1 00:00:12,250 --> 00:00:06,150 you 2 00:00:16,510 --> 00:00:14,670 [Music] 3 00:00:19,390 --> 00:00:16,520 alright that said I'm going to give you 4 00:00:22,530 --> 00:00:19,400 mixed messages because these are slides 5 00:00:26,320 --> 00:00:22,540 that I didn't prepare at all I'm giving 6 00:00:28,840 --> 00:00:26,330 giving this talk for Casey who reminded 7 00:00:30,760 --> 00:00:28,850 me that he's at a New Horizons team 8 00:00:32,799 --> 00:00:30,770 he'll be here later in the week and so 9 00:00:38,470 --> 00:00:32,809 that's fine and I'm happy to give your 10 00:00:39,820 --> 00:00:38,480 poster imagine my surprise when I open 11 00:00:42,310 --> 00:00:39,830 my emails and like oh I'm giving the 12 00:00:44,590 --> 00:00:42,320 talk okay so this is not the talk that I 13 00:00:46,090 --> 00:00:44,600 would give now I'm a co-author in the 14 00:00:48,880 --> 00:00:46,100 last one I barely know what this is 15 00:00:51,490 --> 00:00:48,890 about so I'm going to use this as a 16 00:00:53,530 --> 00:00:51,500 demonstration of some basic astronomy 17 00:00:57,549 --> 00:00:53,540 science concepts perhaps but also how 18 00:00:59,920 --> 00:00:57,559 not to prepare and get to talk this is 19 00:01:03,060 --> 00:00:59,930 ultimately I talked about some spectra 20 00:01:05,380 --> 00:01:03,070 that were required using the IRT F 21 00:01:07,450 --> 00:01:05,390 telescope facility in the specs 22 00:01:09,400 --> 00:01:07,460 instrument and I want to just talk about 23 00:01:11,440 --> 00:01:09,410 what those are and what we're doing with 24 00:01:13,749 --> 00:01:11,450 them in the near future 25 00:01:16,630 --> 00:01:13,759 and it's the main result so far has been 26 00:01:19,690 --> 00:01:16,640 to get better spectral types of the 27 00:01:23,920 --> 00:01:19,700 stars that we've observed and this is 28 00:01:25,210 --> 00:01:23,930 important for bio signatures because if 29 00:01:27,940 --> 00:01:25,220 you're going to understand the chemistry 30 00:01:30,460 --> 00:01:27,950 on a planet then you're going to need to 31 00:01:32,050 --> 00:01:30,470 know what chemical compositions that 32 00:01:32,950 --> 00:01:32,060 that planet was made out of and you're 33 00:01:35,200 --> 00:01:32,960 going to want to know what is the 34 00:01:37,179 --> 00:01:35,210 spectral type of the star which affects 35 00:01:38,289 --> 00:01:37,189 the spectrum that impinges on the planet 36 00:01:39,570 --> 00:01:38,299 and determines photochemistry 37 00:01:42,010 --> 00:01:39,580 so all these things are important 38 00:01:44,590 --> 00:01:42,020 instead of saying that I'm going to call 39 00:01:46,380 --> 00:01:44,600 this a very nerds I RTF specs I don't 40 00:01:49,380 --> 00:01:46,390 think there are enough acronyms so 41 00:01:52,510 --> 00:01:49,390 exosystem spectral characterization and 42 00:01:54,819 --> 00:01:52,520 put on a graph you can't really read 43 00:01:56,770 --> 00:01:54,829 okay alright so this is something you 44 00:02:01,569 --> 00:01:56,780 should probably not do is give a list of 45 00:02:04,749 --> 00:02:01,579 things and you can't read and especially 46 00:02:06,280 --> 00:02:04,759 to start off with the list which I think 47 00:02:08,560 --> 00:02:06,290 I should just start with the conclusions 48 00:02:10,630 --> 00:02:08,570 which is that we can type the spectral 49 00:02:12,880 --> 00:02:10,640 types of stars much better using this 50 00:02:16,810 --> 00:02:12,890 infrared spectra where you need somebody 51 00:02:19,030 --> 00:02:16,820 to help us extract chemical abundances 52 00:02:19,990 --> 00:02:19,040 from these IR spectra and we'll show 53 00:02:22,479 --> 00:02:20,000 some of those results 54 00:02:23,949 --> 00:02:22,489 but instead Casey chose to say hey we 55 00:02:24,230 --> 00:02:23,959 got some new observing