1 00:00:00,790 --> 00:00:07,320 [Music] 2 00:00:11,289 --> 00:00:09,240 [Applause] 3 00:00:12,879 --> 00:00:11,299 all right so today I'm going to talk to 4 00:00:15,730 --> 00:00:12,889 you about corals which is a laser 5 00:00:17,950 --> 00:00:15,740 desorption / ablation mass spectrometer 6 00:00:19,720 --> 00:00:17,960 if you had the opportunity to go to the 7 00:00:22,120 --> 00:00:19,730 workshop yesterday you would have heard 8 00:00:24,820 --> 00:00:22,130 me describe it grandly in one minute 9 00:00:25,960 --> 00:00:24,830 using arm wavy movements but today 10 00:00:28,960 --> 00:00:25,970 you're gonna actually see that it's a 11 00:00:30,550 --> 00:00:28,970 it's a real instrument so I normally 12 00:00:32,290 --> 00:00:30,560 start off when I try to talk about this 13 00:00:34,660 --> 00:00:32,300 particular instrument concept by 14 00:00:36,040 --> 00:00:34,670 advocating for mass spectrometry but 15 00:00:38,590 --> 00:00:36,050 Peter did that for me so I don't really 16 00:00:42,280 --> 00:00:38,600 have to do that right now I will kind of 17 00:00:45,970 --> 00:00:42,290 introduce maybe the evolutionary arc of 18 00:00:48,040 --> 00:00:45,980 mass analyzers so there's our variety of 19 00:00:50,260 --> 00:00:48,050 options when you want when you know you 20 00:00:53,529 --> 00:00:50,270 want to fly a mass spectrometer of types 21 00:00:55,240 --> 00:00:53,539 of mass filters that you can fly I'm a 22 00:00:57,100 --> 00:00:55,250 product of NASA Goddard so I'm 23 00:00:59,380 --> 00:00:57,110 intimately familiar with quadrupole mass 24 00:01:02,650 --> 00:00:59,390 spectrometry which has been surveying 25 00:01:04,749 --> 00:01:02,660 the solar system since pioneer Venus but 26 00:01:06,510 --> 00:01:04,759 we have sector field instruments that 27 00:01:08,859 --> 00:01:06,520 were before then in the Apollo era 28 00:01:12,160 --> 00:01:08,869 time-of-flight instruments from Vega 29 00:01:14,350 --> 00:01:12,170 Giotto Rosetta and then most more 30 00:01:16,089 --> 00:01:14,360 recently are the Paul type ion traps 31 00:01:17,199 --> 00:01:16,099 that were flown on Rosetta and then we 32 00:01:19,029 --> 00:01:17,209 heard a little bit about the Mars 33 00:01:22,180 --> 00:01:19,039 organic molecule analyzer the moma 34 00:01:24,430 --> 00:01:22,190 instrument onboard the ExoMars Rover so 35 00:01:26,980 --> 00:01:24,440 all of these systems have been qualified 36 00:01:29,440 --> 00:01:26,990 or have successfully successfully been 37 00:01:31,410 --> 00:01:29,450 deployed to a number of planetary 38 00:01:33,699 --> 00:01:31,420 environments so they're by definition 39 00:01:35,320 --> 00:01:33,709 heritage or legacy analyzers and they 40 00:01:37,109 --> 00:01:35,330 still bring a lot to the table and 41 00:01:39,490 --> 00:01:37,119 they're viable instruments for 42 00:01:41,830 --> 00:01:39,500 progressive future mission concepts 43 00:01:43,419 --> 00:01:41,840 they're relatively low cost because once 44 00:01:45,699 --> 00:01:43,429 you've flown at once you have a heritage 45 00:01:47,760 --> 00:01:45,709 designed to pull from they're relatively 46 00:01:51,370 --> 00:01:47,770 low risk because they've been shown to 47 00:01:53,080 --> 00:01:51,380 survive launch cruise deployment and we 48 00:01:55,479 --> 00:01:53,090 know what we get from them from a 49 00:01:58,029 --> 00:01:55,489 performance perspective however since 50 00:02:00,339 --> 00:01:58,039 the Apollo era for sector field 51 00:02:02,169 --> 00:02:00,349 instruments for example on there's been 52 00:02:04,120 --> 00:02:02,179 a lot of time and a lot of investment in 53 00:02:06,880 --> 00:02:04,130 advancing what I'm gonna call 54 00:02:08,979 --> 00:02:06,890 next-generation technologies that kind 55 