:17,430 an orbit so we're going from full phase 149 00:06:22,490 --> 00:06:20,789 to new phase the y-axis is polarization 150 00:06:23,930 --> 00:06:22,500 and parts per million so that's telling 151 00:06:25,939 --> 00:06:23,940 us the size of the signal current 152 00:06:30,379 --> 00:06:25,949 polarimeters are sensitive to about one 153 00:06:32,930 --> 00:06:30,389 part per million and then at the top 154 00:06:34,399 --> 00:06:32,940 I've merged some small end with the 155 00:06:37,130 --> 00:06:34,409 dashed lines I've merged some key 156 00:06:38,590 --> 00:06:37,140 features to look for I just want to 157 00:06:42,070 --> 00:06:38,600 point out that the 158 00:06:43,620 --> 00:06:42,080 maximum polarization is not necessarily 159 00:06:45,430 --> 00:06:43,630 the same as where we find the maximum 160 00:06:47,980 --> 00:06:45,440 signal we need to combine the 161 00:06:48,730 --> 00:06:47,990 polarization in some cases with the 162 00:06:50,650 --> 00:06:48,740 amount of light that we're getting 163 00:06:52,120 --> 00:06:50,660 reflected off the planet and if we're 164 00:06:54,070 --> 00:06:52,130 looking at a rainbow that that might 165 00:06:55,090 --> 00:06:54,080 shift depending on the species producing 166 00:06:58,300 --> 00:06:55,100 the rainbow and the wavelength that 167 00:07:00,340 --> 00:06:58,310 we're looking at so our first point to 168 00:07:04,240 --> 00:07:00,350 examine here with one of the tracklist 169 00:07:05,980 --> 00:07:04,250 cases is that polarizing features have 170 00:07:07,780 --> 00:07:05,990 distinct shapes and of course their 171 00:07:08,800 --> 00:07:07,790 dominance varies with wavelength as you 172 00:07:10,660 --> 00:07:08,810 might expect the Rayleigh scattering 173 00:07:13,060 --> 00:07:10,670 will be very strong if you're looking at 174 00:07:14,830 --> 00:07:13,070 blue wavelengths and if you can start 175 00:07:17,200 --> 00:07:14,840 moving towards redder wavelengths if you 176 00:07:18,940 --> 00:07:17,210 had a planet that had ocean glint that 177 00:07:21,700 --> 00:07:18,950 would be a strong polarizing feature and 178 00:07:24,850 --> 00:07:21,710 that would start to pop out as you look 179 00:07:28,360 --> 00:07:24,860 towards redder and redder wavelengths if 180 00:07:30,490 --> 00:07:28,370 we have a planet that has a cloud 181 00:07:32,260 --> 00:07:30,500 present we get these a very distinct 182 00:07:35,230 --> 00:07:32,270 rainbow features these are very clear 183 00:07:38,500 --> 00:07:35,240 features to see in polarized light the 184 00:07:39,670 --> 00:07:38,510 strength of the rainbow compared to the 185 00:07:42,220 --> 00:07:39,680 other features like the Rayleigh 186 00:07:45,730 --> 00:07:42,230 scattering will depend on the cloud 187 00:07:47,560 --> 00:07:45,740 height if you're very interested in how 188 00:07:48,940 --> 00:07:47,570 to determine your cloud height and kind 189 00:07:50,770 --> 00:07:48,950 of disentangle that from molecular 190 00:07:53,920 --> 00:07:50,780 abundances I would highly recommend 191 00:07:58,990 --> 00:07:53,930 looking at the paper from Thomas Boucher 192 00:08:00,460 --> 00:07:59,000 Oh tomorrow she I'm sorry from 2017 it's 193 00:08:06,700 --> 00:08:00,470 a really brilliant paper but I can't get 194 00:08:08,740 --> 00:08:06,710 into that right now right and so even in 195 00:08:11,590 --> 00:08:08,750 cases like this where we have an 196 00:08:13,780 --> 00:08:11,600 atmosphere that is maybe very strongly 197 00:08:17,350 --> 00:08:13,790 really scattering and we're masking that 198 00:08:19,750 --> 00:08:17,360 a weaker rainbow signal from a different 199 00:08:23,050 --> 00:08:19,760 species