1 00:00:05,030 --> 00:00:02,230 hi everyone my name is chris visa 2 00:00:06,470 --> 00:00:05,040 program and i'm a fifth year phd student 3 00:00:08,150 --> 00:00:06,480 at caltech 4 00:00:10,230 --> 00:00:08,160 and today i'll be talking a little bit 5 00:00:12,789 --> 00:00:10,240 about our project studying the 6 00:00:16,630 --> 00:00:12,799 atmospheric evolution of three young 7 00:00:18,070 --> 00:00:16,640 planets in the v1298 tau system 8 00:00:20,470 --> 00:00:18,080 this is work that i've done with my 9 00:00:22,150 --> 00:00:20,480 advisor heather knudsen along with all 10 00:00:23,830 --> 00:00:22,160 of the collaborators you see on the 11 00:00:25,750 --> 00:00:23,840 screen 12 00:00:27,830 --> 00:00:25,760 first i'm going to be talking about the 13 00:00:29,470 --> 00:00:27,840 evolving atmospheres of young planets 14 00:00:32,069 --> 00:00:29,480 and why this topic might be 15 00:00:33,590 --> 00:00:32,079 astrobiologically relevant 16 00:00:35,430 --> 00:00:33,600 then i'm going to talk about how we 17 00:00:37,510 --> 00:00:35,440 actually make observations of 18 00:00:39,270 --> 00:00:37,520 atmospheric evolution in young planets 19 00:00:42,630 --> 00:00:39,280 and in particular i'll be discussing a 20 00:00:45,190 --> 00:00:42,640 technique called helium photometry 21 00:00:47,990 --> 00:00:45,200 and finally i'll discuss our recent 22 00:00:50,950 --> 00:00:48,000 results applying helium photometry to 23 00:00:52,630 --> 00:00:50,960 the planets in the v1298 tau system and 24 00:00:54,229 --> 00:00:52,640 i'll motivate some future work that i 25 00:00:56,069 --> 00:00:54,239 hope will get done over the next few 26 00:00:57,590 --> 00:00:56,079 years 27 00:00:59,590 --> 00:00:57,600 the fundamental question that we're 28 00:01:03,990 --> 00:00:59,600 trying to answer is how do planetary 29 00:01:08,630 --> 00:01:06,390 to situate ourselves the majority of 30 00:01:10,870 --> 00:01:08,640 extrasolar planets planets orbiting 31 00:01:13,109 --> 00:01:10,880 stars that are not our sun 32 00:01:15,670 --> 00:01:13,119 orbit quite close to their host stars 33 00:01:16,789 --> 00:01:15,680 within an orbital period of 100 days or 34 00:01:18,149 --> 00:01:16,799 so 35 00:01:19,990 --> 00:01:18,159 this means that these planets are 36 00:01:22,550 --> 00:01:20,000 getting constantly bombarded by 37 00:01:25,350 --> 00:01:22,560 high-energy radiation and that can 38 00:01:27,109 --> 00:01:25,360 really change how the planet looks to us 39 00:01:29,270 --> 00:01:27,119 and how the planet evolves over its 40 00:01:31,590 --> 00:01:29,280 lifetime 41 00:01:33,510 --> 00:01:31,600 consider a hydrogen atom living in an 42 00:01:36,149 --> 00:01:33,520 exoplanet atmosphere 43 00:01:37,990 --> 00:01:36,159 because the planet is so irradiated 44 00:01:41,109 --> 00:01:38,000 that hydrogen atom is going to see an 45 00:01:44,630 --> 00:01:41,119 extreme ultraviolet photon with 46 00:01:46,710 --> 00:01:44,640 energy exceeding 13.6 electron volts 47 00:01:49,030 --> 00:01:46,720 quite often 48 00:01:51,910 --> 00:01:49,040 and what that photon can do is it can 49 00:01:56,709 --> 00:01:51,920 ionize the hydrogen atom 50 00:01:59,109 --> 00:01:56,719 but if the photon energy exceeds 13.6 ev 51 00:02:01,030 --> 00:01:59,119 that excess energy has to go somewhere 52 00:02:03,109 --> 00:02:01,040 and it goes into heating 53 00:02:05,270 --> 00:02:03,119 the gas goes into the thermal energy of 54 00:02:07,270 --> 00:02:05,280 the planetary atmosphere 55 00:02:08,790 --> 00:02:07,280 and as this happens many many times 56 00:02:10,229 --> 00:02:08,800 because the planet is severely 57 00:02:12,309 --> 00:02:10,239 irradiated 58 00:02:14,790 --> 00:02:12,319 for many many hydrogen