time and we're 56 00:02:27,290 --> 00:02:24,240 going 57 00:02:30,320 --> 00:02:27,300 - look at these host stars of in the 58 00:02:33,260 --> 00:02:30,330 infrared a few microns emission from 16 59 00:02:35,240 --> 00:02:33,270 of the best Kepler host stars with 60 00:02:37,460 --> 00:02:35,250 planets in the terrestrial habitable 61 00:02:39,200 --> 00:02:37,470 zone we're going to be observing these 62 00:02:40,490 --> 00:02:39,210 stars in June and we're going to get 63 00:02:42,650 --> 00:02:40,500 more data like the rest of the data 64 00:02:43,700 --> 00:02:42,660 you're going to see and we want to know 65 00:02:45,770 --> 00:02:43,710 what can we expect from these 66 00:02:47,240 --> 00:02:45,780 measurements and then we're going to 67 00:02:49,670 --> 00:02:47,250 look at some of the measurements we've 68 00:02:51,410 --> 00:02:49,680 already taken okay so this is all part 69 00:02:56,530 --> 00:02:51,420 of a survey that Casey's been involved 70 00:02:58,790 --> 00:02:56,540 with culty nerds it's 50 plus nerds 71 00:03:02,600 --> 00:02:58,800 targets so it sounds like senior 72 00:03:04,580 --> 00:03:02,610 scientist doesn't it yeah we have 73 00:03:06,800 --> 00:03:04,590 observed a number of systems that have 74 00:03:10,550 --> 00:03:06,810 some sort of circumstellar material and 75 00:03:13,310 --> 00:03:10,560 the infrared from about 0.8 microns to 5 76 00:03:17,360 --> 00:03:13,320 microns spectral resolution about a 77 00:03:19,970 --> 00:03:17,370 thousand to 2,000 with some pretty good 78 00:03:21,950 --> 00:03:19,980 photometry gives us some new interesting 79 00:03:27,620 --> 00:03:21,960 windows into what these spectral types 80 00:03:28,940 --> 00:03:27,630 are like so these graphs don't don't 81 00:03:30,530 --> 00:03:28,950 look at the middle one because you know 82 00:03:33,620 --> 00:03:30,540 that you can read that's the one you 83 00:03:35,930 --> 00:03:33,630 don't want to look at is yeah this is 84 00:03:38,090 --> 00:03:35,940 ridiculous do not ever kids don't put in 85 00:03:40,760 --> 00:03:38,100 a graph just puts labels that they're 86 00:03:42,740 --> 00:03:40,770 too small to read even on my laptop I 87 00:03:44,240 --> 00:03:42,750 can't even read them on your laptop he's 88 00:03:47,200 --> 00:03:44,250 just trying to say though we can get 89 00:03:52,810 --> 00:03:47,210 data and they kind of look like this and 90 00:03:58,970 --> 00:03:56,180 okay so the first thing we need to do is 91 00:04:01,310 --> 00:03:58,980 to figure out the spectral types of 92 00:04:02,360 --> 00:04:01,320 stars you'd think we could know this you 93 00:04:09,580 --> 00:04:02,370 guys are all familiar with spectral 94 00:04:12,890 --> 00:04:09,590 types oba FG km/l T and the mnemonic 95 00:04:14,990 --> 00:04:12,900 yeah and why right so only boring 96 00:04:20,199 --> 00:04:15,000 astronomers find gratification knowing 97 00:04:24,740 --> 00:04:23,330 so these are the different spectral 98 00:04:26,990 --> 00:04:24,750 types in the spectra that you can get of 99 00:04:28,939 --> 00:04:27,000 comparable quality to the spectra that 100 00:04:30,710 --> 00:04:28,949 we've obtained in the infrared you can 101 00:04:32,480 --> 00:04:30,720 see how many features that are and you 102 00:04:35,210 --> 00:04:32,490 can use these spectral features in these 103 00:04:37,640 --> 00:04:35,220 absorption lines to type them Rainer at 104 00:04:41,210 --> 00:04:37,650 all 2009 have done this for 200 stars 105 00:04:46,400 --> 00:04:41,220 f G M and K stars hey why should it be 106 00:04:49,430 --> 00:04:46,410 FG km don't you think FG m k okay so and 107 00:04:51,170 --> 00:04:49,440 they have been able to get em basically 108 00:04:52,700 --> 00:04:51,180 characterize the Stars based on the 109 00:04:54,650 --> 00:04:52,710 equivalent