1 00:00:11,420 --> 00:00:09,020 alright great well I'm really excited to 2 00:00:13,160 --> 00:00:11,430 be following these talks because last 3 00:00:14,779 --> 00:00:13,170 few have concentrated on prebiotic 4 00:00:18,050 --> 00:00:14,789 chemistry in the early Earth and I want 5 00:00:21,350 --> 00:00:18,060 to go even earlier about this early in 6 00:00:23,630 --> 00:00:21,360 the formation of the earth so when I 7 00:00:26,170 --> 00:00:23,640 think about the life cycle I think on a 8 00:00:28,370 --> 00:00:26,180 more cosmic scale where we start with a 9 00:00:31,130 --> 00:00:28,380 protoplanetary nebula here which 10 00:00:33,680 --> 00:00:31,140 eventually as a star turns on collapses 11 00:00:36,920 --> 00:00:33,690 down to form a protoplanetary disk thin 12 00:00:38,959 --> 00:00:36,930 that disk you get condensation of dust 13 00:00:41,329 --> 00:00:38,969 grains and Isis into larger bodies 14 00:00:44,119 --> 00:00:41,339 comets asteroids planetesimals and 15 00:00:46,009 --> 00:00:44,129 eventually planets and then on those 16 00:00:47,630 --> 00:00:46,019 planets you eventually get the impact of 17 00:00:49,819 --> 00:00:47,640 a lot of the leftover comets and 18 00:00:52,189 --> 00:00:49,829 asteroids and at some point in this life 19 00:00:55,630 --> 00:00:52,199 cycle life is formed and then is 20 00:00:59,799 --> 00:00:55,640 destroyed in a fiery explosion and 21 00:01:05,329 --> 00:00:59,809 returned back into the cosmic lifecycle 22 00:01:08,480 --> 00:01:05,339 so we've heard a lot about getting life 23 00:01:10,070 --> 00:01:08,490 from say amino acids as a starting 24 00:01:12,470 --> 00:01:10,080 material and we all know that amino 25 00:01:15,410 --> 00:01:12,480 acids are found in comets from the start 26 00:01:17,240 --> 00:01:15,420 up mission or meteoritic samples but 27 00:01:19,070 --> 00:01:17,250 what we don't know in my field 28 00:01:20,390 --> 00:01:19,080 astrochemistry is how the heck those 29 00:01:22,160 --> 00:01:20,400 things got there in the first place 30 00:01:24,800 --> 00:01:22,170 there's been a lot of theories but 31 00:01:27,170 --> 00:01:24,810 there's no proof definitive proof of how 32 00:01:29,300 --> 00:01:27,180 those amino acids glycine being that the 33 00:01:33,050 --> 00:01:29,310 simplest and most abundant one we found 34 00:01:36,080 --> 00:01:33,060 got their start with so I'm interested 35 00:01:39,440 --> 00:01:36,090 in exactly where in this cycle from the 36 00:01:41,240 --> 00:01:39,450 protoplanetary nebula to even impact on 37 00:01:43,040 --> 00:01:41,250 the planet did glycine form that it 38 00:01:47,150 --> 00:01:43,050 formed the gas phase one of these two 39 00:01:49,610 --> 00:01:47,160 phases did it form in the icy surfaces 40 00:01:51,350 --> 00:01:49,620 of dust grains anywhere along this path 41 00:01:53,870 --> 00:01:51,360 or did you have to wait until you're in 42 00:01:55,400 --> 00:01:53,880 the bulk ice on comets or even there's 43 00:01:58,940 --> 00:01:55,410 been some theoretical papers that say if 44 00:02:01,070 --> 00:01:58,950 you smash a comment into the earth the 45 00:02:03,380 --> 00:02:01,080 heat of that impact can drive the 46 00:02:10,009 --> 00:02:03,390 formation of a whole bunch of organic 47 00:02:11,449 --> 00:02:10,019 molecules so last year I presented on 48 00:02:14,570 --> 00:02:11,459 the search for a molecule called 49 00:02:16,940 --> 