and helium atoms 59 00:02:17,270 --> 00:02:14,800 in the planetary atmosphere 60 00:02:19,990 --> 00:02:17,280 the net effect is the planetary 61 00:02:22,470 --> 00:02:20,000 atmosphere can heat up so much 62 00:02:25,110 --> 00:02:22,480 that it becomes gravitationally unbound 63 00:02:27,670 --> 00:02:25,120 that the planetary atmosphere is just 64 00:02:31,910 --> 00:02:29,430 and we can imagine that this has pretty 65 00:02:35,589 --> 00:02:31,920 important consequences for the planetary 66 00:02:37,589 --> 00:02:35,599 mass as the material is literally being 67 00:02:39,910 --> 00:02:37,599 lost from the system 68 00:02:41,509 --> 00:02:39,920 for the planetary radius as well as i'll 69 00:02:44,070 --> 00:02:41,519 show in a second 70 00:02:45,910 --> 00:02:44,080 and also for habitability the presence 71 00:02:48,470 --> 00:02:45,920 or absence of an atmosphere is known to 72 00:02:50,949 --> 00:02:48,480 be quite astrobiologically relevant and 73 00:02:53,509 --> 00:02:50,959 so understanding the primary factors 74 00:02:56,309 --> 00:02:53,519 that control whether a planet can retain 75 00:02:57,830 --> 00:02:56,319 or whether it loses an atmosphere is of 76 00:03:01,190 --> 00:02:57,840 utmost importance 77 00:03:05,110 --> 00:03:03,110 now to briefly mention one consequence 78 00:03:06,949 --> 00:03:05,120 of atmospheric evolution we can take a 79 00:03:09,830 --> 00:03:06,959 look at the histogram of observed 80 00:03:11,670 --> 00:03:09,840 exoplanet radii from bj fulton's work 81 00:03:13,589 --> 00:03:11,680 done in 2018. 82 00:03:16,710 --> 00:03:13,599 what's being shown here is the average 83 00:03:19,030 --> 00:03:16,720 number of planets per star as a function 84 00:03:21,589 --> 00:03:19,040 of planetary size and i've indicated the 85 00:03:23,030 --> 00:03:21,599 sizes of earth neptune and jupiter for 86 00:03:24,789 --> 00:03:23,040 reference 87 00:03:26,149 --> 00:03:24,799 and while you can see that the most 88 00:03:28,710 --> 00:03:26,159 common type of planet that's been 89 00:03:31,589 --> 00:03:28,720 discovered to date is something between 90 00:03:33,030 --> 00:03:31,599 the size of the earth and neptune 91 00:03:34,630 --> 00:03:33,040 we can see that the distribution is 92 00:03:36,550 --> 00:03:34,640 pretty bimodal 93 00:03:38,630 --> 00:03:36,560 and actually this has a lot to do with 94 00:03:40,869 --> 00:03:38,640 atmospheric evolution we think that 95 00:03:43,270 --> 00:03:40,879 planets on the large side of this radius 96 00:03:45,750 --> 00:03:43,280 gap called subneptunes 97 00:03:48,070 --> 00:03:45,760 at around 2.5 earth radii 98 00:03:49,990 --> 00:03:48,080 we think that these planets retained 99 00:03:52,949 --> 00:03:50,000 most of their atmosphere against the 100 00:03:54,710 --> 00:03:52,959 effects of atmospheric escape 101 00:03:56,229 --> 00:03:54,720 and we think planets on the small side 102 00:03:58,949 --> 00:03:56,239 of the radius gap 103 00:04:00,149 --> 00:03:58,959 at around 1.5 earth radii 104 00:04:01,750 --> 00:04:00,159 we think that they lost their 105 00:04:04,149 --> 00:04:01,760 atmospheres 106 00:04:06,470 --> 00:04:04,159 and so clearly atmospheric evolution has 107 00:04:07,429 --> 00:04:06,480 an outsized impact on how planets appear 108 00:04:09,350 --> 00:04:07,439 to us 109 00:04:11,589 --> 00:04:09,360 and how planets evolve over their 110 00:04:14,070 --> 00:04:11,599 lifetimes 111 00:04:16,550 --> 00:04:14,080 now to understand when this process is 112 00:04:18,629 --> 00:04:16,560 happening over a planet's lifetime it's 113 00:04:20,870 --> 00:04:18,639 necessary to look at the high energy 114 00:04:22,629 --> 00:04:20,880 radiation of the host star 115 00:04:24,469 --> 00:04:22,639 and