in the cloud if we're moving 200 00:08:25,510 --> 00:08:23,060 towards red wavelengths we're starting 201 00:08:28,030 --> 00:08:25,520 to be able to pick out the difference in 202 00:08:33,130 --> 00:08:28,040 those curves the one that has the cloud 203 00:08:34,540 --> 00:08:33,140 present the one that does not so 204 00:08:36,100 --> 00:08:34,550 different scenarios of cloudy 205 00:08:38,110 --> 00:08:36,110 atmospheres do you seem to be 206 00:08:40,480 --> 00:08:38,120 distinguishable just looking at these 207 00:08:43,870 --> 00:08:40,490 different Trappist archetypes you can 208 00:08:45,310 --> 00:08:43,880 tell them apart from one another and of 209 00:08:48,460 --> 00:08:45,320 course they're going to change in 210 00:08:51,550 --> 00:08:48,470 wavelength in particular and predictable 211 00:08:52,150 --> 00:08:51,560 ways so this is suggesting that this 212 00:08:54,280 --> 00:08:52,160 might be 213 00:08:56,590 --> 00:08:54,290 useful technique to tell different kind 214 00:09:00,790 --> 00:08:56,600 of basic anticipated planet archetypes 215 00:09:02,199 --> 00:09:00,800 apart and I should point out that I'm 216 00:09:04,499 --> 00:09:02,209 kind of simplifying things here I'm 217 00:09:06,699 --> 00:09:04,509 showing you the total polarization in 218 00:09:08,170 --> 00:09:06,709 reality we're normally looking at Stokes 219 00:09:10,780 --> 00:09:08,180 parameters we have a little bit more 220 00:09:12,280 --> 00:09:10,790 information than the last few plots that 221 00:09:14,110 --> 00:09:12,290 I've shown you so we're looking at 222 00:09:15,970 --> 00:09:14,120 Stokes Q and U and we're getting 223 00:09:18,689 --> 00:09:15,980 positive and negative values that also 224 00:09:22,379 --> 00:09:18,699 behave in particular ways depending on 225 00:09:24,519 --> 00:09:22,389 your rainbow behavior and your 226 00:09:27,879 --> 00:09:24,529 scattering surface if you're looking at 227 00:09:30,340 --> 00:09:27,889 a surface if the values on the y-axis 228 00:09:33,280 --> 00:09:30,350 have been wearing you after I told you 229 00:09:35,619 --> 00:09:33,290 we can currently detect on to around one 230 00:09:37,689 --> 00:09:35,629 part per million you might consider 231 00:09:43,240 --> 00:09:37,699 looking at sub Neptune's mini Neptune's 232 00:09:45,220 --> 00:09:43,250 so GJ 1214b depending on its cub specie 233 00:09:47,800 --> 00:09:45,230 is dominant in the upper atmosphere and 234 00:09:50,559 --> 00:09:47,810 the size of the particles can produce 235 00:09:53,100 --> 00:09:50,569 optical effects that would be near 236 00:09:56,710 --> 00:09:53,110 current detection limits with 237 00:09:58,720 --> 00:09:56,720 contemporary polarimeters so we're 238 00:10:02,850 --> 00:09:58,730 getting very close to that one part per 239 00:10:10,120 --> 00:10:07,800 so with a part per million precision 240 00:10:12,460 --> 00:10:10,130 polarimeter which is what we currently 241 00:10:14,550 --> 00:10:12,470 have and several hours of observation 242 00:10:18,490 --> 00:10:14,560 which is pretty typical of an aperture 243 00:10:19,900 --> 00:10:18,500 polarimeter observing these days if we 244 00:10:21,699 --> 00:10:19,910 were looking for one of these one 245 00:10:25,269 --> 00:10:21,709 designed part per million signals from a 246 00:10:27,340 --> 00:10:25,279 planet we could do that currently just 247 00:10:28,870 --> 00:10:27,350 with what we have right now with a 248 00:10:30,490 --> 00:10:28,880 4-metre class telescopes if we're 249 00:10:32,620 --> 00:10:30,500 looking at a star like HD one eight nine 250 00:10:35,230 --> 00:10:32,630 if we're looking at a star like Proxima 251 00:10:37,689 --> 00:10:35,240 