00:02:14,580 hydroxylamine here n h 2o h and this was 50 00:02:19,140 --> 00:02:16,950 kind of the last gasp for trying to form 51 00:02:20,940 --> 00:02:19,150 glycine in the gas phase 52 00:02:22,380 --> 00:02:20,950 this reaction with acetic acid which is 53 00:02:26,429 --> 00:02:22,390 very abundant in the interstellar medium 54 00:02:28,050 --> 00:02:26,439 directly forms glycine and NH 2 H was 55 00:02:30,089 --> 00:02:28,060 predicted by us for chemical models to 56 00:02:32,460 --> 00:02:30,099 be quite abundant but as it turned out 57 00:02:34,140 --> 00:02:32,470 we couldn't find it at all in fact our 58 00:02:35,520 --> 00:02:34,150 upper limits were about a million times 59 00:02:38,429 --> 00:02:35,530 less than what was predicted by the 60 00:02:40,289 --> 00:02:38,439 theories and then some very recent 61 00:02:42,000 --> 00:02:40,299 theoretical work has said this reaction 62 00:02:44,339 --> 00:02:42,010 has a reaction berry and won't go in the 63 00:02:46,259 --> 00:02:44,349 gas phase in the is M anyways so that 64 00:02:48,059 --> 00:02:46,269 kind of Nyx's the formation of glycine 65 00:02:49,920 --> 00:02:48,069 in the gas phase as long as as far as 66 00:02:52,440 --> 00:02:49,930 we're concerned so that leaves us with 67 00:02:55,170 --> 00:02:52,450 the solid phase and just about four 68 00:02:57,960 --> 00:02:55,180 months ago a very talented astro 69 00:03:00,899 --> 00:02:57,970 chemical modeller Rob Garrard use a 70 00:03:04,410 --> 00:03:00,909 complex gas grain reaction Network to 71 00:03:07,440 --> 00:03:04,420 see if he could form glycine in the icy 72 00:03:09,360 --> 00:03:07,450 mantels of dust grains and in fact he 73 00:03:11,250 --> 00:03:09,370 finds yeah we can form it and then we 74 00:03:14,099 --> 00:03:11,260 can actually pop it off from those dust 75 00:03:16,860 --> 00:03:14,109 grains into the gas phase and use Alma 76 00:03:19,080 --> 00:03:16,870 our most sensitive radio telescope to 77 00:03:21,690 --> 00:03:19,090 detect it there's the signal the 78 00:03:24,300 --> 00:03:21,700 strongest signal from glycine towards a 79 00:03:27,750 --> 00:03:24,310 nearby star forming region that's really 80 00:03:30,000 --> 00:03:27,760 cool but the accuracy of these gas grain 81 00:03:31,559 --> 00:03:30,010 chemical networks relies necessarily on 82 00:03:33,270 --> 00:03:31,569 how well we know the starting parameters 83 00:03:35,460 --> 00:03:33,280 what's available to work within these 84 00:03:36,720 --> 00:03:35,470 Isis how much is there there of it and 85 00:03:40,319 --> 00:03:36,730 what's the temperature of these 86 00:03:41,759 --> 00:03:40,329 molecules and the problem is in Isis we 87 00:03:43,740 --> 00:03:41,769 know very little about what's actually 88 00:03:46,470 --> 00:03:43,750 there we think we know a lot but we have 89 00:03:48,839 --> 00:03:46,480 very little proof this is a list of 90 00:03:51,000 --> 00:03:48,849 detected molecules in Isis we know about 91 00:03:53,280 --> 00:03:51,010 a hundred and seventy or so molecules in 92 00:03:54,990 --> 00:03:53,290 the interstellar medium the ones that 93 00:03:56,610 --> 00:03:55,000 aren't in brackets are the only ones 94 00:03:58,500 --> 00:03:56,620 that are confirmed to be a nice as the 95 00:04:00,479 --> 00:03:58,510 ones in brackets we think we see what 96 00:04:02,640 --> 00:04:00,489 we're not certain and these are the 97 00:04:05,550 --> 00:04:02,650 major ice constituents you see here are 98 00:04:06,899 --> 00:04:05,560 actually quite simple molecules and the 99 00:04:08,399 --> 00:04:06,909 reason we're having so much trouble is 100 00:04:10,199 --> 00:04:08,409 because these observations are being 101 00:04:11,849 --> 00:04:10,209 done in the infrared the infrared is 102 00:04:14,369 --> 00:04:11,859 great for getting simple abundant 103 00:04:16,319 --> 00:04:14,379 molecules but it suffers a bit for a few 104 00:04:18,330 --> 00:04:16,329 reasons you have to do all of your 105 00:04:20,189 --> 00:04:18,340 observations in absorption for the most 106 00:04:22,800 --> 00:04:20,199 part which means that the ice that 107 00:04:24,480 --> 00:04:22,810 you're looking at behind it on a direct 108 00:04:26,640 --> 00:04:24,490 line of sight to us has to be a really 109 00:04:28,980 --> 00:04:26,650 bright source to absorb against that's 110 00:04:30,779 --> 00:04:28,990 usually a star and that really limits 111 00:04:32,730 --> 00:04:30,789 the number of places we can go looking 112 00:04:35,070 --> 00:04:32,740 for so our sample size is low too 113 00:04:37,469 --> 00:04:35,080 art with and the features in the 114 00:04:39,180 --> 00:04:37,479 infrared are usually broad and they 115 00:04:40,620 --> 00:04:39,190 blend together in these Isis and you 116 00:04:42,120 --> 00:04:40,630 really have to have an abundant molecule 117 00:04:44,580 --> 00:04:42,130 with distinct features to pick them out 118 00:04:45,990 --> 00:04:44,590 if you want to look in a mission that 119 00:04:48,330 --> 00:04:46,000 would be cool you wouldn't have to have 120 00:04:49,980 --> 00:04:48,340 a background star but the problem is if 121 00:04:51,689 --> 00:04:49,990 you want to fall on the part of the 122 00:04:54,240 --> 00:04:51,699 blackbody radiation curve where you can 123 00:04:56,490 --> 00:04:54,250 actually get light out of the grains in 124 00:04:58,290 --> 00:04:56,500 a detectable amount the grains have to 125 00:04:59,999 --> 00:04:58,300 be so hot that you can't have ice on 126 00:05:01,350 --> 00:05:00,009 them in the first place the other 127 00:05:02,999 --> 00:05:01,360 problem is the clouds that you're 128 00:05:04,710 --> 00:05:03,009 emitting from have such a high optical 129 00:05:06,960 --> 00:05:04,720 depth those photons just can't escape 130 00:05:10,170 --> 00:05:06,970 first part so you're kind of screwed for 131 00:05:11,999 --> 00:05:10,180 a mission and in the laboratory you're 132 00:05:13,499 --> 00:05:12,009 in directly measuring the optical 133 00:05:16,800 --> 00:05:13,509 constants that's n the index of 134 00:05:18,120 --> 00:05:16,810 refraction k the amount of absorption 135 00:05:20,610 --> 00:05:18,130 you get through here and these are 136 00:05:22,439 --> 00:05:20,620 really important for modelers who are 137 00:05:24,270 --> 00:05:22,449 looking at radiative transfer so how 138 00:05:28,320 --> 00:05:24,280 light gets through different layers of 139 00:05:29,939 --> 00:05:28,330 Isis say and unfortunately in directly 140 00:05:31,230 --> 00:05:29,949 measuring these in the infrared produces 141 00:05:33,180 --> 00:05:31,240 errors and those errors propagate 142 00:05:36,149 --> 00:05:33,190 through and make these calculations a 143 00:05:38,040 --> 00:05:36,159 little wishy-washy so what I want to do 144 00:05:39,540 --> 00:05:38,050 is see if we can get a little