00:02:11,979 --> 00:02:08,989 of are are pushing the forefront of the 56 00:02:14,260 --> 00:02:11,989 field forward this is my arbitrary way 57 00:02:17,020 --> 00:02:14,270 of designating how those technologies 58 00:02:19,600 --> 00:02:17,030 might be classified there are those that 59 00:02:21,940 --> 00:02:19,610 maybe use heritage analyzers but add 60 00:02:22,480 --> 00:02:21,950 something new to them to enhance the 61 00:02:25,690 --> 00:02:22,490 performance 62 00:02:27,730 --> 00:02:25,700 to extend the mass range to increase one 63 00:02:29,560 --> 00:02:27,740 performance metric or another but what 64 00:02:32,860 --> 00:02:29,570 I'm going to talk to you today about it 65 00:02:34,570 --> 00:02:32,870 are two key capabilities that I think we 66 00:02:36,970 --> 00:02:34,580 really need to focus in on especially in 67 00:02:39,400 --> 00:02:36,980 the astrobiology context and that's 68 00:02:41,410 --> 00:02:39,410 molecular disambiguation and when we're 69 00:02:43,690 --> 00:02:41,420 talking about a Europa Lander mission we 70 00:02:47,320 --> 00:02:43,700 need innovative sampling and ionization 71 00:02:49,630 --> 00:02:47,330 sources so here's a traditional mass 72 00:02:51,100 --> 00:02:49,640 spectrum those who have seen my 73 00:02:53,050 --> 00:02:51,110 presentations before notice I always 74 00:02:54,790 --> 00:02:53,060 seem to pick on this one but once you 75 00:02:57,430 --> 00:02:54,800 make an animation you want to kind of 76 00:02:59,710 --> 00:02:57,440 stick with it so this is a spectrum from 77 00:03:02,800 --> 00:02:59,720 one of the inbound flybys of the Cassini 78 00:03:04,420 --> 00:03:02,810 Asst this is Cassini I and M s and we 79 00:03:06,640 --> 00:03:04,430 have matched to charge ratio on the x 80 00:03:08,620 --> 00:03:06,650 axis and we have intensity on the Y and 81 00:03:11,890 --> 00:03:08,630 we see there are a bunch of features 82 00:03:14,380 --> 00:03:11,900 here and we have a good idea of what the 83 00:03:17,740 --> 00:03:14,390 primary constituents of these Peaks are 84 00:03:20,740 --> 00:03:17,750 because you know we can one way we can 85 00:03:22,900 --> 00:03:20,750 do is we can try to rebuild reproduce 86 00:03:25,690 --> 00:03:22,910 the relative abundances of these Peaks 87 00:03:27,790 --> 00:03:25,700 looking at diagnostic fragmentation 88 00:03:30,040 --> 00:03:27,800 patterns or isotopic abundances of 89 00:03:32,310 --> 00:03:30,050 plausible species underneath each of 90 00:03:35,410 --> 00:03:32,320 these some people in the room do this 91 00:03:37,090 --> 00:03:35,420 there are also you know when you're a 92 00:03:39,250 --> 00:03:37,100 spaceflight instrument usually you don't 93 00:03:41,530 --> 00:03:39,260 fly a single analytical instrument so 94 00:03:43,630 --> 00:03:41,540 you can have corroborated measurements 95 00:03:45,370 --> 00:03:43,640 from other complimentary payload 96 00:03:47,740 --> 00:03:45,380 instruments that can give you some 97 00:03:50,680 --> 00:03:47,750 insight into what these Peaks might be 98 00:03:52,900 --> 00:03:50,690 but we can't with 100% certainty say 99 00:03:55,000 --> 00:03:52,910 that there aren't at least some minor 100 00:03:58,090 --> 00:03:55,010 component of these Peaks could be a 101 00:04:00,400 --> 00:03:58,100 variety of molecular signatures as I 102 00:04:02,800 --> 00:04:00,410 said I'm kind of pushing for a laser 103 00:04:06,070 --> 00:04:02,810 ablation mass spectrometer so once you 104 00:04:08,470 --> 00:04:06,080 start adding more novel ionization 105 00:04:10,540 --> 00:04:08,480 sources then you start adding in organic 106 00:04:12,850 --> 00:04:10,550 isobaric interferences that you have to 107 00:04:14,110 --> 00:04:12,860 account for so the problems not going 108 