1 00:00:00,220 --> 00:00:12,940 [Music] 2 00:00:16,190 --> 00:00:15,080 so I met salim a graduate student at 3 00:00:18,830 --> 00:00:16,200 University of Washington working with 4 00:00:20,090 --> 00:00:18,840 the vdl and recently we did a project to 5 00:00:21,410 --> 00:00:20,100 see if we could constrain anything about 6 00:00:23,600 --> 00:00:21,420 Proxima Centauri be looking at the 7 00:00:25,280 --> 00:00:23,610 overall emission specifically the five 8 00:00:27,500 --> 00:00:25,290 five seven seven a green line which you 9 00:00:28,760 --> 00:00:27,510 can see here this beautiful image so a 10 00:00:30,109 --> 00:00:28,770 little review about Aurora they are 11 00:00:31,850 --> 00:00:30,119 driven by star planet interaction 12 00:00:33,350 --> 00:00:31,860 typically you have some forcing from the 13 00:00:35,180 --> 00:00:33,360 stellar wind or a transient activity 14 00:00:36,890 --> 00:00:35,190 like what you see here in this cartoon 15 00:00:38,720 --> 00:00:36,900 which compresses the magnetosphere 16 00:00:40,580 --> 00:00:38,730 energizes particles and causes a lot of 17 00:00:41,750 --> 00:00:40,590 interesting physics but what you get in 18 00:00:43,220 --> 00:00:41,760 the end is the precipitation of 19 00:00:45,020 --> 00:00:43,230 particles down into the atmosphere along 20 00:00:47,810 --> 00:00:45,030 the magnetic field and forms these 21 00:00:48,979 --> 00:00:47,820 beautiful bands of color and around in 22 00:00:50,630 --> 00:00:48,989 forms it's a royal oval that we are 23 00:00:53,599 --> 00:00:50,640 where this characteristic a little years 24 00:00:55,430 --> 00:00:53,609 to seeing and so in general I want to 25 00:00:56,930 --> 00:00:55,440 point out that we are looking for Aurora 26 00:00:58,970 --> 00:00:56,940 airglow so we're looking for these 27 00:01:00,799 --> 00:00:58,980 discrete localized and intense emissions 28 00:01:02,330 --> 00:01:00,809 coming from the planet where don't care 29 00:01:04,430 --> 00:01:02,340 about air glow it's a little too faint 30 00:01:06,710 --> 00:01:04,440 we could put our calculations in oh 31 00:01:07,730 --> 00:01:06,720 there's no real chance to see that at 32 00:01:12,160 --> 00:01:07,740 least with present instruments and 33 00:01:15,950 --> 00:01:14,210 so we want a really good star planet 34 00:01:18,020 --> 00:01:15,960 contrast luckily Proxima Centauri is an 35 00:01:19,039 --> 00:01:18,030 indoor so it's beneficial to look in the 36 00:01:20,749 --> 00:01:19,049 optical region if we want to see 37 00:01:24,350 --> 00:01:20,759 something from the planet so the harps 38 00:01:26,660 --> 00:01:24,360 data you can see here yes here check it 39 00:01:28,160 --> 00:01:26,670 in blue if you can actually see that is 40 00:01:30,710 --> 00:01:28,170 right in the middle the optical where 41 00:01:34,280 --> 00:01:30,720 Proxima Centauri actually has whoops so 42 00:01:35,740 --> 00:01:34,290 Proxima Centauri actually has very low 43 00:01:40,039 --> 00:01:35,750 flux and so we're going to look for the 44 00:01:41,330 --> 00:01:40,049 50 577 oxygen line there and it's really 45 00:01:42,380 --> 00:01:41,340 exciting if we could see these lines 46 00:01:43,819 --> 00:01:42,390 because not only would it provide 47 00:01:45,620 --> 00:01:43,829 independent verification of the planet 48 00:01:47,330 --> 00:01:45,630 itself it would also help to constrain 49 00:01:49,340 --> 00:01:47,340 orbital parameters as well as be a 50 00:01:51,260 --> 00:01:49,350 direct verification and identification 51 00:01:52,520 --> 00:01:51,270 of atmospheric species so that would be 52 00:01:54,620 --> 00:01:52,530 very awesome whether it's oxygen or 53 00:01:55,760 --> 00:01:54,630 nitrogen or hydrogen or whatever it'll 54 00:01:57,980 --> 00:01:55,770 be a nice direct