bit better 145 00:05:40,980 --> 00:05:39,550 by looking in the terahertz region of 146 00:05:43,140 --> 00:05:40,990 the spectrum so my background is in 147 00:05:46,920 --> 00:05:43,150 laboratory microwave spectroscopy and 148 00:05:48,959 --> 00:05:46,930 submillimetre spectroscopy and in space 149 00:05:51,180 --> 00:05:48,969 astronomical observations in absorption 150 00:05:53,430 --> 00:05:51,190 you don't need a background star to 151 00:05:55,409 --> 00:05:53,440 absorb in the terahertz the black and 152 00:05:57,029 --> 00:05:55,419 grey body radiation coming off of dust 153 00:05:58,770 --> 00:05:57,039 is sufficiently you can just absorb 154 00:06:00,450 --> 00:05:58,780 against the background continuum so we 155 00:06:03,540 --> 00:06:00,460 can look at a whole lot more place as a 156 00:06:05,219 --> 00:06:03,550 wider sample set and there might 157 00:06:06,809 --> 00:06:05,229 actually be some narrower features here 158 00:06:09,420 --> 00:06:06,819 and the terahertz features tend to be a 159 00:06:11,399 --> 00:06:09,430 little more distinct spectrally we can 160 00:06:13,709 --> 00:06:11,409 also look at a mission because the 161 00:06:15,469 --> 00:06:13,719 blackbody curve allows us to have colder 162 00:06:18,629 --> 00:06:15,479 ice grains that are emitting photons 163 00:06:20,010 --> 00:06:18,639 that we can see especially since there's 164 00:06:21,300 --> 00:06:20,020 a lower optical depth in the terahertz 165 00:06:24,290 --> 00:06:21,310 so they have a better chance of reaching 166 00:06:26,969 --> 00:06:24,300 us so we can look at their signals and 167 00:06:28,649 --> 00:06:26,979 we can also directly measure the optical 168 00:06:31,680 --> 00:06:28,659 constants so we get are so much higher 169 00:06:34,020 --> 00:06:31,690 accuracy and the terahertz so what's our 170 00:06:36,659 --> 00:06:34,030 experimental tech what's been done in 171 00:06:38,189 --> 00:06:36,669 the terahertz so far experimentally well 172 00:06:39,409 --> 00:06:38,199 some people have tried to cheat they 173 00:06:42,029 --> 00:06:39,419 take a Fourier transform infrared 174 00:06:43,890 --> 00:06:42,039 spectrometer and push it out of spec and 175 00:06:45,719 --> 00:06:43,900 then get all the way down to about three 176 00:06:48,119 --> 00:06:45,729 terahertz which is pretty good 177 00:06:50,820 --> 00:06:48,129 and they have fairly decent resolution 178 00:06:52,290 --> 00:06:50,830 about one wave number but you're still 179 00:06:54,059 --> 00:06:52,300 in directly measuring the optical 180 00:06:56,429 --> 00:06:54,069 constants and the work done so far has 181 00:06:59,659 --> 00:06:56,439 been largely on these known interstellar 182 00:07:01,709 --> 00:06:59,669 molecules so water methanol ammonia 183 00:07:04,920 --> 00:07:01,719 simple things that we already know are 184 00:07:06,540 --> 00:07:04,930 there so what we want to do is see if we 185 00:07:08,159 --> 00:07:06,550 can look at some more interesting 186 00:07:10,649 --> 00:07:08,169 molecules that we think have to be in 187 00:07:13,260 --> 00:07:10,659 these Isis to form glycine but we're not 188 00:07:15,179 --> 00:07:13,270 certain so we take a silicon substrate 189 00:07:17,909 --> 00:07:15,189 ins few millimeters thick and cool it 190 00:07:22,260 --> 00:07:17,919 down to between 10 and 150 Kelvin and an 191 00:07:24,929 --> 00:07:22,270 evacuated healing cryostat we spray