00:04:15,910 --> 00:04:14,120 away it's actually getting a little bit 109 00:04:18,280 --> 00:04:15,920 more complicated with these advanced 110 00:04:20,740 --> 00:04:18,290 technologies so we have a bunch of ways 111 00:04:22,780 --> 00:04:20,750 that we can try to separate these 112 00:04:24,430 --> 00:04:22,790 signals that are potentially competing 113 00:04:26,140 --> 00:04:24,440 with one another we've done this 114 00:04:27,880 --> 00:04:26,150 historically by using things like gas 115 00:04:31,330 --> 00:04:27,890 chromatography which will use the 116 00:04:32,800 --> 00:04:31,340 affinity of competing molecules their 117 00:04:34,900 --> 00:04:32,810 affinity for the stationary phase to 118 00:04:35,680 --> 00:04:34,910 separate them out through time that's 119 00:04:36,220 --> 00:04:35,690 still viable 120 00:04:39,460 --> 00:04:36,230 the 121 00:04:40,990 --> 00:04:39,470 MoMA instrument uses a kind of a neat 122 00:04:43,950 --> 00:04:41,000 little tool called tandem mass 123 00:04:46,060 --> 00:04:43,960 spectrometry and that's where you can 124 00:04:48,340 --> 00:04:46,070 this one there you go 125 00:04:50,560 --> 00:04:48,350 you can see a peak of interest you may 126 00:04:52,450 --> 00:04:50,570 not know what it is exactly but you can 127 00:04:54,760 --> 00:04:52,460 eject the peaks that you're not 128 00:04:57,100 --> 00:04:54,770 interested in focus in on this one and 129 00:04:59,110 --> 00:04:57,110 intentionally break it apart to look at 130 00:05:01,000 --> 00:04:59,120 the structure of that molecule and to 131 00:05:03,220 --> 00:05:01,010 provide confidence and what you think it 132 00:05:05,890 --> 00:05:03,230 is and what I'm going to be pushing for 133 00:05:08,980 --> 00:05:05,900 today is what's called ultra-high mass 134 00:05:10,270 --> 00:05:08,990 resolution and that's where those Peaks 135 00:05:12,040 --> 00:05:10,280 that you saw on the previous slide 136 00:05:14,170 --> 00:05:12,050 becomes so skinny 137 00:05:15,840 --> 00:05:14,180 that you can actually elucidate the 138 00:05:17,710 --> 00:05:15,850 different components that might be 139 00:05:19,930 --> 00:05:17,720 competing with them so this is a 140 00:05:22,390 --> 00:05:19,940 Murchison sample we've heard you know 141 00:05:25,360 --> 00:05:22,400 number of talks have highlighted the 142 00:05:27,010 --> 00:05:25,370 complexity of Murchison sample but it 143 00:05:29,920 --> 00:05:27,020 just shows that within what looks like a 144 00:05:32,380 --> 00:05:29,930 single peak are a multitude of Peaks so 145 00:05:35,260 --> 00:05:32,390 if you're able to tickle out that that's 146 00:05:37,600 --> 00:05:35,270 dead at complexity than it really 147 00:05:40,000 --> 00:05:37,610 provides something so paul Mahaffey gave 148 00:05:42,460 --> 00:05:40,010 another kind of visual so I'm gonna give 149 00:05:45,580 --> 00:05:42,470 a different concept he he talked about a 150 00:05:47,770 --> 00:05:45,590 monatomic isobaric interference here we 151 00:05:49,060 --> 00:05:47,780 have a polyatomic so we have two organic 152 00:05:52,030 --> 00:05:49,070 compounds since we're talking about 153 00:05:55,960 --> 00:05:52,040 europa and with a lot of traditional 154 00:05:57,970 --> 00:05:55,970 instruments two peaks two distinct 155 00:05:59,860 --> 00:05:57,980 organic compounds might overlap with one 156 00:06:01,720 --> 00:05:59,870 another but as we progress towards 157 00:06:03,550 --> 00:06:01,730 higher and higher resolution instruments 158 00:06:06,160 --> 00:06:03,560 we're able to effectively separate them 159 00:06:10,210 --> 00:06:06,170 out without requiring an additional sub 160 00:06:12,490 --> 00:06:10,220 system like a chromatography system so 161 00:06:14,140 --> 00:06:12,500 the type