observation of the 55 00:01:59,630 --> 00:01:57,990 atmosphere so in general I'm going to 56 00:02:01,249 --> 00:01:59,640 tell you how we estimated the signal 57 00:02:03,380 --> 00:02:01,259 strength how detectable we think those 58 00:02:04,730 --> 00:02:03,390 signals are and then about the search 59 00:02:08,150 --> 00:02:04,740 through the harps the available harps 60 00:02:09,950 --> 00:02:08,160 data the discovery data so for the 61 00:02:11,780 --> 00:02:09,960 signal strength we use two separate 62 00:02:13,490 --> 00:02:11,790 models the one is just a simple kinetic 63 00:02:15,800 --> 00:02:13,500 forcing model and the second is an 64 00:02:18,110 --> 00:02:15,810 empirical image CD fit model by weighing 65 00:02:19,460 --> 00:02:18,120 at all 2014 both of which miss a lot of 66 00:02:20,660 --> 00:02:19,470 magneto spirit physics but they should 67 00:02:22,220 --> 00:02:20,670 be just good enough close to close 68 00:02:24,009 --> 00:02:22,230 enough to a nice order of magnitude 69 00:02:26,179 --> 00:02:24,019 calculation for the aural emission 70 00:02:28,789 --> 00:02:26,189 and so you can think of the 71 00:02:30,649 --> 00:02:28,799 magnetosphere as basically an obstacle 72 00:02:33,319 --> 00:02:30,659 and the fluid flow of the stellar winds 73 00:02:35,149 --> 00:02:33,329 it has some cross-sectional area that is 74 00:02:37,759 --> 00:02:35,159 upon which the stellar wind will impact 75 00:02:39,050 --> 00:02:37,769 and dump energy and so the stellar wind 76 00:02:40,720 --> 00:02:39,060 has some kinetic energy and so therefore 77 00:02:43,339 --> 00:02:40,730 you can calculate simply the power 78 00:02:45,500 --> 00:02:43,349 dumped onto the surface of the 79 00:02:47,059 --> 00:02:45,510 magnetosphere however only a fraction of 80 00:02:49,520 --> 00:02:47,069 that power is then transformed into 81 00:02:51,199 --> 00:02:49,530 electromagnetic auroral emission which 82 00:02:54,860 --> 00:02:51,209 you can see here for Earth it happens to 83 00:02:56,690 --> 00:02:54,870 be by 1% efficiency on average and only 84 00:02:58,399 --> 00:02:56,700 about 2% of that is the five five seven 85 00:02:59,720 --> 00:02:58,409 seven green line and actually that's a 86 00:03:01,729 --> 00:02:59,730 pretty big percentage for a single line 87 00:03:03,920 --> 00:03:01,739 but only got two percent so this is a 88 00:03:06,619 --> 00:03:03,930 very simple kinetic forcing model which 89 00:03:10,099 --> 00:03:06,629 we can use and this gives us a value of 90 00:03:11,659 --> 00:03:10,109 approximately 40 to 50 gigawatts for the 91 00:03:13,520 --> 00:03:11,669 output of just this five five seven 92 00:03:16,220 --> 00:03:13,530 seven green line which is about seventy 93 00:03:18,439 --> 00:03:16,230 to eighty times that of Earth okay so 94 00:03:20,089 --> 00:03:18,449 fairly bright on the second method I 95 00:03:21,949 --> 00:03:20,099 mentioned is wing at all 2014 this 96 00:03:25,670 --> 00:03:21,959 horribly ugly non-linear equation here 97 00:03:28,550 --> 00:03:25,680 they used a 3d global MHD model to fit 98 00:03:29,990 --> 00:03:28,560 the magnetopause surface and across a 99 00:03:32,119 --> 00:03:30,000 wide range of stellar wind parameters 100 00:03:33,399 --> 00:03:32,129 and then fitted or excuse me an invalid 101 00:03:36,920 --> 00:03:33,409 ated against satellite data 102 00:03:38,030 --> 00:03:36,930 magnetospheric satellite data to get an 103 00:03:40,309 --> 00:03:38,040 empirical fit to make sure that is 104 00:03:43,189 --> 00:03:40,319 empirically correct and you can see that 105 00:03:44,509 --> 00:03:43,199 it has the kinetic portion can 106 00:03:46,309 --> 00:03:44,519 contribute by the stellar wind but it 107 00:03:49,129 --> 00:03:46,319 also importantly includes the magnetic a 108 