what's being plotted here is the 116 00:04:27,749 --> 00:04:24,479 x-ray luminosity 117 00:04:28,710 --> 00:04:27,759 of three different stellar models with 118 00:04:30,469 --> 00:04:28,720 different 119 00:04:33,110 --> 00:04:30,479 rotation rates 120 00:04:35,990 --> 00:04:33,120 as a function of stellar age and you can 121 00:04:38,390 --> 00:04:36,000 see that for all three models the star 122 00:04:40,710 --> 00:04:38,400 is outputting much more x-ray luminosity 123 00:04:42,390 --> 00:04:40,720 over the first 100 million years or so 124 00:04:44,469 --> 00:04:42,400 of its life 125 00:04:46,230 --> 00:04:44,479 and what that leads us to conclude is 126 00:04:48,550 --> 00:04:46,240 that we should try to observe 127 00:04:51,430 --> 00:04:48,560 atmospheric escape when it's happening 128 00:04:54,150 --> 00:04:51,440 to planets that are less than around 100 129 00:04:56,710 --> 00:04:54,160 million years old or so 130 00:04:58,629 --> 00:04:56,720 now the problem is that most planets 131 00:05:00,950 --> 00:04:58,639 that have ever been discovered 132 00:05:03,830 --> 00:05:00,960 are about a gig a year or older most of 133 00:05:05,510 --> 00:05:03,840 these planets are positively ancient 134 00:05:08,310 --> 00:05:05,520 compared to the time scales on which 135 00:05:10,070 --> 00:05:08,320 atmospheric escape happens 136 00:05:11,590 --> 00:05:10,080 so the problem is we've never observed 137 00:05:13,430 --> 00:05:11,600 how the atmospheres of young planets 138 00:05:14,790 --> 00:05:13,440 evolved before 139 00:05:16,790 --> 00:05:14,800 and this really prevents us from 140 00:05:18,629 --> 00:05:16,800 answering the question how efficiently 141 00:05:19,430 --> 00:05:18,639 can young planets turn radiation into 142 00:05:21,590 --> 00:05:19,440 heat 143 00:05:24,469 --> 00:05:21,600 this is the primary control on whether a 144 00:05:26,469 --> 00:05:24,479 planet keeps or loses its atmosphere and 145 00:05:29,749 --> 00:05:26,479 so this quantity is of utmost 146 00:05:31,830 --> 00:05:29,759 astrobiological relevance 147 00:05:35,350 --> 00:05:31,840 to remedy this we looked at the young 148 00:05:37,510 --> 00:05:35,360 transiting system v1298 tau 149 00:05:38,870 --> 00:05:37,520 which was discovered by trevor david in 150 00:05:40,870 --> 00:05:38,880 2019 151 00:05:42,870 --> 00:05:40,880 now i'll clarify what transiting means 152 00:05:44,469 --> 00:05:42,880 in a second but basically it just means 153 00:05:46,390 --> 00:05:44,479 that the planets pass in front of the 154 00:05:48,710 --> 00:05:46,400 host star with respect to our line of 155 00:05:51,110 --> 00:05:48,720 sight 156 00:05:53,110 --> 00:05:51,120 now this system is 23 million years old 157 00:05:57,350 --> 00:05:53,120 so it's young enough for us to observe 158 00:05:58,790 --> 00:05:57,360 atmospheric escape occurring in action 159 00:06:01,430 --> 00:05:58,800 there are three known planets in the 160 00:06:03,510 --> 00:06:01,440 system planet c with orbital period 8 161 00:06:04,950 --> 00:06:03,520 days and a size about half that of 162 00:06:07,670 --> 00:06:04,960 jupiter 163 00:06:10,870 --> 00:06:07,680 planet d with orbital period 12 days and 164 00:06:13,510 --> 00:06:10,880 a little bit larger than planet c 165 00:06:17,189 --> 00:06:13,520 and then planet b with orbital period 24 166 00:06:19,350 --> 00:06:17,199 days and a size about that of jupiter 167 00:06:21,670 --> 00:06:19,360 so now that we've selected a target we 168 00:06:24,230 --> 00:06:21,680 can ask how do we observe atmospheric 169 00:06:26,230 --> 00:06:24,240 escape in action 170 00:06:28,550 --> 00:06:26,240 one way to do this is with a technique 171 00:06:30,390 --> 00:06:28,560 called transit spectroscopy 172 