of analyzer that I'm fighting 162 00:06:16,180 --> 00:06:14,150 you know advocating for here is called 163 00:06:17,860 --> 00:06:16,190 an orbit trap mass analyzer and the way 164 00:06:19,900 --> 00:06:17,870 it works is a little bit different than 165 00:06:23,110 --> 00:06:19,910 all of those heritage analyzers you have 166 00:06:25,870 --> 00:06:23,120 a source of ions and a pulse gets 167 00:06:27,760 --> 00:06:25,880 injected into this analyzer and they 168 00:06:30,310 --> 00:06:27,770 oscillate around this football-shaped 169 00:06:32,770 --> 00:06:30,320 electrode and the rate at which they 170 00:06:35,710 --> 00:06:32,780 oscillate maps to the mass-to-charge 171 00:06:38,080 --> 00:06:35,720 ratio of those species it's kind of neat 172 00:06:39,790 --> 00:06:38,090 for spaceflight not just because of the 173 00:06:42,460 --> 00:06:39,800 science products which is are these 174 00:06:45,010 --> 00:06:42,470 high-resolution mass spectra but there 175 00:06:47,130 --> 00:06:45,020 are no heavy magnets there are no RF 176 00:06:49,780 --> 00:06:47,140 supplies and there's actually no 177 00:06:50,020 --> 00:06:49,790 traditional detector assembly which is 178 00:06:51,910 --> 00:06:50,030 off 179 00:06:53,950 --> 00:06:51,920 considered a consumable for spaceflight 180 00:06:56,320 --> 00:06:53,960 applications and so you're able to start 181 00:06:58,540 --> 00:06:56,330 identifying what were previously 182 00:07:00,880 --> 00:06:58,550 isobaric species with the same nominal 183 00:07:03,040 --> 00:07:00,890 mass-to-charge ratio separating them out 184 00:07:06,070 --> 00:07:03,050 and that allows you to do you know some 185 00:07:07,570 --> 00:07:06,080 more quantitative metrics so what I want 186 00:07:10,000 --> 00:07:07,580 to do is to take that type of mass 187 00:07:13,480 --> 00:07:10,010 analyzer and integrate it with a laser 188 00:07:16,570 --> 00:07:13,490 source why a laser well there are a 189 00:07:20,440 --> 00:07:16,580 variety of reasons for it specific to 190 00:07:23,110 --> 00:07:20,450 Europa laser is access the less volatile 191 00:07:24,940 --> 00:07:23,120 the more refractory organics that may be 192 00:07:27,310 --> 00:07:24,950 embedded in the sample but they also 193 00:07:30,160 --> 00:07:27,320 allow us to break apart the inorganic 194 00:07:32,020 --> 00:07:30,170 phases so the salts and the other you 195 00:07:34,480 --> 00:07:32,030 know geological phases that may have 196 00:07:36,730 --> 00:07:34,490 been brought to the surface from ocean 197 00:07:38,860 --> 00:07:36,740 exchange can be accessed with these with 198 00:07:42,070 --> 00:07:38,870 these laser sources it doesn't require 199 00:07:43,960 --> 00:07:42,080 physical contact with the sample it 200 00:07:46,120 --> 00:07:43,970 provides spatially resolved measurements 201 00:07:48,700 --> 00:07:46,130 so you're limited the spatial resolution 202 00:07:51,580 --> 00:07:48,710 is only limited to the size of your your 203 00:07:53,650 --> 00:07:51,590 laser beam and a good example of some 204 00:07:56,170 --> 00:07:53,660 you know other benefits that it brings 205 00:07:58,120 --> 00:07:56,180 to the table are are highlighted by the 206 00:08:01,090 --> 00:07:58,130 moma instrument which will fly the first 207 00:08:03,940 --> 00:08:01,100 laser enabled mass spectrometry to space 208 00:08:06,190 --> 00:08:03,950 and so here we can see you know these 209 00:08:07,870 --> 00:08:06,200 are synthetic Mars analog samples but 210 00:08:11,680 --> 00:08:07,880 we've doped it with an organic compound 211 00:08:13,780 --> 00:08:11,690 and regardless of what the matrix is 212 00:08:16,870 --> 00:08:13,790 whether it's a single mineral of 213 00:08:19,540 --> 00:08:16,880 basaltic matrix or a phyllosilicate