1 00:00:12,250 --> 00:00:06,150 you 2 00:00:16,000 --> 00:00:14,129 [Music] 3 00:00:17,560 --> 00:00:16,010 well first I'd like to thank my 4 00:00:18,700 --> 00:00:17,570 conference organizers for giving me the 5 00:00:20,380 --> 00:00:18,710 opportunity to speak with you today 6 00:00:22,480 --> 00:00:20,390 about some of my thesis research and 7 00:00:25,390 --> 00:00:22,490 low-mass stars and containing this trend 8 00:00:30,160 --> 00:00:25,400 of basically learning more about the 9 00:00:31,540 --> 00:00:30,170 m-dwarf population and this is doing and 10 00:00:32,470 --> 00:00:31,550 I'd also like to take a moment to 11 00:00:36,220 --> 00:00:32,480 acknowledge my collaborators on this 12 00:00:38,680 --> 00:00:36,230 project as well okay so first off as 13 00:00:39,939 --> 00:00:38,690 we've heard M Norris are really forming 14 00:00:42,460 --> 00:00:39,949 the dominant constituent of the sellout 15 00:00:44,850 --> 00:00:42,470 of population and this is visualized 16 00:00:46,720 --> 00:00:44,860 here on the right and a snapshot from a 17 00:00:49,270 --> 00:00:46,730 graphic from a drew Cordell and the 18 00:00:51,160 --> 00:00:49,280 recons team of the solar neighborhood so 19 00:00:52,959 --> 00:00:51,170 looking at the 25 parsecs with our Sun 20 00:00:55,240 --> 00:00:52,969 here at the center showing the over 20 21 00:00:56,799 --> 00:00:55,250 over 75 percent of the stars in our 22 00:00:58,959 --> 00:00:56,809 solar neighborhood are these low mass M 23 00:01:00,610 --> 00:00:58,969 dwarf stars and that we and as we've 24 00:01:02,170 --> 00:01:00,620 heard already this week there's great 25 00:01:04,090 --> 00:01:02,180 intrinsic interest in understanding the 26 00:01:05,499 --> 00:01:04,100 planet properties of these stars as well 27 00:01:07,090 --> 00:01:05,509 as investigating and assessing their 28 00:01:09,570 --> 00:01:07,100 however will zones and intrinsic 29 00:01:11,950 --> 00:01:09,580 properties so one of the things that 30 00:01:13,630 --> 00:01:11,960 despite the the great abundance 31 00:01:15,279 --> 00:01:13,640 preponderance of these low mass stars 32 00:01:16,359 --> 00:01:15,289 there's still a lot that we haven't 33 00:01:18,130 --> 00:01:16,369 learned yet about their binary 34 00:01:19,870 --> 00:01:18,140 properties the properties of their pro 35 00:01:21,850 --> 00:01:19,880 planetary discs and the platforming 36 00:01:23,620 --> 00:01:21,860 potential of these systems and so of 37 00:01:25,390 --> 00:01:23,630 course all of these three key aspects 38 00:01:26,760 --> 00:01:25,400 play into what we can understand about 39 00:01:29,249 --> 00:01:26,770 the habitable zones when these systems 40 00:01:31,179 --> 00:01:29,259 the disk truncation that might be 41 00:01:33,100 --> 00:01:31,189 altered by the presence of a binary 42 00:01:35,109 --> 00:01:33,110 companion the content of the disks 43 00:01:36,850 --> 00:01:35,119 youselves and a dynamical history and 44 00:01:38,800 --> 00:01:36,860 evolution and interplay between the star 45 00:01:40,179 --> 00:01:38,810 the disk and planet and so to 46 00:01:44,200 --> 00:01:40,189 investigate this today I'm going to be 47 00:01:46,990 --> 00:01:44,210 talking about two main results so there 48 00:01:49,480 --> 00:01:47,000 we go one field m-dwarf multiplicity so 49 00:01:51,370 --> 00:01:49,490 we're looking at just this interior 15 50 