00:03:51,999 --> 00:03:49,139 flower power that you're connecting on 109 00:03:54,020 --> 00:03:52,009 to the magnetosphere both includes the 110 00:03:55,309 --> 00:03:54,030 magnitude and the orientation of the 111 00:03:57,110 --> 00:03:55,319 field which are important because you 112 00:03:58,520 --> 00:03:57,120 must take into account the pointing flux 113 00:03:59,719 --> 00:03:58,530 entering my needle sphere as well as the 114 00:04:01,520 --> 00:03:59,729 orientation of a field which can drive 115 00:04:03,770 --> 00:04:01,530 energetic reconnection events both of 116 00:04:06,349 --> 00:04:03,780 which can affect energization particles 117 00:04:09,050 --> 00:04:06,359 and overall precipitation so we followed 118 00:04:11,089 --> 00:04:09,060 their lead and found a few empirical 119 00:04:12,949 --> 00:04:11,099 measurements of say electron populations 120 00:04:15,319 --> 00:04:12,959 and how they relate to the brightness of 121 00:04:17,089 --> 00:04:15,329 the 577 green line and tried to 122 00:04:19,580 --> 00:04:17,099 determine as close to data as possible 123 00:04:22,670 --> 00:04:19,590 what we would actually see and this is 124 00:04:24,800 --> 00:04:22,680 what we find so for the quiet version 125 00:04:26,959 --> 00:04:24,810 meaning we have no stellar activity and 126 00:04:28,459 --> 00:04:26,969 no geomagnetic activity occurring it 127 00:04:32,029 --> 00:04:28,469 matches pretty well with just a simple 128 00:04:35,510 --> 00:04:32,039 kinetic model including geomagnetic sub 129 00:04:37,150 --> 00:04:35,520 storm activity which we use we use a 130 00:04:38,320 --> 00:04:37,160 proxy basically within 131 00:04:40,030 --> 00:04:38,330 assume very strong reconnection at the 132 00:04:41,680 --> 00:04:40,040 Magneto's claws and reality the 133 00:04:42,790 --> 00:04:41,690 geomagnetic storms have stronger 134 00:04:43,900 --> 00:04:42,800 connections with magneto caused by 135 00:04:45,130 --> 00:04:43,910 driver strong marine current which 136 00:04:46,840 --> 00:04:45,140 effectively weakens the magnetic field 137 00:04:50,280 --> 00:04:46,850 of the planet and can affect their world 138 00:04:53,050 --> 00:04:50,290 activity but you see here we jump up to 139 00:04:56,200 --> 00:04:53,060 140 to 240 gigawatts or so for the Green 140 00:04:57,780 --> 00:04:56,210 Line including the effects of stellar 141 00:04:59,770 --> 00:04:57,790 activity this is a coronal mass ejection 142 00:05:02,230 --> 00:04:59,780 so you know order magnitude greater 143 00:05:03,550 --> 00:05:02,240 density and magnetic flux and a factor 144 00:05:05,260 --> 00:05:03,560 of two or three higher speed and this 145 00:05:07,510 --> 00:05:05,270 ejection of energetic particles out from 146 00:05:09,460 --> 00:05:07,520 the star we jump up to four to eight 147 00:05:11,110 --> 00:05:09,470 terawatts and then if you assume that 148 00:05:12,640 --> 00:05:11,120 this one of these coronal mass ejections 149 00:05:14,320 --> 00:05:12,650 actually drive sub storm activity on the 150 00:05:14,830 --> 00:05:14,330 planet we jump up in the tens of 151 00:05:16,870 --> 00:05:14,840 terawatts 152 00:05:19,120 --> 00:05:16,880 okay so again missing a lot of physics 153 00:05:21,580 --> 00:05:19,130 but decent order of magnitude estimation 154 00:05:22,960 --> 00:05:21,590 and so this ends up being on the order 155 00:05:26,730 --> 00:05:22,970 of tens of thousands of times Earth's 156 00:05:29,110 --> 00:05:26,740 nominal five five seven seven emission 157 00:05:31,450 --> 00:05:29,120 for low to moderate geomagnetic 158 00:05:33,220 --> 00:05:31,460 geomagnetic activity so it looks pretty 159 00:05:35,110 --> 00:05:33,230 good it looks fairly promising I mean 160 00:05:39,010 --> 00:05:35,120 relatively anyway but let's actually 