widths the depths of those 110 00:04:57,710 --> 00:04:54,660 absorption features that specific ones 111 00:05:01,060 --> 00:04:57,720 and build up a library of stars and and 112 00:05:03,350 --> 00:05:01,070 we have taken these stars and the colors 113 00:05:07,969 --> 00:05:03,360 obviously is from the legend that's at 114 00:05:10,340 --> 00:05:07,979 the bottom on the next slide so we have 115 00:05:12,860 --> 00:05:10,350 disks we have stars with disk we have 116 00:05:14,930 --> 00:05:12,870 stars with circumstellar material that 117 00:05:17,719 --> 00:05:14,940 seems to have followed a giant impact we 118 00:05:20,540 --> 00:05:17,729 have disk that of a planet observing the 119 00:05:22,340 --> 00:05:20,550 system or just hot dust anyway there are 120 00:05:28,340 --> 00:05:22,350 these different types of systems all 121 00:05:31,640 --> 00:05:28,350 with different circumstances 122 00:05:33,320 --> 00:05:31,650 okay we can characterize these obviously 123 00:05:36,549 --> 00:05:33,330 you need all this other information as 124 00:05:43,269 --> 00:05:41,159 okay so here are some representative 125 00:05:46,689 --> 00:05:43,279 spectra that we've taken so here's 126 00:05:49,239 --> 00:05:46,699 here's the important thing you need to 127 00:05:51,699 --> 00:05:49,249 ignore this graph you need to look at 128 00:05:53,679 --> 00:05:51,709 this one first so the first thing we do 129 00:05:56,769 --> 00:05:53,689 is we need to characterize the depth of 130 00:05:59,679 --> 00:05:56,779 the absorption features in particular 131 00:06:01,329 --> 00:05:59,689 wavelength and to know the depth of an 132 00:06:03,249 --> 00:06:01,339 absorption feature of course you want to 133 00:06:04,959 --> 00:06:03,259 know how much is that particular atomic 134 00:06:07,479 --> 00:06:04,969 transition absorbing out of the 135 00:06:09,159 --> 00:06:07,489 continuum starlight and to do that you 136 00:06:11,079 --> 00:06:09,169 need to know the continuum starlight and 137 00:06:12,609 --> 00:06:11,089 it's a real challenge in the infrared 138 00:06:14,589 --> 00:06:12,619 because there are so many spectral 139 00:06:16,779 --> 00:06:14,599 features that it's very hard to even fit 140 00:06:18,729 --> 00:06:16,789 a continuum and so you have to use 141 00:06:20,889 --> 00:06:18,739 smoothing of a spectrum to get a 142 00:06:22,659 --> 00:06:20,899 continuum like this then you can start 143 00:06:26,979 --> 00:06:22,669 to look at specific absorption features 144 00:06:29,739 --> 00:06:26,989 and get the depth of those features and 145 00:06:32,819 --> 00:06:29,749 now these are six atomic lines these two 146 00:06:36,579 --> 00:06:32,829 are magnesium these two are sodium and 147 00:06:39,099 --> 00:06:36,589 these are the depth of the absorption 148 00:06:41,609 --> 00:06:39,109 the equivalent widths as a function of 149 00:06:44,019 --> 00:06:41,619 the spectral type which is mostly just 150 00:06:46,899 --> 00:06:44,029 temperature here which is basically : K 151 00:06:48,879 --> 00:06:46,909 or M or whatever as a function of 152 00:06:50,979 --> 00:06:48,889 temperature but it turns out it's 153 00:06:53,289 --> 00:06:50,989 different if you're talking about a K 154 00:06:55,659 --> 00:06:53,299 star on the main sequence or if you're 155 00:06:58,209 --> 00:06:55,669 talking about a K star that is a giant 156 00:07:00,249 --> 00:06:58,219 star and so these red curves are showing 157 00:07:02,589 --> 00:07:00,259 what that library from Rainer at all 158 00:07:05,919 --> 00:07:02,599 2009 says are the equivalent widths if 159 00:07:07,929 --> 00:07:05,929 you're talking about K dwarfs G dwarfs 160 00:07:09,279 --> 00:07:07,939 etc and the blue and green lines are 161 00:07:13,599 --> 00:07:09,289 what those equivalents would be if 162 00:07:16,029 --> 