00:01:53,109 --> 00:01:51,380 parsec region of the closest brightest m 51 00:01:54,969 --> 00:01:53,119 dwarf to measure their binary properties 52 00:01:56,620 --> 00:01:54,979 and then we're going to move outward to 53 00:01:57,940 --> 00:01:56,630 the tourist star forming region one 54 00:01:59,260 --> 00:01:57,950 hundred and forty parts like distant 55 00:02:01,090 --> 00:01:59,270 which is about one to two million years 56 00:02:03,340 --> 00:02:01,100 old to understand the protoplanetary 57 00:02:06,700 --> 00:02:03,350 disk properties of much younger analog 58 00:02:09,340 --> 00:02:06,710 systems so starting off of the binaries 59 00:02:12,370 --> 00:02:09,350 the first thing that I talk about is our 60 00:02:14,920 --> 00:02:12,380 M dwarfs in multiples or mm survey so 61 00:02:17,229 --> 00:02:14,930 this is a volume limited survey of 245 62 00:02:19,539 --> 00:02:17,239 stars within fifteen parsecs and we can 63 00:02:21,920 --> 00:02:19,549 see that plotted here on this these are 64 00:02:24,050 --> 00:02:21,930 all about 500 stars 65 00:02:25,760 --> 00:02:24,060 within 15 parsecs of the Sun from the 66 00:02:27,440 --> 00:02:25,770 Hipparchus satellite we're looking at 67 00:02:29,060 --> 00:02:27,450 the brightness and V magnitude versus 68 00:02:31,220 --> 00:02:29,070 the color and we're focusing on this 69 00:02:33,230 --> 00:02:31,230 region here of the early M dwarf stars 70 00:02:34,820 --> 00:02:33,240 and the early to mid M dwarfs also have 71 00:02:36,200 --> 00:02:34,830 a nice match with the target selection 72 00:02:37,760 --> 00:02:36,210 that will be upcoming for for example 73 00:02:39,920 --> 00:02:37,770 the test mission which will look at the 74 00:02:41,840 --> 00:02:39,930 nearest brightest M stars with this 75 00:02:43,970 --> 00:02:41,850 population we're searching for stellar 76 00:02:45,740 --> 00:02:43,980 and sub speller companions so looking 77 00:02:47,600 --> 00:02:45,750 for binaries with orbital separations 78 00:02:49,880 --> 00:02:47,610 from about one of you all the way up to 79 00:02:51,590 --> 00:02:49,890 10,000 au and we're doing this with a 80 00:02:54,710 --> 00:02:51,600 combination of multi epoch imaging 81 00:02:56,900 --> 00:02:54,720 approaches so we have high-resolution 82 00:02:58,760 --> 00:02:56,910 archival high-resolution new and 83 00:03:00,800 --> 00:02:58,770 archival adaptive optics imaging and 84 00:03:02,750 --> 00:03:00,810 this lets us look very close in from 85 00:03:04,940 --> 00:03:02,760 about 1 to 100 au for close binary 86 00:03:07,280 --> 00:03:04,950 companions and we complement this with 87 00:03:09,560 --> 00:03:07,290 our tribal wide field plate imaging from 88 00:03:11,300 --> 00:03:09,570 a historic digitized surveys that really 89 00:03:14,360 --> 00:03:11,310 give us about more than 50 years of 90 00:03:18,080 --> 00:03:14,370 baseline to find comoving wide objects 91 00:03:19,850 --> 00:03:18,090 out to ten thousand eight so shown here 92 00:03:21,470 --> 00:03:19,860 we can see some of the example companion 93 00:03:23,720 --> 00:03:21,480 systems with a variety of architectures 94 00:03:26,630 --> 00:03:23,730 mass ratios between the primary and 95 00:03:28,610 --> 00:03:26,640 companion star and of this 245 stars we 96 00:03:31,520 --> 00:03:28,620 find about 65 of them have comoving 97 00:03:33,350 --> 00:03:31,530 stellar companions