161 00:05:40,330 --> 00:05:39,020 talk about the technical team so this is 162 00:05:42,340 --> 00:05:40,340 the line here on the right this is a 163 00:05:43,810 --> 00:05:42,350 nice high-resolution spectrum we 164 00:05:46,210 --> 00:05:43,820 produced for Proxima Centauri B as 165 00:05:48,880 --> 00:05:46,220 viewed from quadrature you can see the 166 00:05:50,440 --> 00:05:48,890 green line here that we injected it's a 167 00:05:52,420 --> 00:05:50,450 point one terawatt so at the lower end 168 00:05:55,000 --> 00:05:52,430 of our estimations that I just showed 169 00:05:56,409 --> 00:05:55,010 you it has pretty high flux density so 170 00:05:59,230 --> 00:05:56,419 that looks promising however it's an 171 00:06:01,150 --> 00:05:59,240 extremely narrow line and so your active 172 00:06:03,730 --> 00:06:01,160 width is around a third of an angstrom 173 00:06:05,860 --> 00:06:03,740 or so and so you're going to be very 174 00:06:08,920 --> 00:06:05,870 high resolving power to be able to see 175 00:06:12,280 --> 00:06:08,930 any of these very narrow very intense 176 00:06:13,330 --> 00:06:12,290 lines and my understanding is for a lot 177 00:06:16,450 --> 00:06:13,340 of these future missions we discussed 178 00:06:18,640 --> 00:06:16,460 this week we're discussing them in terms 179 00:06:21,640 --> 00:06:18,650 of our value about 100 resolving power 180 00:06:24,190 --> 00:06:21,650 100 which for our full width half max of 181 00:06:25,810 --> 00:06:24,200 this line we calculated means the 182 00:06:27,790 --> 00:06:25,820 spectral element width is about 1,000 183 00:06:28,720 --> 00:06:27,800 times the width of our line so we're not 184 00:06:30,040 --> 00:06:28,730 going to be able to see anything it just 185 00:06:31,510 --> 00:06:30,050 going to be smeared out and lost so we 186 00:06:33,070 --> 00:06:31,520 have to have high resolving power to 187 00:06:35,350 --> 00:06:33,080 view any of these these lines that are 188 00:06:36,340 --> 00:06:35,360 extremely narrow like this obviously so 189 00:06:38,560 --> 00:06:36,350 that means we want to have the best 190 00:06:40,030 --> 00:06:38,570 planet star contrast possible and so 191 00:06:41,940 --> 00:06:40,040 this is a plot of a planet star contrast 192 00:06:44,490 --> 00:06:41,950 in colors and contours 193 00:06:46,200 --> 00:06:44,500 with resolving power on the y-axis and 194 00:06:48,180 --> 00:06:46,210 mom scale and our calculated five five 195 00:06:51,600 --> 00:06:48,190 seven seven green overall power on the 196 00:06:53,460 --> 00:06:51,610 x-axis in log scale also the dashed 197 00:06:55,910 --> 00:06:53,470 lines represent the full width half 198 00:06:58,590 --> 00:06:55,920 maximum selling power in orange and the 199 00:07:01,470 --> 00:06:58,600 equivalent whip resolving power and the 200 00:07:03,630 --> 00:07:01,480 diagonal as it is a function of the 201 00:07:05,250 --> 00:07:03,640 power of emission and so basically you 202 00:07:06,600 --> 00:07:05,260 want to have your observation be inside 203 00:07:08,820 --> 00:07:06,610 this wedge and with the best climate 204 00:07:10,470 --> 00:07:08,830 stark contrast possible harpes for 205 00:07:11,940 --> 00:07:10,480 instance has a resulting power of one 206 00:07:15,750 --> 00:07:11,950 hundred and fifteen thousand so that's 207 00:07:17,070 --> 00:07:15,760 that's our nominal idea that we need to 208 00:07:19,710 --> 00:07:17,080 know somewhere in the order of 10 to the 209 00:07:20,910 --> 00:07:19,720 4 is 10 to the 5 resolving power and if 210 00:07:22,560 --> 00:07:20,920 you look at the powers that we I just 211 00:07:25,920 --> 00:07:22,570 told you on the estimates of our signal 212 00:07:27,720 --> 00:07:25,930 we see that we obtain a star planet 213 00:07:30,000 --> 00:07:27,730 