00:06:31,990 --> 00:06:30,400 so in the transit method we're watching 173 00:06:34,550 --> 00:06:32,000 planets as they pass in front of their 174 00:06:36,070 --> 00:06:34,560 host stars and block out a little bit of 175 00:06:38,790 --> 00:06:36,080 the star's light 176 00:06:40,629 --> 00:06:38,800 and larger planets block out 177 00:06:42,710 --> 00:06:40,639 proportionally more light from the host 178 00:06:44,629 --> 00:06:42,720 star 179 00:06:47,029 --> 00:06:44,639 now we can visualize this diagram in 180 00:06:50,070 --> 00:06:47,039 this very not to scale cartoon shown 181 00:06:52,150 --> 00:06:50,080 here and again some light from the host 182 00:06:54,150 --> 00:06:52,160 star will be blocked by the planet and 183 00:06:56,309 --> 00:06:54,160 won't reach your telescope 184 00:06:58,150 --> 00:06:56,319 during a transit i should say but some 185 00:07:01,029 --> 00:06:58,160 of the light will reach your telescope 186 00:07:02,950 --> 00:07:01,039 and this is kind of the nominal case 187 00:07:05,189 --> 00:07:02,960 however when a planet's atmosphere is 188 00:07:06,710 --> 00:07:05,199 escaping some of that light is actually 189 00:07:09,110 --> 00:07:06,720 getting filtered through that low 190 00:07:11,110 --> 00:07:09,120 density escaping atmosphere 191 00:07:13,270 --> 00:07:11,120 and if we can choose 192 00:07:16,309 --> 00:07:13,280 to observe at a wavelength where that 193 00:07:18,550 --> 00:07:16,319 low density tenuous gas becomes opaque 194 00:07:20,870 --> 00:07:18,560 then suddenly the planet 195 00:07:23,430 --> 00:07:20,880 will absorb it'll block out much more 196 00:07:25,029 --> 00:07:23,440 light and the planet will appear much 197 00:07:27,029 --> 00:07:25,039 larger to us 198 00:07:28,870 --> 00:07:27,039 so now we'll quickly describe how we 199 00:07:31,430 --> 00:07:28,880 make these measurements in practice uh 200 00:07:34,070 --> 00:07:31,440 with helium photometry 201 00:07:35,670 --> 00:07:34,080 so our experimental experimental design 202 00:07:38,150 --> 00:07:35,680 is pretty simple 203 00:07:39,990 --> 00:07:38,160 we take light from the telescope we pass 204 00:07:42,309 --> 00:07:40,000 it through an optical element called an 205 00:07:44,469 --> 00:07:42,319 engineered diffuser which just helps us 206 00:07:46,070 --> 00:07:44,479 control systematics 207 00:07:48,629 --> 00:07:46,080 that light then goes through an ultra 208 00:07:52,390 --> 00:07:48,639 narrow bandpass filter that is centered 209 00:07:54,390 --> 00:07:52,400 on that 1080 1083 nanometer line 210 00:07:56,150 --> 00:07:54,400 uh and then it forms our image where we 211 00:07:57,990 --> 00:07:56,160 can take a picture much like you would 212 00:08:00,469 --> 00:07:58,000 take a picture with your iphone camera 213 00:08:02,469 --> 00:08:00,479 except that we take it in the infrared 214 00:08:03,909 --> 00:08:02,479 and we take many many many pictures over 215 00:08:06,390 --> 00:08:03,919 the course of a night 216 00:08:09,990 --> 00:08:06,400 and we track the star's brightness in 217 00:08:12,390 --> 00:08:10,000 all those pictures to form a light curve 218 00:08:14,629 --> 00:08:12,400 and based on how much light gets blocked 219 00:08:16,950 --> 00:08:14,639 out during the planetary transit we can 220 00:08:19,110 --> 00:08:16,960 tell whether or not helium absorption is 221 00:08:21,510 --> 00:08:19,120 going on in the planetary atmosphere and 222 00:08:24,710 --> 00:08:21,520 in so doing we can tell how quickly that 223 00:08:28,309 --> 00:08:26,790 so here's an example of a measurement we 224 00:08:33,110 --> 00:08:28,319 made when we were commissioning this 225 00:08:36,389 --> 00:08:33,120 observing mode of the planet wasp 69b 226 00:08:38,630 --> 00:08:36,399 