ranging from as close 98 00:03:35,900 --> 00:03:33,360 as about point Q all the way out to 99 00:03:37,820 --> 00:03:35,910 about 2500 au and on the right we're 100 00:03:39,890 --> 00:03:37,830 looking at our survey sensitivity so 101 00:03:41,420 --> 00:03:39,900 this is the mass in solar masses of a 102 00:03:43,160 --> 00:03:41,430 companion that we could detect in our 103 00:03:44,510 --> 00:03:43,170 imaging survey you can see that we get 104 00:03:46,310 --> 00:03:44,520 all the way down to the bottom of the 105 00:03:49,220 --> 00:03:46,320 main sequence so the transition between 106 00:03:51,500 --> 00:03:49,230 hydrogen burning stars to brown dwarfs 107 00:03:54,440 --> 00:03:51,510 and planets and then we are sensitive to 108 00:03:55,730 --> 00:03:54,450 about 3 au with a by 106 there's an 109 00:03:58,940 --> 00:03:55,740 almost hundred percent completeness to 110 00:04:01,520 --> 00:03:58,950 finding companions in this range so we 111 00:04:02,900 --> 00:04:01,530 can take these binary detection and we 112 00:04:05,120 --> 00:04:02,910 can start to look at kind of aggregate 113 00:04:06,740 --> 00:04:05,130 population properties of our nearest m 114 00:04:08,150 --> 00:04:06,750 dwarf neighbors and so what we're 115 00:04:09,830 --> 00:04:08,160 looking at here is the separation 116 00:04:12,410 --> 00:04:09,840 distribution so this is just a histogram 117 00:04:14,420 --> 00:04:12,420 of the fraction of systems as a function 118 00:04:17,150 --> 00:04:14,430 of the separation of the systems in the 119 00:04:19,310 --> 00:04:17,160 AU and what I want to take it like the 120 00:04:21,260 --> 00:04:19,320 take away home take a waypoint here to 121 00:04:22,850 --> 00:04:21,270 be is that the closer orbital 122 00:04:25,310 --> 00:04:22,860 separations are found with these lower 123 00:04:27,800 --> 00:04:25,320 mass primary stars so if we start with a 124 00:04:29,870 --> 00:04:27,810 type stars in about 300 au is where we 125 00:04:32,719 --> 00:04:29,880 find the typical binary separation if we 126 00:04:34,410 --> 00:04:32,729 move inward to solar-type fgk stars then 127 00:04:35,850 --> 00:04:34,420 it's about 30 au and 128 00:04:37,680 --> 00:04:35,860 you can see in our read mr. Graham here 129 00:04:39,720 --> 00:04:37,690 we actually don't see the population 130 00:04:41,610 --> 00:04:39,730 turnover but we see the bulk of the 131 00:04:43,650 --> 00:04:41,620 binaries are at this sort of six to ten 132 00:04:48,180 --> 00:04:43,660 au separation range so very very close 133 00:04:49,890 --> 00:04:48,190 tight binary systems we can then take 134 00:04:51,480 --> 00:04:49,900 our population and look at just a 135 00:04:54,540 --> 00:04:51,490 fraction of systems that have binary as 136 00:04:56,100 --> 00:04:54,550 all and so what we're looking at here is 137 00:04:57,570 --> 00:04:56,110 the companion star fraction as a 138 00:04:59,970 --> 00:04:57,580 function of primary mass so the most 139 00:05:01,590 --> 00:04:59,980 massive stars here solar-type stars are 140 00:05:04,380 --> 00:05:01,600 new I'm dwarf points and then the brown 141 00:05:06,480 --> 00:05:04,390 dwarf population and what we see is that 142 00:05:07,980 --> 00:05:06,490 we have decreasing multiplicities with 143 00:05:11,000 --> 00:05:07,990 decreasing primary mess well me about 144 00:05:14,010 --> 00:05:11,010 23% of M dwarfs