contrast or keeping planet star contrast 214 00:07:31,980 --> 00:07:30,010 of 8 times 10 to the 7 and 7 times 10 to 215 00:07:34,650 --> 00:07:31,990 the minus 5 for direct observation in 216 00:07:37,800 --> 00:07:34,660 the optical around for this emission of 217 00:07:40,440 --> 00:07:37,810 Proxima Centauri so I'm pretty good for 218 00:07:42,690 --> 00:07:40,450 direct observation looking for the 219 00:07:44,010 --> 00:07:42,700 submission but what does this say about 220 00:07:47,910 --> 00:07:44,020 the actual integration time you would 221 00:07:49,200 --> 00:07:47,920 need well so we calculated the 222 00:07:52,140 --> 00:07:49,210 integration time to reach a signal noise 223 00:07:53,670 --> 00:07:52,150 of 6 with an R value of 150 thousand in 224 00:07:55,140 --> 00:07:53,680 all cases so here in x-axis we're 225 00:07:57,330 --> 00:07:55,150 looking at integration time and hours 226 00:08:01,140 --> 00:07:57,340 log scale and we did this for harps have 227 00:08:03,180 --> 00:08:01,150 exlude war and a 30 meter telescope the 228 00:08:04,680 --> 00:08:03,190 green bar is one point our low end point 229 00:08:05,190 --> 00:08:04,690 one terawatts a yellow bar is 10 230 00:08:07,350 --> 00:08:05,200 terawatts 231 00:08:08,670 --> 00:08:07,360 and then highly unlikely which I mostly 232 00:08:12,120 --> 00:08:08,680 ignore the tails and terawatt emission 233 00:08:14,670 --> 00:08:12,130 in red and so you can see for harps we 234 00:08:16,770 --> 00:08:14,680 need somewhere between present-day 235 00:08:20,790 --> 00:08:16,780 hundred thousand to one billion hours of 236 00:08:23,610 --> 00:08:20,800 integration time highly unlikely say 237 00:08:24,960 --> 00:08:23,620 unlikely but for these future 238 00:08:26,340 --> 00:08:24,970 instruments you can see especially on 239 00:08:27,900 --> 00:08:26,350 the top end here for 10 terawatts we 240 00:08:30,000 --> 00:08:27,910 start getting down to the 10 hour one 241 00:08:31,590 --> 00:08:30,010 hour point three hours of integration 242 00:08:34,770 --> 00:08:31,600 time so this becomes highly probable and 243 00:08:36,270 --> 00:08:34,780 I will say that given the activity at 244 00:08:38,040 --> 00:08:36,280 high activity Proxima Centauri and 245 00:08:39,300 --> 00:08:38,050 assuming of course that you have a 246 00:08:41,969 --> 00:08:39,310 magnetic field which we've assumed in 247 00:08:43,950 --> 00:08:41,979 Earth's dipole our sized planet 248 00:08:46,710 --> 00:08:43,960 given exactly if you have a magnetic 249 00:08:48,180 --> 00:08:46,720 field you're likely to drive these logs 250 00:08:50,100 --> 00:08:48,190 team activity is going to likely drive 251 00:08:52,660 --> 00:08:50,110 sub storm activity on the planet there 252 00:08:54,820 --> 00:08:52,670 all these assumptions and 253 00:08:56,140 --> 00:08:54,830 you're going to have some signal that's 254 00:08:57,430 --> 00:08:56,150 between the two bounds that we got at 255 00:08:58,900 --> 00:08:57,440 this point one terawatt in 10 terawatts 256 00:09:00,850 --> 00:08:58,910 so the average flux that we'll see when 257 00:09:02,830 --> 00:09:00,860 we look to cross missing tardy if it has 258 00:09:04,080 --> 00:09:02,840 an atmosphere in a magnetic field it's 259 00:09:06,460 --> 00:09:04,090 going to be somewhere between these 260 00:09:07,750 --> 00:09:06,470 green and yellow lines and you look at 261 00:09:09,250 --> 00:09:07,760 these future missions and you absolutely 262 00:09:11,710 --> 00:09:09,260 see that within a few days these 263 00:09:13,840 --> 00:09:11,720 missions could your admissions and/or 264 00:09:15,990 --> 00:09:13,850 ground-based scope for the 30-meter I 265 00:09:18,850 --> 00:09:16,000 could actually pick out these signals 266 00:09:19,720 --> 00:09:18,860 