00:07:13,609 you're talking about K Giants and so by 163 00:07:19,479 --> 00:07:16,039 looking at the equivalent width in a 164 00:07:21,789 --> 00:07:19,489 spectrum matching them to spectral types 165 00:07:23,319 --> 00:07:21,799 you can get some information about 166 00:07:25,449 --> 00:07:23,329 whether you're looking at a giant if it 167 00:07:28,389 --> 00:07:25,459 lines with the blue green bars here or 168 00:07:30,009 --> 00:07:28,399 red and it's important to do this in 169 00:07:32,139 --> 00:07:30,019 multiple lines because if you look at an 170 00:07:33,999 --> 00:07:32,149 equivalent with you could have it 171 00:07:35,949 --> 00:07:34,009 matching at this spectral type or this 172 00:07:41,439 --> 00:07:35,959 spectral type but it's not going to work 173 00:07:43,359 --> 00:07:41,449 that way for all of these stars and with 174 00:07:46,600 --> 00:07:43,369 with all of those lines so by looking at 175 00:07:48,700 --> 00:07:46,610 a multiple of multiplicity of lines you 176 00:07:50,500 --> 00:07:48,710 can get exact spectral types 177 00:07:54,430 --> 00:07:50,510 so it turns out that there was a star 178 00:07:56,650 --> 00:07:54,440 that type of 3 162 that was classified 179 00:07:59,890 --> 00:07:56,660 previously as a main-sequence star of a 180 00:08:03,490 --> 00:07:59,900 k4 to k7 type but instead it turns out 181 00:08:05,020 --> 00:08:03,500 to be K 2 class 3 giant and so this is 182 00:08:07,870 --> 00:08:05,030 very important that's not a star you 183 00:08:09,970 --> 00:08:07,880 would want to look for life around so 184 00:08:13,300 --> 00:08:09,980 this sort of basic work is very 185 00:08:17,080 --> 00:08:13,310 important to do and especially in the 186 00:08:19,090 --> 00:08:17,090 infrared here okay we can also look at 187 00:08:20,980 --> 00:08:19,100 emission lines that was absorption lines 188 00:08:23,830 --> 00:08:20,990 and we can look at equivalent widths of 189 00:08:25,870 --> 00:08:23,840 emission lines in a similar way and you 190 00:08:27,520 --> 00:08:25,880 can find out other information but in 191 00:08:31,870 --> 00:08:27,530 case you didn't tell me what happens 192 00:08:34,180 --> 00:08:31,880 here I'm going to skip that okay now 193 00:08:35,920 --> 00:08:34,190 another feature of the infrared is that 194 00:08:38,260 --> 00:08:35,930 you can start to look for circumstellar 195 00:08:41,560 --> 00:08:38,270 gas as well as dust and so first we want 196 00:08:43,990 --> 00:08:41,570 to talk about gas and in this wavelength 197 00:08:46,360 --> 00:08:44,000 range you have these overtones from Co 198 00:08:50,140 --> 00:08:46,370 emission and we do see this in a number 199 00:08:52,270 --> 00:08:50,150 of systems as you can read which system 200 00:08:55,300 --> 00:08:52,280 we're talking about here ok that's 201 00:08:57,040 --> 00:08:55,310 actually a reference that's ANOVA which 202 00:09:00,280 --> 00:08:57,050 is known to have Co emission and then 203 00:09:01,960 --> 00:09:00,290 this is 5100 which is a system plant 204 00:09:03,370 --> 00:09:01,970 information and it also is showing some 205 00:09:04,600 --> 00:09:03,380 CEOs or from solar got so that's 206 00:09:07,510 --> 00:09:04,610 something interesting that we can get 207 00:09:12,100 --> 00:09:07,520 out of the spectra and sometimes we see 208 00:09:14,560 --> 00:09:12,110 see own absorption as well so ha ok so 209 00:09:16,210 --> 00:09:14,570 this is 50 100 and it's showing Co a 210 00:09:18,280 --> 00:09:16,220 mission and you put that here to show 211 00:09:22,330 --> 00:09:18,290 you that we're seeing absorption of 212 00:09:24,190 --> 00:09:22,340 radiation from foreground material in 213 00:09:26,800 --> 00:09:24,200 front of some of these stars at exactly 214 00:09:29,650 --> 00:09:26,810 the wavelength that we see Co emission 