we 214 00:08:23,200 --> 00:08:19,550 can also add potentially degradation 215 00:08:25,750 --> 00:08:23,210 oxidative compounds in there and what 216 00:08:27,820 --> 00:08:25,760 otherwise might be you know might have 217 00:08:30,040 --> 00:08:27,830 induced the combustion of this organic 218 00:08:32,230 --> 00:08:30,050 because the pulse-width of a laser is so 219 00:08:34,450 --> 00:08:32,240 short we don't actually thermally alter 220 00:08:36,550 --> 00:08:34,460 the sample as much as a pyrolysis 221 00:08:40,330 --> 00:08:36,560 technique and so we're able to see that 222 00:08:42,340 --> 00:08:40,340 the primary molecule on top of that 223 00:08:44,020 --> 00:08:42,350 laser processing requires orders of 224 00:08:46,780 --> 00:08:44,030 magnitude less sample than traditional 225 00:08:50,770 --> 00:08:46,790 pyrolysis techniques and if you have the 226 00:08:52,660 --> 00:08:50,780 mass and available to fly maybe I'll 227 00:08:56,410 --> 00:08:52,670 call it an overqualified laser system if 228 00:08:58,180 --> 00:08:56,420 you have a high-energy laser system more 229 00:09:00,130 --> 00:08:58,190 than you need to maybe desorb some of 230 00:09:02,530 --> 00:09:00,140 these organics that also allows you to 231 00:09:03,129 --> 00:09:02,540 do a kind of pseudo tandem mass 232 00:09:05,439 --> 00:09:03,139 spectrometry 233 00:09:07,720 --> 00:09:05,449 so you can identify your organic at a 234 00:09:09,669 --> 00:09:07,730 low fluence and if you want to derive 235 00:09:11,619 --> 00:09:09,679 some of the structure if you want to try 236 00:09:13,379 --> 00:09:11,629 to identify if it's an isomer which 237 00:09:15,879 --> 00:09:13,389 which isomer it might be you can 238 00:09:18,249 --> 00:09:15,889 inundate it with more energy than you 239 00:09:20,169 --> 00:09:18,259 need to just see it intentionally break 240 00:09:25,590 --> 00:09:20,179 it up that way and give yourself some 241 00:09:27,909 --> 00:09:25,600 pseudo tandem mass spectrum so this 242 00:09:31,359 --> 00:09:27,919 orbit trap mass analyzer there's been a 243 00:09:34,269 --> 00:09:31,369 prototype in the in an overly oil France 244 00:09:36,099 --> 00:09:34,279 operational since maybe 2012 and so I 245 00:09:38,559 --> 00:09:36,109 had the opportunity to go out there a 246 00:09:40,299 --> 00:09:38,569 little over a year ago and that kind of 247 00:09:42,309 --> 00:09:40,309 serves as the proof of concept for the 248 00:09:44,799 --> 00:09:42,319 corrals instrument so I'm gonna say when 249 00:09:46,509 --> 00:09:44,809 you need to conform to the form fit and 250 00:09:50,499 --> 00:09:46,519 function of a flight instrument it 251 00:09:52,329 --> 00:09:50,509 certainly met the function we're 252 00:09:54,549 --> 00:09:52,339 building up this is a breadboard we have 253 00:09:55,989 --> 00:09:54,559 in operation now at NASA Goddard only 254 00:09:59,109 --> 00:09:55,999 brought online within the last couple of 255 00:10:00,789 --> 00:09:59,119 weeks and this the inside of this 256 00:10:02,199 --> 00:10:00,799 instrument looks just like with the 257 00:10:05,499 --> 00:10:02,209 corrals instrument wheel so this meets 258 00:10:07,869 --> 00:10:05,509 the form and the function but with this 259 00:10:10,419 --> 00:10:07,879 IC to opportunity and with negotiations 260 00:10:12,989 --> 00:10:10,429 going on with at JPL pre project team 261 00:10:16,329 --> 00:10:12,999 were designing this and we will be 262 00:10:17,979 --> 00:10:16,339 building and qualifying the an 263 00:10:20,039 --> 00:10:17,989 engineering test unit that meets the 264 00:10:23,079 --> 00:10:20,049 form fit and function of a flight model 265 00:10:24,850 --> 00:10:23,089 so we've we have a prototype of the 266 00:10:27,369 --> 00:10:24,860 