within a reasonable time and so I should 267 00:09:21,280 --> 00:09:19,730 I should mention I shoulda mentioned 268 00:09:23,080 --> 00:09:21,290 this at the beginning leVoir we 269 00:09:24,610 --> 00:09:23,090 estimated this for a 16 years of war and 270 00:09:26,170 --> 00:09:24,620 this is the certainty of telescope with 271 00:09:30,070 --> 00:09:26,180 a coronagraph of design contrast 10 to 272 00:09:32,050 --> 00:09:30,080 the minus 7 ok so given what I just told 273 00:09:34,240 --> 00:09:32,060 you about harps we did look through the 274 00:09:37,390 --> 00:09:34,250 data and we need you know at least a 275 00:09:40,300 --> 00:09:37,400 hundred thousand hours but we have 70 so 276 00:09:42,400 --> 00:09:40,310 let's see what we can actually find so 277 00:09:44,500 --> 00:09:42,410 to the pipeline that we followed for 278 00:09:47,140 --> 00:09:44,510 time purposes I'm not going to go into 279 00:09:49,270 --> 00:09:47,150 it too much but basically remove the 280 00:09:51,250 --> 00:09:49,280 stellar signal we docile ship into the 281 00:09:52,960 --> 00:09:51,260 proximities rest frame and then want to 282 00:09:56,110 --> 00:09:52,970 stack all of this flux and book for our 283 00:09:57,430 --> 00:09:56,120 5 5 7 7 but it's a radial velocity 284 00:09:58,660 --> 00:09:57,440 measurement so we have to be careful 285 00:10:01,030 --> 00:09:58,670 about looking through the Earth's 286 00:10:04,450 --> 00:10:01,040 atmosphere where we have 5 5 7 7 airglow 287 00:10:05,920 --> 00:10:04,460 and or and the fact that we're looking 288 00:10:07,750 --> 00:10:05,930 to Proxima Centauri which relatively 289 00:10:08,920 --> 00:10:07,760 orbits rapidly and therefore the Rd 290 00:10:11,290 --> 00:10:08,930 signal will be passing through what 291 00:10:14,290 --> 00:10:11,300 we're seeing in overlapping from the 292 00:10:15,850 --> 00:10:14,300 earth so anytime anyone overlaps occurs 293 00:10:17,620 --> 00:10:15,860 either you know from earth signal with 294 00:10:19,690 --> 00:10:17,630 the planet or Proxima Centauri or signal 295 00:10:20,740 --> 00:10:19,700 with the planet we removed that data and 296 00:10:22,750 --> 00:10:20,750 don't consider it to make sure we're not 297 00:10:24,520 --> 00:10:22,760 contaminating and then we use a filter 298 00:10:27,190 --> 00:10:24,530 to get rid of the noise and stack around 299 00:10:31,750 --> 00:10:27,200 the second two bins around the line of 300 00:10:33,550 --> 00:10:31,760 interest so here's a strongest signal we 301 00:10:36,160 --> 00:10:33,560 performing a grid search because we had 302 00:10:37,390 --> 00:10:36,170 to constrain some orbit parameters of 303 00:10:38,860 --> 00:10:37,400 the Rd measurement because the 304 00:10:41,560 --> 00:10:38,870 inclination is absolutely unknown due to 305 00:10:42,820 --> 00:10:41,570 the method used so but our strongest 306 00:10:44,860 --> 00:10:42,830 signal came out with an inclination of 307 00:10:47,410 --> 00:10:44,870 52 degrees this period in the mean 308 00:10:49,420 --> 00:10:47,420 longitude and you can see that here this 309 00:10:51,490 --> 00:10:49,430 is in the rest frame of Proxima Centauri 310 00:10:53,470 --> 00:10:51,500 B this is the blue window you see the 311 00:10:56,350 --> 00:10:53,480 center here centered on our line of 312 00:10:58,660 --> 00:10:56,360 interest and you can see that the earth 313 00:11:00,550 --> 00:10:58,670 lines and then the tiller Cline's from 314 00:11:03,580 --> 00:11:00,560 Earth in green and the lines from the 315 00:11:04,900 --> 00:11:03,590 host star in red and again because we're 316 00:11:05,790 --> 00:11:04,910 now in the rest frame Proxima Centauri B 317 00:11:10,530 --> 00:11:05,800 we see 318 00:11:12,600 --> 00:11:10,540 the nice Doppler shift of Earth and the 