gas 192 00:07:28,589 --> 00:07:24,939 phase molecules at it and they freeze 193 00:07:30,600 --> 00:07:28,599 into a layer of ice so this is a really 194 00:07:32,480 --> 00:07:30,610 simple technique and then we can shoot 195 00:07:35,369 --> 00:07:32,490 radiation through it so we have our own 196 00:07:37,529 --> 00:07:35,379 ftir here for diagnostic purposes and 197 00:07:38,969 --> 00:07:37,539 then we can shoot terahertz through the 198 00:07:43,170 --> 00:07:38,979 other way and we detect these signals 199 00:07:44,519 --> 00:07:43,180 and transfer them to absorption spectra 200 00:07:46,920 --> 00:07:44,529 so here's a layout of the actual 201 00:07:49,679 --> 00:07:46,930 spectrometer we have our silicon 202 00:07:52,350 --> 00:07:49,689 substrate here in our cryo set our ftir 203 00:07:54,360 --> 00:07:52,360 gets bounced in the way we generate our 204 00:07:55,920 --> 00:07:54,370 terahertz is actually really cool we 205 00:07:59,550 --> 00:07:55,930 take a really high-powered laser 206 00:08:01,350 --> 00:07:59,560 operating at 800 nanometers we frequency 207 00:08:03,300 --> 00:08:01,360 double some of the light so we have two 208 00:08:05,820 --> 00:08:03,310 colors of light going into our nitrogen 209 00:08:07,879 --> 00:08:05,830 purge box and then we focus it down if 210 00:08:10,170 --> 00:08:07,889 you focus it right it turns into a 211 00:08:13,079 --> 00:08:10,180 plasma in air it looks like a little 212 00:08:14,969 --> 00:08:13,089 miniature Sun and it's the oscillation 213 00:08:17,070 --> 00:08:14,979 of electrons back and forth in this 214 00:08:21,119 --> 00:08:17,080 plasma that emits a very broad very 215 00:08:22,529 --> 00:08:21,129 intense burst of terahertz radiation so 216 00:08:24,480 --> 00:08:22,539 we take that focus it through the sample 217 00:08:25,949 --> 00:08:24,490 and then detect it on the other side 218 00:08:27,480 --> 00:08:25,959 using what's called electro-optical 219 00:08:29,129 --> 00:08:27,490 rectification which is a really cool 220 00:08:31,320 --> 00:08:29,139 technique that I don't have time to talk 221 00:08:33,089 --> 00:08:31,330 about suffice it to say what it does is 222 00:08:35,370 --> 00:08:33,099 it directly measures the electric field 223 00:08:37,259 --> 00:08:35,380 of our pulse that's how we can get these 224 00:08:38,939 --> 00:08:37,269 optical constants out directly we don't 225 00:08:41,490 --> 00:08:38,949 have to do any Kramer's chromate kroenig 226 00:08:44,519 --> 00:08:41,500 analyses or other assumptions get these 227 00:08:47,220 --> 00:08:44,529 optical constants out right now we can 228 00:08:50,730 --> 00:08:47,230 cover from about 300 gigahertz to 7.5 229 00:08:52,710 --> 00:08:50,740 terahertz at modest resolution within 230 00:08:54,630 --> 00:08:52,720 the next few months we know we can get 231 00:08:56,879 --> 00:08:54,640 ourselves probably up to about 20 232 00:08:59,579 --> 00:08:56,889 terahertz in broadband but 233 00:09:02,400 --> 00:08:59,589 and down to about a factor of 10 better 234 00:09:03,869 --> 00:09:02,410 and resolution so this is what we've 235 00:09:05,669 --> 00:09:03,879 looked at so far we've had our 236 00:09:08,249 --> 00:09:05,679 instrument operating for about a little 237 00:09:10,979 --> 00:09:08,259 over a month at this level of efficiency 238 00:09:13,139 --> 00:09:10,989 we've done the simple Isis so far as 239 00:09:17,039 --> 