now this planet when observed at other 227 00:08:41,829 --> 00:08:38,640 less special wavelengths 228 00:08:43,829 --> 00:08:41,839 looks like this in the blue 229 00:08:45,990 --> 00:08:43,839 what's being shown here is the star's 230 00:08:47,350 --> 00:08:46,000 brightness over time and you can see 231 00:08:49,110 --> 00:08:47,360 that the planet 232 00:08:50,710 --> 00:08:49,120 at the transit center is blocking out a 233 00:08:52,790 --> 00:08:50,720 little less than two percent of the 234 00:08:55,269 --> 00:08:52,800 star's light 235 00:08:57,829 --> 00:08:55,279 however when we measured it at 1083 236 00:09:00,230 --> 00:08:57,839 nanometers we got the data in gray 237 00:09:03,110 --> 00:09:00,240 which are binned in black and shown with 238 00:09:05,829 --> 00:09:03,120 our best fit model in red 239 00:09:08,150 --> 00:09:05,839 and clearly at 1083 nanometers the 240 00:09:10,630 --> 00:09:08,160 planet blocks out more than two percent 241 00:09:12,630 --> 00:09:10,640 of the star's light 242 00:09:14,790 --> 00:09:12,640 and so we use this measurement to 243 00:09:18,550 --> 00:09:14,800 confirm the presence of helium in the 244 00:09:19,910 --> 00:09:18,560 atmosphere of wasp 69b at 10.1 sigma 245 00:09:20,630 --> 00:09:19,920 confidence 246 00:09:22,710 --> 00:09:20,640 now 247 00:09:24,389 --> 00:09:22,720 this system is pretty old so it doesn't 248 00:09:26,310 --> 00:09:24,399 tell us about what's going on when 249 00:09:28,230 --> 00:09:26,320 atmospheric escape is most important for 250 00:09:30,230 --> 00:09:28,240 a planet's life but it helped us 251 00:09:32,630 --> 00:09:30,240 understand how our instrument worked and 252 00:09:37,269 --> 00:09:32,640 it helped us confirm that everything was 253 00:09:41,829 --> 00:09:39,670 so in this work we applied this 254 00:09:44,070 --> 00:09:41,839 technique to the planets in the v1298 255 00:09:46,710 --> 00:09:44,080 tau system and now we'll describe some 256 00:09:49,190 --> 00:09:46,720 of the results that we saw 257 00:09:51,990 --> 00:09:49,200 when we looked at the transit of v1298 258 00:09:53,110 --> 00:09:52,000 tau c we weren't able to detect anything 259 00:09:54,949 --> 00:09:53,120 at all 260 00:09:56,790 --> 00:09:54,959 our light curve is shown on the left 261 00:09:59,030 --> 00:09:56,800 with data in gray 262 00:10:02,230 --> 00:09:59,040 uh bend in black 263 00:10:04,710 --> 00:10:02,240 with a best fit model in the solid line 264 00:10:07,350 --> 00:10:04,720 and the model for the transit at 265 00:10:09,269 --> 00:10:07,360 non 1093 nanometer wavelengths in the 266 00:10:11,030 --> 00:10:09,279 dashed line and i've also shown a 267 00:10:12,949 --> 00:10:11,040 baseline model for 268 00:10:15,509 --> 00:10:12,959 just showing how the star and the 269 00:10:16,949 --> 00:10:15,519 weather evolve over the night 270 00:10:19,509 --> 00:10:16,959 uh in red 271 00:10:21,509 --> 00:10:19,519 and you can see that the model the solid 272 00:10:24,470 --> 00:10:21,519 line doesn't really indicate that we 273 00:10:26,150 --> 00:10:24,480 detected transit at any confidence 274 00:10:28,310 --> 00:10:26,160 this is kind of disappointing and it's 275 00:10:30,230 --> 00:10:28,320 probably due to poor weather which you 276 00:10:31,829 --> 00:10:30,240 know sometimes you get unlucky 277 00:10:33,590 --> 00:10:31,839 but at the same time we can definitely 278 00:10:35,590 --> 00:10:33,600 rule out a very large transit in the 279 00:10:38,630 --> 00:10:35,600 helium line which is an important result 280 00:10:43,110 --> 00:10:40,389 when we looked at planet b i've shown 281 00:10:45,030 --> 00:10:43,120 the same thing for planet b on the right 282 00:10:47,350 --> 00:10:45,040 we did detect the planet 