319 00:11:14,429 --> 00:11:12,610 star from that point of view so since we 320 00:11:16,919 --> 00:11:14,439 have all of our flux stacked up we can 321 00:11:19,470 --> 00:11:16,929 just are in the flux alone nicely lined 322 00:11:20,429 --> 00:11:19,480 up here for the planet we can just add 323 00:11:22,679 --> 00:11:20,439 all the flux together and look for our 324 00:11:26,340 --> 00:11:22,689 signal we do this and this is what we 325 00:11:28,979 --> 00:11:26,350 see here is the signal it's there's a 326 00:11:29,970 --> 00:11:28,989 bump there yes unfortunately it's in the 327 00:11:31,530 --> 00:11:29,980 middle of bunch of noise and 328 00:11:32,999 --> 00:11:31,540 inconsistent with rest of the noise and 329 00:11:36,479 --> 00:11:33,009 when you've been at the same thing 330 00:11:37,859 --> 00:11:36,489 happens so and in fact it is consistent 331 00:11:40,499 --> 00:11:37,869 with noise what we do is we take we did 332 00:11:43,410 --> 00:11:40,509 then saw this and took a window of 200 333 00:11:45,629 --> 00:11:43,420 angstroms around the other side of the 334 00:11:47,189 --> 00:11:45,639 line of interest and ran this exact this 335 00:11:48,600 --> 00:11:47,199 exact same pipeline the exact same grid 336 00:11:50,160 --> 00:11:48,610 search found the strongest signal for 337 00:11:52,109 --> 00:11:50,170 each wavelength in a 200 angstrom window 338 00:11:54,470 --> 00:11:52,119 and we see this so it's consistent with 339 00:11:57,389 --> 00:11:54,480 correlated stellar noise unfortunately 340 00:11:59,999 --> 00:11:57,399 and we don't expect any emission from 341 00:12:04,559 --> 00:12:00,009 the planet on either side of the 577 342 00:12:05,999 --> 00:12:04,569 line so yeah there's a lot of this going 343 00:12:07,109 --> 00:12:06,009 on so we failed to move all the noise 344 00:12:08,340 --> 00:12:07,119 and that's going to be a limiting 345 00:12:10,019 --> 00:12:08,350 factors or they're seeing these lines at 346 00:12:11,999 --> 00:12:10,029 this point I think at least with the 347 00:12:15,210 --> 00:12:12,009 harps data so the significance is point 348 00:12:18,030 --> 00:12:15,220 7 sigma 20% false alarm probability so 349 00:12:19,470 --> 00:12:18,040 we will actually say that absolutely not 350 00:12:24,600 --> 00:12:19,480 detection because we don't have the 351 00:12:25,739 --> 00:12:24,610 requisite 1 billion hours of data ok but 352 00:12:27,809 --> 00:12:25,749 all is not lost as I mentioned these 353 00:12:29,009 --> 00:12:27,819 future missions have a do enough of a 354 00:12:30,840 --> 00:12:29,019 light bucket that they can collect the 355 00:12:32,160 --> 00:12:30,850 signal and but we need a high resolution 356 00:12:34,439 --> 00:12:32,170 spectrograph to take these signals out 357 00:12:35,879 --> 00:12:34,449 and so that's part of the hope that 358 00:12:37,049 --> 00:12:35,889 we'll see that in the future that these 359 00:12:39,359 --> 00:12:37,059 you know 10 to the 4 to the 5 360 00:12:40,889 --> 00:12:39,369 spectrograph will be included we did 361 00:12:42,749 --> 00:12:40,899 actually elevation we did actually also 362 00:12:44,669 --> 00:12:42,759 ran a search for the strong 3917 363 00:12:46,919 --> 00:12:44,679 nitrogen line and the 6300 oxygen line 364 00:12:48,659 --> 00:12:46,929 but also it's all nothing 365 00:12:51,960 --> 00:12:48,669 so I told you about our signal strength 366 00:12:53,579 --> 00:12:51,970 which is many times that of Earth I told 367 00:12:55,470 --> 00:12:53,589 you about our expected detect ability 368 00:12:57,989 --> 00:12:55,480 and making all these assumptions it 369 00:12:59,340 --> 00:12:57,999 requires really high resolving power and 370 00:13:00,809 --> 00:12:59,350 a large aperture we didn't have that 371 00:13:02,369 --> 00:13:00,819 