have binary companions 145 00:05:16,110 --> 00:05:14,020 but what we're really looking at here is 146 00:05:17,490 --> 00:05:16,120 that we have fewer binary systems the 147 00:05:18,870 --> 00:05:17,500 ones that we do have are much much 148 00:05:20,460 --> 00:05:18,880 closer and this is of course going to 149 00:05:21,960 --> 00:05:20,470 have really important dynamical 150 00:05:23,850 --> 00:05:21,970 interactions with the extent of the 151 00:05:26,480 --> 00:05:23,860 habitable zone dynamical interaction 152 00:05:29,130 --> 00:05:26,490 between the disk and planets 153 00:05:31,320 --> 00:05:29,140 okay so we're going to move outward now 154 00:05:32,610 --> 00:05:31,330 140 parsecs distant to the torah' star 155 00:05:34,830 --> 00:05:32,620 forming region shown in the background 156 00:05:37,080 --> 00:05:34,840 here and what we wanted to do here was 157 00:05:39,120 --> 00:05:37,090 really understand the dust inventory 158 00:05:40,560 --> 00:05:39,130 within disks of these analog systems 159 00:05:43,410 --> 00:05:40,570 that are much younger around low-mass 160 00:05:44,910 --> 00:05:43,420 stars and what we wanted to be able to 161 00:05:46,920 --> 00:05:44,920 do with these measurements of the disk 162 00:05:48,870 --> 00:05:46,930 mass within the planetary disc is kind 163 00:05:50,700 --> 00:05:48,880 of get a handle on the planet forming 164 00:05:52,170 --> 00:05:50,710 potential of M dwarfs and how that might 165 00:05:54,450 --> 00:05:52,180 compare to that of higher mass stars 166 00:05:55,560 --> 00:05:54,460 then we can take those properties and we 167 00:05:57,180 --> 00:05:55,570 can try to understand how they might 168 00:06:01,530 --> 00:05:57,190 vary with the mass of the central star 169 00:06:03,480 --> 00:06:01,540 the region age and environment and so 170 00:06:05,460 --> 00:06:03,490 this is part of an ongoing survey the 171 00:06:09,000 --> 00:06:05,470 torus boundary is substellar or T Buster 172 00:06:10,920 --> 00:06:09,010 race and was started in 2014 we took far 173 00:06:12,720 --> 00:06:10,930 infrared detection of the lowest mass 174 00:06:14,390 --> 00:06:12,730 stars the latest M dwarfs and brown 175 00:06:17,070 --> 00:06:14,400 dwarfs in this young star forming region 176 00:06:18,600 --> 00:06:17,080 with known for our detections we know 177 00:06:21,240 --> 00:06:18,610 that they have protoplanetary disks and 178 00:06:23,310 --> 00:06:21,250 we followed them up with Alma 885 micron 179 00:06:25,050 --> 00:06:23,320 continuum observations and these really 180 00:06:27,150 --> 00:06:25,060 give us a handle on the submillimetre 181 00:06:30,210 --> 00:06:27,160 emission from the dust grains in the 182 00:06:31,680 --> 00:06:30,220 propietary disk systems and show here is 183 00:06:33,570 --> 00:06:31,690 that the population that we're looking 184 00:06:38,120 --> 00:06:33,580 at this time spans the breadth of the 185 00:06:44,480 --> 00:06:40,670 okay so what we found from the survey of 186 00:06:46,220 --> 00:06:44,490 24 targets which include 10-round or 187 00:06:48,200 --> 00:06:46,230 systems and twelve very low mass star 188 00:06:50,450 --> 00:06:48,210 systems is that we have 22 detections 189 00:06:53,900 --> 00:06:50,460 which is really quite a surprise these 190 00:06:55,790 --> 00:06:53,910 objects are so faint and young and the 191 00:06:57,230 --> 00:06:55,800 