283 00:10:49,350 --> 00:10:47,360 uh the transit of this planet 284 00:10:51,030 --> 00:10:49,360 but we don't think we detected any clear 285 00:10:53,509 --> 00:10:51,040 helium absorption 286 00:10:56,150 --> 00:10:53,519 our best fit model is shown 287 00:10:58,069 --> 00:10:56,160 on the right in the solid green line and 288 00:11:01,509 --> 00:10:58,079 the dash green line shows the best fit 289 00:11:03,190 --> 00:11:01,519 model at non 1083 nanometer wavelengths 290 00:11:05,030 --> 00:11:03,200 and you can see that the models kind of 291 00:11:07,269 --> 00:11:05,040 overly each other they have slightly 292 00:11:09,509 --> 00:11:07,279 different shapes but they're not really 293 00:11:11,030 --> 00:11:09,519 distinguishable in any statistically 294 00:11:13,030 --> 00:11:11,040 significant way 295 00:11:14,550 --> 00:11:13,040 so a larger transit in the helium line 296 00:11:16,310 --> 00:11:14,560 is still possible but we would 297 00:11:17,670 --> 00:11:16,320 definitely need more data to confirm 298 00:11:19,750 --> 00:11:17,680 that 299 00:11:21,910 --> 00:11:19,760 now when we looked at planet d we think 300 00:11:24,150 --> 00:11:21,920 we see a tentative detection 301 00:11:25,910 --> 00:11:24,160 now we took two knights of data on this 302 00:11:27,509 --> 00:11:25,920 planet which are shown with the circles 303 00:11:28,470 --> 00:11:27,519 and triangles in the light curve on the 304 00:11:30,310 --> 00:11:28,480 left 305 00:11:32,150 --> 00:11:30,320 and the signal appears consistent in 306 00:11:34,870 --> 00:11:32,160 amplitude across both knights of data 307 00:11:36,470 --> 00:11:34,880 collection which is really exciting 308 00:11:38,310 --> 00:11:36,480 however 309 00:11:40,470 --> 00:11:38,320 to stitch this light curve together we 310 00:11:42,150 --> 00:11:40,480 did require a transit timing offset 311 00:11:44,550 --> 00:11:42,160 which is the slight deviation from a 312 00:11:46,870 --> 00:11:44,560 keplerian orbit and that was enough to 313 00:11:48,389 --> 00:11:46,880 make us a bit hesitant about the result 314 00:11:50,949 --> 00:11:48,399 and so we're calling it a tentative 315 00:11:52,870 --> 00:11:50,959 detection rather than a slam dunk 316 00:11:54,310 --> 00:11:52,880 still it's a really interesting result 317 00:11:56,870 --> 00:11:54,320 and it means that this planet should be 318 00:11:58,629 --> 00:11:56,880 prioritized for future follow-up 319 00:12:00,790 --> 00:11:58,639 to summarize our work 320 00:12:02,710 --> 00:12:00,800 we are attempting to measure atmospheric 321 00:12:03,509 --> 00:12:02,720 escape from young planets for the first 322 00:12:05,670 --> 00:12:03,519 time 323 00:12:08,230 --> 00:12:05,680 and here's a graphic of the geometry of 324 00:12:10,310 --> 00:12:08,240 what we're actually measuring 325 00:12:12,710 --> 00:12:10,320 now we tentatively detect helium 326 00:12:14,470 --> 00:12:12,720 absorption for v1298 tau d 327 00:12:16,389 --> 00:12:14,480 which indicates that this might be the 328 00:12:19,269 --> 00:12:16,399 first known young planet with 329 00:12:21,110 --> 00:12:19,279 observationally accessible mass loss and 330 00:12:23,509 --> 00:12:21,120 in the future we'd of course like to get 331 00:12:25,509 --> 00:12:23,519 more data which uh we'll be hopefully 332 00:12:27,750 --> 00:12:25,519 gathering some more full transits in the 333 00:12:29,030 --> 00:12:27,760 winter weather permitting 334 00:12:31,030 --> 00:12:29,040 and we'd also like to measure the 335 00:12:32,710 --> 00:12:31,040 planetary masses to know the 336 00:12:34,470 --> 00:12:32,720 gravitational potentials from which 337 00:12:35,670 --> 00:12:34,480 these planets atmospheres may be 338 00:12:37,430 --> 00:12:35,680 escaping