00:09:13,149 well as methyl formate here which is a 240 00:09:18,539 --> 00:09:17,049 very well-known interstellar weed in a 241 00:09:20,189 --> 00:09:18,549 more complex molecule and we've also 242 00:09:21,929 --> 00:09:20,199 started to do some mixtures and I think 243 00:09:23,629 --> 00:09:21,939 my labmates back home have actually run 244 00:09:25,559 --> 00:09:23,639 a few more mixtures while I've been here 245 00:09:27,629 --> 00:09:25,569 so I'm just going to show you results 246 00:09:29,789 --> 00:09:27,639 from to hear the simplest and the most 247 00:09:31,859 --> 00:09:29,799 complex pure species we've run because 248 00:09:32,789 --> 00:09:31,869 their spectra they're cool to look at 249 00:09:34,259 --> 00:09:32,799 but they're all going to look kind of 250 00:09:37,259 --> 00:09:34,269 the same if I show you everything we've 251 00:09:40,349 --> 00:09:37,269 done so here's water the most abundant 252 00:09:42,059 --> 00:09:40,359 interstellar ice and what we have here 253 00:09:44,489 --> 00:09:42,069 are just three different thicknesses so 254 00:09:45,989 --> 00:09:44,499 we started putting down ice and we 255 00:09:48,210 --> 00:09:45,999 gradually increase the thickness and 256 00:09:50,759 --> 00:09:48,220 kept taking absorption spectra from 257 00:09:52,049 --> 00:09:50,769 about 300 gigahertz up to seven and a 258 00:09:54,239 --> 00:09:52,059 half terahertz and you can see here 259 00:09:56,249 --> 00:09:54,249 these nice distinct absorption features 260 00:09:57,509 --> 00:09:56,259 are growing in right out in the 261 00:10:00,150 --> 00:09:57,519 terahertz region that we're interested 262 00:10:01,739 --> 00:10:00,160 in it we can also tell the difference in 263 00:10:03,809 --> 00:10:01,749 the structure of the ice so if you 264 00:10:05,369 --> 00:10:03,819 deposit at a higher temperature there's 265 00:10:07,769 --> 00:10:05,379 energy for these molecules to move 266 00:10:11,249 --> 00:10:07,779 around and get into a formation that 267 00:10:12,900 --> 00:10:11,259 they like kristalyn if you deposit at a 268 00:10:15,150 --> 00:10:12,910 lower temperature say down at 10 Kelvin 269 00:10:17,220 --> 00:10:15,160 here they just stick in whatever way 270 00:10:19,859 --> 00:10:17,230 that they actually hit the ice and they 271 00:10:21,389 --> 00:10:19,869 they form an or morphus solid so you can 272 00:10:23,759 --> 00:10:21,399 see the difference in sharp distinct 273 00:10:27,179 --> 00:10:23,769 features versus a just kind of blobby 274 00:10:28,739 --> 00:10:27,189 thing here and the formation of this ice 275 00:10:31,109 --> 00:10:28,749 the weather its crystalline or amorphous 276 00:10:32,669 --> 00:10:31,119 is a big question in an astro chemistry 277 00:10:34,559 --> 00:10:32,679 right now it has a big impact on the way 278 00:10:36,840 --> 00:10:34,569 the molecules move around inside the ice 279 00:10:40,679 --> 00:10:36,850 to react the matrix that they have to 280 00:10:42,179 --> 00:10:40,689 work with so here's methyl formate it's 281 00:10:44,129 --> 00:10:42,189 the poster child for grain surface 282 00:10:46,710 --> 00:10:44,139 chemistry in the is em as far as we know 283 00:10:48,929 --> 00:10:46,720 we can't form this in the gas phase at 284 00:10:50,549 --> 00:10:48,939 all there's a whole whopping ton of it 285 00:10:52,019 --> 00:10:50,559 out there it pollutes our spector all 286 00:10:54,569 --> 