laser operational so here's you know 267 00:10:30,039 --> 00:10:27,379 some of the performance metrics of that 268 00:10:32,289 --> 00:10:30,049 laser system it's hot again it's highly 269 00:10:33,970 --> 00:10:32,299 capable so it brings three times the 270 00:10:35,530 --> 00:10:33,980 energy per pulse that the moma laser 271 00:10:37,600 --> 00:10:35,540 does because we are interested in that 272 00:10:39,309 --> 00:10:37,610 in source decay and all of this put 273 00:10:41,369 --> 00:10:39,319 together should allow us to again 274 00:10:44,259 --> 00:10:41,379 measure the organic and the inorganic 275 00:10:48,549 --> 00:10:44,269 composition of samples delivered from 276 00:10:49,779 --> 00:10:48,559 the europa surface and so I just wanted 277 00:10:51,970 --> 00:10:49,789 to go over some of the data that we've 278 00:10:54,159 --> 00:10:51,980 collected recently so here's an example 279 00:10:56,739 --> 00:10:54,169 of a type of experiment we could run 280 00:10:58,960 --> 00:10:56,749 this is at the in the French laboratory 281 00:11:00,869 --> 00:10:58,970 so here we have magnesium sulfate salt 282 00:11:04,359 --> 00:11:00,879 before and after irradiation 283 00:11:07,299 --> 00:11:04,369 this salt was doped with an amino acid 284 00:11:10,090 --> 00:11:07,309 and so the power of this spectrum shows 285 00:11:11,799 --> 00:11:10,100 that this instrument meets our mass 286 00:11:13,840 --> 00:11:11,809 resolution requirements you can see our 287 00:11:16,239 --> 00:11:13,850 parts per million mass accuracy which is 288 00:11:16,690 --> 00:11:16,249 also critical because that gives you the 289 00:11:19,060 --> 00:11:16,700 molecular 290 00:11:20,710 --> 00:11:19,070 soit geometry but what I really like 291 00:11:23,530 --> 00:11:20,720 about this spectrum is that it shows the 292 00:11:25,390 --> 00:11:23,540 organics the primary molecule the the 293 00:11:26,920 --> 00:11:25,400 quintessential fragment you'll find this 294 00:11:30,310 --> 00:11:26,930 on the NIST database for an e i-- 295 00:11:32,110 --> 00:11:30,320 spectrum - as the dominant fragment and 296 00:11:33,610 --> 00:11:32,120 then the inorganic fraction you can even 297 00:11:35,590 --> 00:11:33,620 if you're a geologist you'll even see 298 00:11:38,830 --> 00:11:35,600 that we can get the isotopic composition 299 00:11:40,990 --> 00:11:38,840 of magnesium as well so we were curious 300 00:11:44,350 --> 00:11:41,000 you know what what are our limits of 301 00:11:46,150 --> 00:11:44,360 detection for example can we see organic 302 00:11:48,370 --> 00:11:46,160 compounds at the level that the moment 303 00:11:50,100 --> 00:11:48,380 instrument does which is at the one Pico 304 00:11:51,730 --> 00:11:50,110 mole per millimeter squared 305 00:11:54,340 --> 00:11:51,740 concentration level because it's a 306 00:11:56,830 --> 00:11:54,350 surface technique and so we kind of 307 00:11:58,780 --> 00:11:56,840 simulated a Europa Lander situation 308 00:12:00,760 --> 00:11:58,790 where we had in our case it was a 309 00:12:03,160 --> 00:12:00,770 solution that was allowed to dry down 310 00:12:05,110 --> 00:12:03,170 rather than an ice to sublimate but 311 00:12:07,570 --> 00:12:05,120 looking at the residue we were able to 312 00:12:09,700 --> 00:12:07,580 see a variety of organics this is just 313 00:12:12,420 --> 00:12:09,710 in positive mode but we're able to see 314 00:12:14,860 --> 00:12:12,430 the molecular ions of amino acids in 315 00:12:16,300 --> 00:12:14,870 this kind of context at the Pico mole 316 00:12:17,890 --> 00:12:16,310 per millimeter square mole so highly 317 00:12:19,810 --> 00:12:17,900 sensitive and again we're able to get 318 00:12:22,930 --> 00:12:19,820 isotopic abundances we heard that that's 