disks where the properties are pretty 192 00:06:59,000 --> 00:06:57,240 uncertain before we were able to use the 193 00:07:01,610 --> 00:06:59,010 sensitivity of allness to measure the 194 00:07:03,530 --> 00:07:01,620 disk the disk dust masses in these 195 00:07:04,970 --> 00:07:03,540 systems and so what we're looking at 196 00:07:07,070 --> 00:07:04,980 here is an example detection this is 197 00:07:09,470 --> 00:07:07,080 just the spectral energy distribution so 198 00:07:10,940 --> 00:07:09,480 the flux at different wavelengths in 199 00:07:12,590 --> 00:07:10,950 microns and so we see the contribution 200 00:07:14,900 --> 00:07:12,600 from the star here the tell-tale 201 00:07:16,340 --> 00:07:14,910 signature of a disk around the system 202 00:07:18,350 --> 00:07:16,350 and the new alma measurement here and 203 00:07:21,230 --> 00:07:18,360 something else you can see is that this 204 00:07:22,670 --> 00:07:21,240 is our beam size the resolving capacity 205 00:07:24,320 --> 00:07:22,680 of the all mobster patient's to 206 00:07:25,220 --> 00:07:24,330 understand the extent of the emission in 207 00:07:26,450 --> 00:07:25,230 the disk and you can see that we're 208 00:07:28,070 --> 00:07:26,460 actually starting to resolve these 209 00:07:30,680 --> 00:07:28,080 systems and get a handle on what the 210 00:07:31,760 --> 00:07:30,690 disk sizes are actually and so what we 211 00:07:33,350 --> 00:07:31,770 can do with these submillimetre 212 00:07:35,780 --> 00:07:33,360 continuum flexes is we hear a little bit 213 00:07:37,340 --> 00:07:35,790 before is we can use these to estimate 214 00:07:39,560 --> 00:07:37,350 the mass of dust and submillimetre 215 00:07:41,210 --> 00:07:39,570 grains for these lowest mass systems we 216 00:07:43,580 --> 00:07:41,220 find that they range from about 0.3 to 217 00:07:46,670 --> 00:07:43,590 22 earth masses in total of some 218 00:07:48,200 --> 00:07:46,680 millimetre greens so we can visualize 219 00:07:49,640 --> 00:07:48,210 this and I'll step through kind of 220 00:07:50,420 --> 00:07:49,650 everything that's going on this plot one 221 00:07:52,400 --> 00:07:50,430 step at a time 222 00:07:55,580 --> 00:07:52,410 right here we're looking at the disk 223 00:07:57,830 --> 00:07:55,590 dust mass in Earth masses so 110 100 as 224 00:08:00,140 --> 00:07:57,840 a function of the disco stellar mass in 225 00:08:02,930 --> 00:08:00,150 solar masses so we have the solar type 226 00:08:04,490 --> 00:08:02,940 FG k stars here we've got the M dwarfs 227 00:08:06,530 --> 00:08:04,500 that really span a broad range of 228 00:08:09,380 --> 00:08:06,540 stellar masses and the brown dwarf 229 00:08:11,540 --> 00:08:09,390 regime demarcate adhere the red points 230 00:08:13,670 --> 00:08:11,550 are our new observations from Alma and 231 00:08:15,230 --> 00:08:13,680 the background points are the what was 232 00:08:17,150 --> 00:08:15,240 previously known for the rest of torus 233 00:08:18,560 --> 00:08:17,160 for the higher mass population can see 234 00:08:20,650 --> 00:08:18,570 that we're extending this well into the 235 00:08:22,910 --> 00:08:20,660 brown dwarf regime with these detection 236 00:08:24,560 --> 00:08:22,920 also plotted here for reference 237 00:08:27,050 --> 00:08:24,570 comparison in high Smulders talkie 238 00:08:29,930 --> 00:08:27,060 tooter are the heavy element masses that 239 