215 00:09:31,270 --> 00:09:29,660 so we are seeing CEO absorption in front 216 00:09:36,130 --> 00:09:31,280 of some of these stars what does it mean 217 00:09:39,130 --> 00:09:36,140 I don't know but we're seeing it ok so 218 00:09:40,750 --> 00:09:39,140 now these are it don't you love it when 219 00:09:42,370 --> 00:09:40,760 a speaker gives up and what a pleasant 220 00:09:44,130 --> 00:09:42,380 surprise look at this slide I didn't 221 00:09:49,860 --> 00:09:44,140 know that was there ok 222 00:09:52,800 --> 00:09:49,870 this is a infrared spectra of F a F G 223 00:09:56,460 --> 00:09:52,810 and K stars and showing that a number of 224 00:09:59,340 --> 00:09:56,470 these systems show not just CEO emission 225 00:10:02,970 --> 00:09:59,350 access but actual continuum infrared 226 00:10:05,940 --> 00:10:02,980 emission excesses at four to five 227 00:10:08,460 --> 00:10:05,950 microns showing that there is dust in 228 00:10:12,960 --> 00:10:08,470 those systems that is emitting engineer 229 00:10:14,550 --> 00:10:12,970 for red and we can compare that to these 230 00:10:16,860 --> 00:10:14,560 same systems we can look at the infrared 231 00:10:19,610 --> 00:10:16,870 spectra at longer wavelengths okay and 232 00:10:25,050 --> 00:10:19,620 it turns out some of these systems have 233 00:10:27,090 --> 00:10:25,060 you can see which ones they they have 234 00:10:29,550 --> 00:10:27,100 they have cold emission in the farm Fred 235 00:10:31,560 --> 00:10:29,560 this is Spitzer data overlaid on these 236 00:10:33,480 --> 00:10:31,570 same systems with the specs data we've 237 00:10:35,670 --> 00:10:33,490 got so some of these dusty systems are 238 00:10:38,009 --> 00:10:35,680 indeed showing dust out in the Kuiper 239 00:10:41,069 --> 00:10:38,019 belt regions or in the mid infrared 240 00:10:42,780 --> 00:10:41,079 region so at one a you they emit in the 241 00:10:45,090 --> 00:10:42,790 mid infrared and you're seeing silicates 242 00:10:47,250 --> 00:10:45,100 or silica hot rock may be due to 243 00:10:49,319 --> 00:10:47,260 planetary collisions generating silica 244 00:10:52,980 --> 00:10:49,329 and then in other systems with planets 245 00:10:55,199 --> 00:10:52,990 we see Co emission and put HL tau here 246 00:10:58,980 --> 00:10:55,209 but HL tau is not in one of these and so 247 00:11:01,949 --> 00:10:58,990 let me go to the conclusions then got a 248 00:11:04,259 --> 00:11:01,959 lot of spectra from the Nerds survey 249 00:11:06,090 --> 00:11:04,269 they use the equivalent which measures 250 00:11:08,610 --> 00:11:06,100 at particular wavelengths of line to do 251 00:11:10,769 --> 00:11:08,620 better spectral typing of the stars but 252 00:11:13,110 --> 00:11:10,779 what we haven't done yet is converted 253 00:11:14,670 --> 00:11:13,120 the spectra into abundances high 254 00:11:17,069 --> 00:11:14,680 precision abundances of these species 255 00:11:19,069 --> 00:11:17,079 and whatever other things are emitting 256 00:11:22,319 --> 00:11:19,079 infrared and that would include a 257 00:11:24,120 --> 00:11:22,329 phosphorus I think so we are looking for 258 00:11:27,180 --> 00:11:24,130 people to help us do the spectral 259 00:11:29,639 --> 00:11:27,190 modeling of the spectra and in the 260 00:11:31,439 --> 00:11:29,649 infrared to get cellar abundances and I 261 00:11:36,020 --> 00:11:31,449 will stop there before I commit more 262 00:11:48,990 --> 00:11:38,100 we have time for a couple questions 263 00:11:53,550 --> 00:11:49,000 couple quick questions please I will 264 00:11:55,320 --> 00:11:53,560 text Katie okay though I should have 265 00:11:56,010 --> 00:11:55,330 practiced the talk but I was I don't 266 00:11:58,860 --> 00:11:56,020 know what I was doing 267 00:12:00,070 --> 00:11:58,870 okay thank you all right let's give our