00:10:52,029 the time and it has to be formed on the 287 00:10:56,340 --> 00:10:54,579 grain surfaces despite that there's no 288 00:10:57,809 --> 00:10:56,350 definitive detection of it or gneisses 289 00:11:01,139 --> 00:10:57,819 so if we can do that that would be 290 00:11:02,729 --> 00:11:01,149 fantastic and it's rather complex 291 00:11:03,929 --> 00:11:02,739 structure so maybe we can see some 292 00:11:06,210 --> 00:11:03,939 interesting features from it and the 293 00:11:07,799 --> 00:11:06,220 terahertz the same kind of plot we're 294 00:11:10,590 --> 00:11:07,809 just making the ice thicker and thicker 295 00:11:12,030 --> 00:11:10,600 as it grows in you can see here we got 296 00:11:13,590 --> 00:11:12,040 actually a lot more structure to the 297 00:11:15,629 --> 00:11:13,600 spectrum than we had in water and in 298 00:11:18,360 --> 00:11:15,639 different places which is fantastic for 299 00:11:20,370 --> 00:11:18,370 distinguishing things we can also look 300 00:11:23,009 --> 00:11:20,380 at crystal and versus amorphous again 301 00:11:24,600 --> 00:11:23,019 and you see here we're excited really 302 00:11:26,309 --> 00:11:24,610 excited about this spectra because these 303 00:11:28,170 --> 00:11:26,319 seem to be very sharp very distinct 304 00:11:29,400 --> 00:11:28,180 features even at low resolution so if 305 00:11:31,079 --> 00:11:29,410 you can imagine ten times better 306 00:11:32,759 --> 00:11:31,089 resolution on this and a couple months 307 00:11:36,329 --> 00:11:32,769 we think we're going to get some really 308 00:11:38,189 --> 00:11:36,339 interesting features here so where are 309 00:11:40,199 --> 00:11:38,199 we going next with this well we want to 310 00:11:42,809 --> 00:11:40,209 compare to the Herschel data archive and 311 00:11:44,519 --> 00:11:42,819 the spectra that are coming off of the 312 00:11:46,170 --> 00:11:44,529 almost science verification data these 313 00:11:48,180 --> 00:11:46,180 operate real near are interested 314 00:11:50,309 --> 00:11:48,190 frequency range these are 315 00:11:51,930 --> 00:11:50,319 state-of-the-art facilities and the data 316 00:11:52,860 --> 00:11:51,940 is all publicly available within the 317 00:11:55,470 --> 00:11:52,870 next year or two which would be 318 00:11:58,139 --> 00:11:55,480 fantastic ideally we'd like to operate 319 00:12:00,389 --> 00:11:58,149 with Sofia the Fifi instrument exactly 320 00:12:01,769 --> 00:12:00,399 mimics our frequency range and about the 321 00:12:04,860 --> 00:12:01,779 same resolution which would be fantastic 322 00:12:06,420 --> 00:12:04,870 but it hasn't come online yet science 323 00:12:07,740 --> 00:12:06,430 testing is just coming up for this new 324 00:12:09,689 --> 00:12:07,750 proposal cycle and they're offering 325 00:12:11,939 --> 00:12:09,699 seven and a half hours of which we're 326 00:12:14,160 --> 00:12:11,949 going to get none so we're going to have 327 00:12:16,530 --> 00:12:14,170 to wait a year to look at that but we're 328 00:12:18,090 --> 00:12:16,540 really excited because even these 329 00:12:19,679 --> 00:12:18,100 preliminary results show that we should 330 00:12:20,939 --> 00:12:19,689 be able to identify some more complex 331 00:12:23,670 --> 00:12:20,949 molecules and get a better understanding 332 00:12:26,730 --> 00:12:23,680 of what we have to work with to make 333 00:12:30,480 --> 00:12:26,740 glycine and other amino