00:08:32,390 --> 00:08:29,940 are metric from the capillarity km stars 240 00:08:34,820 --> 00:08:32,400 and what we've shown up here to kind of 241 00:08:35,990 --> 00:08:34,830 guide the eye is an estimate of what the 242 00:08:39,740 --> 00:08:36,000 minimum a solar nebula 243 00:08:41,000 --> 00:08:39,750 should be so we're saying that from what 244 00:08:43,159 --> 00:08:41,010 we know about the solar system what's 245 00:08:44,930 --> 00:08:43,169 required to form Jupiter and the planets 246 00:08:47,450 --> 00:08:44,940 in our solar system if you estimate that 247 00:08:50,810 --> 00:08:47,460 to be about 30 earth masses were suggest 248 00:08:52,580 --> 00:08:50,820 then you can demarcate this regime as 249 00:08:54,500 --> 00:08:52,590 whether or not your disks actually have 250 00:08:56,750 --> 00:08:54,510 enough solid material to kind of make it 251 00:08:59,000 --> 00:08:56,760 into this into this region and what we 252 00:09:00,350 --> 00:08:59,010 see is that the early under worse and of 253 00:09:02,390 --> 00:09:00,360 course the fgk stars are making into 254 00:09:04,310 --> 00:09:02,400 this region but due to this decline in 255 00:09:06,440 --> 00:09:04,320 dust masses we go to the lowest mass Co 256 00:09:07,790 --> 00:09:06,450 stars the lower mass M dwarfs and brown 257 00:09:09,770 --> 00:09:07,800 dwarfs really aren't making it up into 258 00:09:12,050 --> 00:09:09,780 this regime and this is providing some 259 00:09:14,000 --> 00:09:12,060 signature potentially explaining why 260 00:09:16,070 --> 00:09:14,010 direct imaging surveys have looked have 261 00:09:18,350 --> 00:09:16,080 really focused on the lowest mass M 262 00:09:21,110 --> 00:09:18,360 dwarfs to find directly imaged Jupiter 263 00:09:22,550 --> 00:09:21,120 analogues but it's been very very 264 00:09:23,900 --> 00:09:22,560 difficult to find movies directly image 265 00:09:27,440 --> 00:09:23,910 giant planets around the lowest mass 266 00:09:28,880 --> 00:09:27,450 stars and for reference because we're 267 00:09:30,770 --> 00:09:28,890 all very keen on understanding where 268 00:09:33,530 --> 00:09:30,780 Trappist 1 and similar systems these 269 00:09:35,420 --> 00:09:33,540 exciting new transiting m dwarf 270 00:09:37,880 --> 00:09:35,430 exoplanet systems live chopped this one 271 00:09:39,380 --> 00:09:37,890 is right here at the brown dwarf brown 272 00:09:41,570 --> 00:09:39,390 dwarfs regime and if you take the 273 00:09:43,610 --> 00:09:41,580 estimated masses and the planets from 274 00:09:45,710 --> 00:09:43,620 the most recent papers you can see it 275 00:09:47,540 --> 00:09:45,720 kind of fits here sort of at the top of 276 00:09:49,940 --> 00:09:47,550 that envelope so this is giving us some 277 00:09:51,170 --> 00:09:49,950 idea of maybe starting to look into 278 00:09:53,840 --> 00:09:51,180 things like planet formation if this 279 00:09:58,010 --> 00:09:53,850 efficiency of the dust masses into 280 00:09:59,870 --> 00:09:58,020 planetary bodies and one more thing that 281 00:10:02,030 --> 00:09:59,880 we can do with these data is we can look 282 00:10:03,590 --> 00:10:02,040 at comparison between the very young 1 283 00:10:05,570 --> 00:10:03,600 million year old tourists are from your 284 00:10:08,000 --> 00:10:05,580 region and that of upper Scorpius which 285 00:10:09,620 --> 00:10:08,010 is in the 510 million