Sun and our band we would want to use an 252 00:10:39,429 --> 00:10:37,699 eight meter telescope Proxima Sun and B 253 00:10:41,530 --> 00:10:39,439 band if we want to get some comparison 254 00:10:43,299 --> 00:10:41,540 in the different wavelengths and start 255 00:10:45,819 --> 00:10:43,309 to tell these features more clearly 256 00:10:48,009 --> 00:10:45,829 apart we would need to use a thirty 257 00:10:50,319 --> 00:10:48,019 meter telescope so basically right now 258 00:10:53,619 --> 00:10:50,329 if there was a hot mini Neptune in 259 00:10:55,389 --> 00:10:53,629 Proximus then or something larger and 260 00:10:57,100 --> 00:10:55,399 hotter than that we should be able to 261 00:11:01,299 --> 00:10:57,110 detect it or almost be able to detect it 262 00:11:03,970 --> 00:11:01,309 with a dedicated program if we wanted to 263 00:11:05,710 --> 00:11:03,980 observe a dimmer star of course we just 264 00:11:07,809 --> 00:11:05,720 need to stare longer use them even 265 00:11:10,179 --> 00:11:07,819 bigger telescope if we want to be 266 00:11:11,980 --> 00:11:10,189 looking for planets in polarized light 267 00:11:14,410 --> 00:11:11,990 that are in the habitable zone this 268 00:11:16,269 --> 00:11:14,420 would improve or this would require that 269 00:11:19,840 --> 00:11:16,279 we improve our polarimeter design to 270 00:11:22,629 --> 00:11:19,850 some degree so I tend to kind of 271 00:11:25,110 --> 00:11:22,639 summarize polarimetry by saying that 272 00:11:28,360 --> 00:11:25,120 although the nature of polarimetry 273 00:11:31,179 --> 00:11:28,370 reduces the throughput of your photons 274 00:11:33,429 --> 00:11:31,189 it improves contrast and certainty so we 275 00:11:35,170 --> 00:11:33,439 really need to be thinking about the 276 00:11:38,050 --> 00:11:35,180 scenarios in which this is a useful 277 00:11:39,490 --> 00:11:38,060 technique and whether or not we want to 278 00:11:40,990 --> 00:11:39,500 be building our telescopes and our 279 00:11:42,639 --> 00:11:41,000 instruments for this sort of thing and 280 00:11:44,590 --> 00:11:42,649 if so what particular things we want to 281 00:11:45,970 --> 00:11:44,600 be looking for because it is certainly 282 00:11:47,499 --> 00:11:45,980 useful in some cases particularly 283 00:11:51,119 --> 00:11:47,509 dealing with clouds and things that are 284 00:11:53,740 --> 00:11:51,129 not transiting we need to continue to 285 00:11:55,210 --> 00:11:53,750 characterize noise particularly from 286 00:11:57,730 --> 00:11:55,220 stellar activity and cool stars 287 00:12:00,790 --> 00:11:57,740 especially if we want to keep looking at 288 00:12:03,160 --> 00:12:00,800 M dwarfs to overcome issues with food 289 00:12:06,040 --> 00:12:03,170 put to some degree we can use things 290 00:12:07,540 --> 00:12:06,050 like dedicated stairs and thoughtful 291 00:12:09,009 --> 00:12:07,550 observations being a little more 292 00:12:10,660 --> 00:12:09,019 particular than maybe we've been in the 293 00:12:14,139 --> 00:12:10,670 past about which planets we're looking 294 00:12:16,329 --> 00:12:14,149 at and to overcome noise we can consider 295 00:12:18,790 --> 00:12:16,339 things like simultaneous observations 296 00:12:20,439 --> 00:12:18,800 that will help us characterize things 297 00:12:22,269 --> 00:12:20,449 like stellar activity to help us 298 00:12:24,100 --> 00:12:22,279 characterize that noise and also 299 00:12:26,379 --> 00:12:24,110 improving technology which sounds like a 300 00:12:28,869 --> 00:12:26,389 you know kind of ask a really easy thing 301 00:12:31,150 --> 00:12:28,879 to say an hard thing to do but I just 302 00:12:32,889 --> 00:12:31,160 want to