acids not on 334 00:12:32,550 --> 00:12:30,490 earth but before we got here with that 335 00:12:40,139 --> 00:12:32,560 sources of funding and acknowledgments 336 00:12:52,000 --> 00:12:40,149 and thank you for your attention all 337 00:12:57,560 --> 00:12:55,910 are you planning to propose of your 338 00:13:00,560 --> 00:12:57,570 observations for the next cycle or do 339 00:13:02,630 --> 00:13:00,570 you want to wait for working and 340 00:13:03,800 --> 00:13:02,640 commissioning Oh Fifi yeah we're gonna 341 00:13:06,590 --> 00:13:03,810 have to wait for the commissioning and 342 00:13:08,690 --> 00:13:06,600 safety to go online the great instrument 343 00:13:10,190 --> 00:13:08,700 theoretically covers a good frequency 344 00:13:12,380 --> 00:13:10,200 range but the windows they're offering 345 00:13:15,050 --> 00:13:12,390 are so small they cover maybe one or two 346 00:13:17,360 --> 00:13:15,060 of our resolution elements right now so 347 00:13:19,100 --> 00:13:17,370 it's just not a broadband enough system 348 00:13:20,990 --> 00:13:19,110 we'd love to use Fifi but we don't think 349 00:13:35,500 --> 00:13:21,000 we have a shot at seven and a half hours 350 00:13:40,790 --> 00:13:37,970 so I realize this is an incredibly long 351 00:13:43,190 --> 00:13:40,800 shot but what are the prospects if any 352 00:13:44,600 --> 00:13:43,200 for eventually ever detecting a chiral 353 00:13:48,140 --> 00:13:44,610 signature in this glycine or anything 354 00:13:50,720 --> 00:13:48,150 like that ah well I don't I don't know 355 00:13:53,840 --> 00:13:50,730 what how much to give away here there 356 00:13:56,510 --> 00:13:53,850 are there have been reports mumblings 357 00:13:59,330 --> 00:13:56,520 among my colleagues of some possible 358 00:14:00,590 --> 00:13:59,340 detection of some tyrol molecules most 359 00:14:02,720 --> 00:14:00,600 of these are just single line detection 360 00:14:03,860 --> 00:14:02,730 right now so that's just one spectral 361 00:14:05,840 --> 00:14:03,870 feature not enough to definitively 362 00:14:08,810 --> 00:14:05,850 identify anything but i would say 363 00:14:12,290 --> 00:14:08,820 especially with Alma coming online fully 364 00:14:13,880 --> 00:14:12,300 within the next year or so and we should 365 00:14:17,510 --> 00:14:13,890 we should see some detection of chiral 366 00:14:24,800 --> 00:14:17,520 molecules shortly I think awesome thank 367 00:14:28,340 --> 00:14:24,810 you yeah just to follow up can you there 368 00:14:30,530 --> 00:14:28,350 any ice topic ratio so you can go can we 369 00:14:34,580 --> 00:14:30,540 get isotopic ratios uh yeah absolutely 370 00:14:37,400 --> 00:14:34,590 um so I mean we pick up h2d ratios all 371 00:14:40,070 --> 00:14:37,410 the time and that's actually how we're 372 00:14:41,360 --> 00:14:40,080 trying not us but Astra chemical 373 00:14:44,510 --> 00:14:41,370 modelers are trying to understand the 374 00:14:45,590 --> 00:14:44,520 infall of water to former assoc from the 375 00:14:49,460 --> 00:14:45,600 different parts of forming 376 00:14:51,410 --> 00:14:49,470 protoplanetary disks carbon-12 carbon-13 377 00:14:54,290 --> 00:14:51,420 ratios are easy to pick up from carbon 378 00:14:59,480 --> 00:14:54,300 monoxide measurements as well as oxygen 379 00:15:00,920 --> 00:14:59,490 18 17 ratios yeah all right well if 380 00:15:02,329 --> 00:15:00,930 that's it can we give a hand for all