range and so we're 286 00:10:10,970 --> 00:10:09,630 looking at here again is the same axis 287 00:10:13,040 --> 00:10:10,980 Deaf's mass and Earth's mass earth 288 00:10:15,020 --> 00:10:13,050 masses versus the mass of the star the 289 00:10:16,700 --> 00:10:15,030 red points are all of the young Taurus 290 00:10:19,160 --> 00:10:16,710 populations and then these older 291 00:10:21,650 --> 00:10:19,170 population is shown here in teal points 292 00:10:22,820 --> 00:10:21,660 for older for schoo population and what 293 00:10:25,730 --> 00:10:22,830 we can see is there's about a factor of 294 00:10:26,990 --> 00:10:25,740 3 decrease in the dust mask content from 295 00:10:29,030 --> 00:10:27,000 1 million years to about 10 million 296 00:10:31,040 --> 00:10:29,040 years and so this is giving us some idea 297 00:10:32,930 --> 00:10:31,050 about potential time skills for planet 298 00:10:34,400 --> 00:10:32,940 formation as these submillimetre grains 299 00:10:37,430 --> 00:10:34,410 are converted into potentially larger 300 00:10:38,990 --> 00:10:37,440 bodies and also on I suggest that you 301 00:10:39,920 --> 00:10:39,000 look forward to Ilario stock where she's 302 00:10:42,080 --> 00:10:39,930 going to be doing more of these 303 00:10:46,070 --> 00:10:42,090 comparisons with other types of star 304 00:10:47,870 --> 00:10:46,080 forming regions okay so in summary from 305 00:10:50,690 --> 00:10:47,880 these two investigations into low mass 306 00:10:52,130 --> 00:10:50,700 stars we have the binary occurrence is 307 00:10:53,900 --> 00:10:52,140 lower for M dwarfs but they're closer 308 00:10:55,520 --> 00:10:53,910 and this is going to have important 309 00:10:57,470 --> 00:10:55,530 impact on our understanding of the 310 00:10:58,940 --> 00:10:57,480 properties of these systems if we go to 311 00:11:01,010 --> 00:10:58,950 the younger population and do some 312 00:11:02,210 --> 00:11:01,020 investigations in the submillimetre we 313 00:11:03,980 --> 00:11:02,220 see that there's not only the stuff 314 00:11:05,810 --> 00:11:03,990 depletion but we see significant 315 00:11:07,639 --> 00:11:05,820 we've decreased dust masses for the 316 00:11:09,410 --> 00:11:07,649 lowest mass stars and brown dwarfs and 317 00:11:10,910 --> 00:11:09,420 maybe this is helping us understand 318 00:11:13,490 --> 00:11:10,920 what's happening in terms of the giant 319 00:11:15,199 --> 00:11:13,500 planet population as well as what's 320 00:11:16,670 --> 00:11:15,209 going on for the younger analog 321 00:11:25,639 --> 00:11:16,680 environments for systems like Trappist 322 00:11:29,920 --> 00:11:25,649 thank you for your time all right we 323 00:11:45,280 --> 00:11:38,240 three minutes in fact please come to the 324 00:11:50,600 --> 00:11:48,590 Maggie toka Alera Pascucci I wanted to 325 00:11:52,610 --> 00:11:50,610 know when you say that to resolve the 326 00:11:55,699 --> 00:11:52,620 Browns of disks with Alma what was the 327 00:11:59,630 --> 00:11:55,709 beam that you had a beam was about point 328 00:12:01,850 --> 00:11:59,640 three 2.4 arc seconds and you always 329 00:12:03,470 --> 00:12:01,860 resolve the disc where you see origamis 330 00:12:04,850 --> 00:12:03,480 some are resolving some are unresolved 331 00:12:06,829 --> 00:12:04,860 and a quite a fear in this kind of 332 00:12:09,199 --> 00:12:06,839 marginal regime where they're