319 00:12:24,220 --> 00:12:22,940 maybe not the top priority of a Europa 320 00:12:27,640 --> 00:12:24,230 Lander mission but it's something that 321 00:12:29,440 --> 00:12:27,650 we're able to deliver on as well so more 322 00:12:31,650 --> 00:12:29,450 work is being done looking at the 323 00:12:33,460 --> 00:12:31,660 capabilities of these progressive 324 00:12:35,530 --> 00:12:33,470 instruments that we're building with 325 00:12:37,990 --> 00:12:35,540 progressive levels of fidelity we're 326 00:12:40,570 --> 00:12:38,000 looking at how our fragmentation 327 00:12:42,100 --> 00:12:40,580 patterns they said if you over if you 328 00:12:43,900 --> 00:12:42,110 inundate the sample with excess energy 329 00:12:45,640 --> 00:12:43,910 you can intentionally fragment so we're 330 00:12:47,410 --> 00:12:45,650 looking at correlations between our 331 00:12:49,690 --> 00:12:47,420 fragmentation patterns with a laser 332 00:12:51,880 --> 00:12:49,700 source and how they map to the 333 00:12:54,270 --> 00:12:51,890 traditional misty eye mass spectrum 334 00:12:57,310 --> 00:12:54,280 we're looking at a variety of different 335 00:12:59,260 --> 00:12:57,320 you know compositions sample matrices so 336 00:13:01,150 --> 00:12:59,270 here's a an example for Thole ins which 337 00:13:04,570 --> 00:13:01,160 is apt given the announcement just an 338 00:13:07,090 --> 00:13:04,580 hour ago looking at inorganic phases so 339 00:13:09,280 --> 00:13:07,100 here we're looking at major and minor 340 00:13:15,820 --> 00:13:09,290 elements in a basaltic phase for example 341 00:13:17,590 --> 00:13:15,830 and doped with that's good it's also a 342 00:13:20,740 --> 00:13:17,600 pathfinder for more advanced instruments 343 00:13:22,790 --> 00:13:20,750 but with that I'll leave the conclusion 344 00:13:24,160 --> 00:13:22,800 slide up there 345 00:13:24,850 --> 00:13:24,170 [Applause] 346 00:13:27,990 --> 00:13:24,860 [Music] 347 00:13:28,200 --> 00:13:28,000 [Applause] 348 00:13:45,910 --> 00:13:28,210 [Music] 349 00:13:50,960 --> 00:13:49,670 so the high-mass range can be tuned for 350 00:13:53,450 --> 00:13:50,970 what is so with this type of mass 351 00:13:55,880 --> 00:13:53,460 analyzer you have windows that you can 352 00:13:57,500 --> 00:13:55,890 look at and the window is about 40 x 353 00:13:59,570 --> 00:13:57,510 from your lowest mass to your highest 354 00:14:02,930 --> 00:13:59,580 mass we can certainly see higher so our 355 00:14:04,130 --> 00:14:02,940 our corrals STM has a couple of modes 356 00:14:06,410 --> 00:14:04,140 defined so when we're looking at the 357 00:14:08,570 --> 00:14:06,420 inorganic fraction which might overwhelm 358 00:14:11,990 --> 00:14:08,580 the signal of trace organics we would 359 00:14:14,780 --> 00:14:12,000 look at from you know sodium Mass 23 up 360 00:14:16,370 --> 00:14:14,790 to maybe cut it off at 74 so we don't 361 00:14:20,030 --> 00:14:16,380 have glycine in there and then we could 362 00:14:22,340 --> 00:14:20,040 go from 75 up to 40 X that but it's 363 00:14:25,190 --> 00:14:22,350 actually tunable where you want but it 364 00:14:30,040 --> 00:14:25,200 needs to be 40 X the lowest mass is your 365 00:14:35,180 --> 00:14:32,120 where's the turnoff yeah so we had this 366 00:14:37,970 --> 00:14:35,190 conversation about what how large of a 367 00:14:41,930 --> 00:14:37,980 macro molecule can you analyze without a 368 00:14:44,330 --> 00:14:41,940 multi matrix and so that yeah without 369 00:14:46,160 --> 00:14:44,340 fragmenting it beyond recognition and so 370 00:14:48,380 --> 00:14:46,170 I think I told you this that we were 371 00:14:51,590 --> 00:14:48,390 measuring dye and tripeptides 372 00:14:52,910 --> 00:14:51,600 we haven't tested beyond that as of yet