large aperture unfortunately so we 372 00:13:03,689 --> 00:13:02,379 didn't see anything in the data but we 373 00:13:04,829 --> 00:13:03,699 think the future missions it's it's 374 00:13:06,210 --> 00:13:04,839 likely that we can get some sort of 375 00:13:08,340 --> 00:13:06,220 exciting observation like this and 376 00:13:09,569 --> 00:13:08,350 constrain the atmosphere directly if we 377 00:13:13,919 --> 00:13:09,579 can get all of the technology in place 378 00:13:15,359 --> 00:13:13,929 so thanks to my co-authors and BPL and 379 00:13:20,790 --> 00:13:15,369 thanks to all of you for your attention 380 00:13:25,410 --> 00:13:22,970 [Music] 381 00:13:28,800 --> 00:13:25,420 we have a few minutes for quick 382 00:13:30,300 --> 00:13:28,810 questions hi this is a great effort as I 383 00:13:31,800 --> 00:13:30,310 was wondering if you stack all the lines 384 00:13:33,180 --> 00:13:31,810 together to have in your spectrum is 385 00:13:34,350 --> 00:13:33,190 that a way to sort of decrease the 386 00:13:35,840 --> 00:13:34,360 amount of observing time you need to 387 00:13:38,700 --> 00:13:35,850 detect any emission at all 388 00:13:39,330 --> 00:13:38,710 I'm sorry so if you stack multiple lines 389 00:13:41,670 --> 00:13:39,340 together 390 00:13:44,190 --> 00:13:41,680 I said away sort of to decrease your 391 00:13:45,030 --> 00:13:44,200 observing time you would need I'm not an 392 00:13:47,160 --> 00:13:45,040 observer so that's a really good 393 00:13:48,600 --> 00:13:47,170 question I would refer you to when I co 394 00:13:52,320 --> 00:13:48,610 others and maybe Rodrigo can answer that 395 00:13:53,910 --> 00:13:52,330 now do you mean lines of different 396 00:13:56,130 --> 00:13:53,920 elements or different lines of oxygen 397 00:13:58,020 --> 00:13:56,140 absolutely right but you want to make 398 00:13:59,640 --> 00:13:58,030 sure that you're stacking lines that 399 00:14:01,080 --> 00:13:59,650 exist and so like if you were to stack 400 00:14:03,270 --> 00:14:01,090 the oxygen and the nitrogen line the 401 00:14:04,920 --> 00:14:03,280 nitrogen line doesn't exist you'll get a 402 00:14:07,260 --> 00:14:04,930 lower signal because you're stacking 403 00:14:09,630 --> 00:14:07,270 signal with noise but you've definitely 404 00:14:11,580 --> 00:14:09,640 do a search that way where you you 405 00:14:13,020 --> 00:14:11,590 obviously oxygen has tons of lines of 406 00:14:14,250 --> 00:14:13,030 need for red as well and we could stack 407 00:14:15,660 --> 00:14:14,260 all of those and do some kind of grid 408 00:14:20,180 --> 00:14:15,670 search it would definitely increase your 409 00:14:27,000 --> 00:14:23,040 what is the upper limit correspond to in 410 00:14:28,440 --> 00:14:27,010 terms of terawatts welcome sorry you are 411 00:14:30,210 --> 00:14:28,450 giving the detectability you are 412 00:14:32,160 --> 00:14:30,220 measuring the line strength in terms of 413 00:14:34,260 --> 00:14:32,170 terawatts yes and then you presented an 414 00:14:36,360 --> 00:14:34,270 upper limit in terms of Sigma's what 415 00:14:42,300 --> 00:14:36,370 does that correspond to it in terawatts 416 00:14:44,160 --> 00:14:42,310 oh so I believe so mmm the point seven 417 00:14:46,950 --> 00:14:44,170 think I'm not really sure but we did run 418 00:14:48,060 --> 00:14:46,960 an upper bound of eight segment 419 00:14:49,350 --> 00:14:48,070 detection and I've ended up being 420 00:14:51,270 --> 00:14:49,360 something on the border freed alcantara 421 00:14:53,970 --> 00:14:51,280 watts or so but but the point seven is 422 00:14:55,320 --> 00:14:53,980 no it's something ridiculous that okay 423 00:14:59,490 --> 00:14:55,330 it's in the paper kendra has a spare 424 00:15:00,480 --> 00:14:59,500 let's go let's thank Matt again