only just 333 00:12:12,079 --> 00:12:09,209 resolved in the uv-plane okay all right 334 00:12:15,560 --> 00:12:12,089 so you can give a percentage erina Amish 335 00:12:17,150 --> 00:12:15,570 oh the fraction of systems um let's see 336 00:12:19,010 --> 00:12:17,160 it was actually a bit surprising that 337 00:12:20,690 --> 00:12:19,020 both the brown dwarfs and M dwarfs had 338 00:12:23,210 --> 00:12:20,700 kind of equal fractions of resolved 339 00:12:25,460 --> 00:12:23,220 disks which then again may say something 340 00:12:26,780 --> 00:12:25,470 about the formation processes that are 341 00:12:28,970 --> 00:12:26,790 undergoing in this different stellar 342 00:12:34,910 --> 00:12:28,980 masses of systems but kind of close to 343 00:12:36,710 --> 00:12:34,920 the 50 G's ffth percent range tadka 344 00:12:37,970 --> 00:12:36,720 masak university of arizona so when you 345 00:12:40,430 --> 00:12:37,980 showed that the M dwarf companion 346 00:12:41,269 --> 00:12:40,440 fraction was increasing towards closer 347 00:12:43,220 --> 00:12:41,279 separations 348 00:12:46,069 --> 00:12:43,230 that's from direct imaging of course so 349 00:12:50,000 --> 00:12:46,079 what about RV oh yeah yeah that's great 350 00:12:51,680 --> 00:12:50,010 so there's a section that mysterious gap 351 00:12:53,569 --> 00:12:51,690 within three au where we're not actually 352 00:12:56,269 --> 00:12:53,579 sensitive to companions is a perfect 353 00:12:58,130 --> 00:12:56,279 place to do the radial velocity and 354 00:13:00,050 --> 00:12:58,140 spectroscopic binary population and 355 00:13:01,610 --> 00:13:00,060 there hasn't been a comprehensive survey 356 00:13:03,560 --> 00:13:01,620 to look at like a volume limited sample 357 00:13:05,780 --> 00:13:03,570 in the same way but some preliminary 358 00:13:07,699 --> 00:13:05,790 estimates and some actually estimates 359 00:13:10,010 --> 00:13:07,709 from the kepler eclipsing binary sample 360 00:13:12,199 --> 00:13:10,020 place that even higher so maybe kind of 361 00:13:14,780 --> 00:13:12,209 closer to the like the 16% range at max 362 00:13:16,220 --> 00:13:14,790 but it's desperate for like a 363 00:13:19,180 --> 00:13:16,230 combination of all the techniques to 364 00:13:23,689 --> 00:13:21,680 absolutely thank you wait I had one 365 00:13:26,150 --> 00:13:23,699 Chris yeah I just wanted to know those 366 00:13:28,770 --> 00:13:26,160 deaths masses in the indoors are there 367 00:13:31,170 --> 00:13:28,780 any correlations with ages of the system 368 00:13:33,030 --> 00:13:31,180 yeah so we we looked at that and the 369 00:13:34,740 --> 00:13:33,040 ages are difficult the tourist is 370 00:13:36,240 --> 00:13:34,750 thought to have some spread in age not 371 00:13:39,900 --> 00:13:36,250 just to be one to two million years but 372 00:13:41,460 --> 00:13:39,910 also to have some intrinsic spread but 373 00:13:43,320 --> 00:13:41,470 from the values that were reported for 374 00:13:44,520 --> 00:13:43,330 the ages of the systems that we looked 375 00:13:47,280 --> 00:13:44,530 out there was no correlation between 376 00:13:49,950 --> 00:13:47,290 seeing the slightly older tourists have 377 00:13:51,660 --> 00:13:49,960 a lower desk population but the agents 378 00:13:53,280 --> 00:13:51,670 right knees are pretty big yeah okay 379 00:13:54,400 --> 00:13:53,290 thank you all right let's thank our