point out that hippy the most 303 00:12:34,929 --> 00:12:32,899 sensitive polarimeter in the world right 304 00:12:37,980 --> 00:12:34,939 now for visible wavelengths is built 305 00:12:40,600 --> 00:12:37,990 from the 3d printed components and 306 00:12:43,749 --> 00:12:40,610 optical and lab materials that you can 307 00:12:46,210 --> 00:12:43,759 get out of a lab catalog is a very 308 00:12:48,639 --> 00:12:46,220 inexpensive it's very reproducible and 309 00:12:54,429 --> 00:12:48,649 there are great ideas out there about 310 00:12:56,949 --> 00:12:54,439 how to improve the the noise the the 311 00:12:59,549 --> 00:12:56,959 throughput and the abilities of 312 00:13:01,869 --> 00:12:59,559 polarimeters that people have but 313 00:13:05,079 --> 00:13:01,879 couldn't maybe be funded I don't have a 314 00:13:07,569 --> 00:13:05,089 particular it is just to be clear so I 315 00:13:11,110 --> 00:13:07,579 just want to end on this note of 316 00:13:12,759 --> 00:13:11,120 pointing out that many upcoming space 317 00:13:15,669 --> 00:13:12,769 telescopes and ground-based telescopes 318 00:13:18,550 --> 00:13:15,679 have or considering having or definitely 319 00:13:25,689 --> 00:13:18,560 planning to have polarimeters we 320 00:13:28,600 --> 00:13:25,699 voir origins Space Telescope the TMT the 321 00:13:30,850 --> 00:13:28,610 e-elt w first all have plans for 322 00:13:32,350 --> 00:13:30,860 polarimeters or considering fans for 323 00:13:37,179 --> 00:13:32,360 polarimeters we need to think really 324 00:13:39,759 --> 00:13:37,189 hard over what wavelengths those 325 00:13:41,559 --> 00:13:39,769 polarimeters will cover for example 326 00:13:45,340 --> 00:13:41,569 leVoir will only be in the UV and 327 00:13:46,629 --> 00:13:45,350 origins would Chris be in infrared and 328 00:13:48,160 --> 00:13:46,639 the kind of science that we would be 329 00:13:50,079 --> 00:13:48,170 able to do with that we also need to 330 00:13:52,840 --> 00:13:50,089 think about architecture and whether 331 00:13:55,720 --> 00:13:52,850 it's useful for the kind of science that 332 00:13:58,540 --> 00:13:55,730 we want to do for us to have our 333 00:14:00,910 --> 00:13:58,550 polarimeters in front of our own master 334 00:14:02,920 --> 00:14:00,920 after them because that's going to also 335 00:14:05,590 --> 00:14:02,930 determine obviously the type of science 336 00:14:16,720 --> 00:14:05,600 that we could be doing and without all 337 00:14:21,210 --> 00:14:16,730 open it to questions yes so are you 338 00:14:23,559 --> 00:14:21,220 assuming like it covers the entire 339 00:14:26,350 --> 00:14:23,569 planet like a disk integrated right so 340 00:14:30,429 --> 00:14:26,360 then you're really combining yeah yeah 341 00:14:34,960 --> 00:14:30,439 so so these are disk integrated the 342 00:14:36,790 --> 00:14:34,970 signals for planets that have a uniform 343 00:14:38,170 --> 00:14:36,800 coverage of whatever it is that I've 344 00:14:39,670 --> 00:14:38,180 done there so they can have a different 345 00:14:41,740 --> 00:14:39,680 grounds and a different you know 346 00:14:44,829 --> 00:14:41,750 different layers of clouds but it's over 347 00:14:47,139 --> 00:14:44,839 the entire planet the output from these 348 00:14:50,619 --> 00:14:47,149 star which is modeling code that I use 349 00:14:54,639 --> 00:14:50,629 actually does produce a pretty outfit so 350 00:14:56,079 --> 00:14:54,649 it's in the works I guess I don't know 351 00:14:58,900 --> 00:14:56,089 how fast it'll come up but it's in the 352 00:15:05,490 --> 00:14:58,910 works to be able to produce or be able 353 00:15:07,869 --> 00:15:05,500 to use a 3d input to like improve the 354 00:15:19,030 --> 00:15:07,879 swath of things that we could be 355 00:15:22,110 --> 00:15:19,040 exploring with B star yeah RJ hi RJ from 356 00:15:24,280 --> 00:15:22,120 Oxford at the beginning you mentioned 357 00:15:25,419 --> 00:15:24,290 chiral molecules and then you said you 358 00:15:28,480 --> 00:15:25,429 were going to talk about it anymore but 359 00:15:30,730 --> 00:15:28,490 I wanted to ask if so do chiral 360 00:15:32,200 --> 00:15:30,740 molecules produce like a noticeable 361 00:15:36,550 --> 00:15:32,210 polar 362 00:15:41,920 --> 00:15:36,560 signal in mmm spectroscopy yeah so 363 00:15:45,100 --> 00:15:41,930 chiral molecules can impart circularly 364 00:15:48,220 --> 00:15:45,110 polarized light that's really too weak 365 00:15:51,699 --> 00:15:48,230 of a signal for anytime in the near 366 00:15:53,980 --> 00:15:51,709 future to be doing that with exoplanets 367 00:15:56,380 --> 00:15:53,990 most likely but it's something that's 368 00:15:58,120 --> 00:15:56,390 really useful and interesting for 369 00:16:00,250 --> 00:15:58,130 astrobiology studies in our own solar 370 00:16:02,019 --> 00:16:00,260 system you could potentially be doing 371 00:16:22,810 --> 00:16:02,029 this just with like a Europa Lander or 372 00:16:24,699 --> 00:16:22,820 something like that yes that was a 373 00:16:27,460 --> 00:16:24,709 really interesting talk Ted camasta q 374 00:16:30,130 --> 00:16:27,470 Chicago so it seemed like you needed 375 00:16:31,750 --> 00:16:30,140 like phase resolved observations to get 376 00:16:33,010 --> 00:16:31,760 information about say like clouds or 377 00:16:35,230 --> 00:16:33,020 something in the atmosphere do you 378 00:16:36,790 --> 00:16:35,240 always need like a full half orbit phase 379 00:16:38,110 --> 00:16:36,800 curve or is there like shorter term 380 00:16:41,590 --> 00:16:38,120 observations that can tell you something 381 00:16:42,940 --> 00:16:41,600 similar you could if you have some idea 382 00:16:44,650 --> 00:16:42,950 of what you want to look for or what you 383 00:16:46,510 --> 00:16:44,660 could anticipate from a planet which I 384 00:16:48,220 --> 00:16:46,520 mean you can just sometimes do from 385 00:16:50,920 --> 00:16:48,230 physics knowing the size of it and what 386 00:16:54,579 --> 00:16:50,930 sort of you know Cubs you might expect 387 00:16:57,130 --> 00:16:54,589 where you can just kind of sample around 388 00:16:58,720 --> 00:16:57,140 where you might expect say a rainbow and 389 00:17:01,120 --> 00:16:58,730 see if you do see the peak in the 390 00:17:02,290 --> 00:17:01,130 rainbow exactly where you predict if you 391 00:17:04,540 --> 00:17:02,300 think that there's water clouds at the 392 00:17:06,880 --> 00:17:04,550 top of the atmosphere does that arise at 393 00:17:10,540 --> 00:17:06,890 the right spot for the cloud height that 394 00:17:11,980 --> 00:17:10,550 you expect you can you can really narrow 395 00:17:16,329 --> 00:17:11,990 this down so you can just do a lot of 396 00:17:17,290 --> 00:17:16,339 sampling at a particular point if that's 397 00:17:19,829 --> 00:17:17,300 something that you're looking for if 398 00:17:21,880 --> 00:17:19,839 you're trying to do something like 399 00:17:23,140 --> 00:17:21,890 constraint orbital parameters or 400 00:17:25,090 --> 00:17:23,150 something like that that's depending a 401 00:17:26,199 --> 00:17:25,100 lot more on like the general shape up 402 00:17:32,919 --> 00:17:26,209 the curves and you would want really 403 00:17:33,330 --> 00:17:32,929 good sampling throughout if there are no 404 00:17:35,340 --> 00:17:33,340 additional 405 00:17:35,880 --> 00:17:35,350 questions thank Kim