1 00:00:00,010 --> 00:00:04,070 [music] 2 00:00:04,090 --> 00:00:08,190 [music] 3 00:00:08,210 --> 00:00:12,200 Narrator: When a massive star 4 00:00:12,220 --> 00:00:16,250 explodes as a supernova, its core may be crushed into one of two types 5 00:00:16,270 --> 00:00:20,360 of compact remnant: a black hole, or a neutron star. 6 00:00:20,380 --> 00:00:24,510 Neutron stars are the size of a city, but 7 00:00:24,530 --> 00:00:28,660 contain more mass than our sun. They rotate rapidly, host 8 00:00:28,680 --> 00:00:32,720 powerful magnetic fields, and produce beams of radiation that emit a wide 9 00:00:32,740 --> 00:00:36,880 range of energy. When we detect pulses as the beams sweep over 10 00:00:36,900 --> 00:00:41,060 Earth, the object is known as a pulsar. Paul Ray: They can spin at 11 00:00:41,080 --> 00:00:45,150 many times per second on their axis; the fastest pulsars spin over 700 times 12 00:00:45,170 --> 00:00:49,180 per second. And that rapidly spinning massive object, generates 13 00:00:49,200 --> 00:00:53,260 extremely strong magnetic fields and accelerates particles to 14 00:00:53,280 --> 00:00:57,400 high energies. And we see that those accelerated particles 15 00:00:57,420 --> 00:01:01,440 emitting energy in the form of gamma rays, x-rays, and radio waves. 16 00:01:01,460 --> 00:01:05,480 And when that beam sweeps past the line of sight to the Earth we see it pulse on 17 00:01:05,500 --> 00:01:09,540 and that's why they're named pulsars. Narrator: The most 18 00:01:09,560 --> 00:01:13,670 sensitive tool for observing pulsars in gamma-ray light is NASA's 19 00:01:13,690 --> 00:01:17,840 Fermi Gamma-ray Space Telescope. Fermi scans the entire 20 00:01:17,860 --> 00:01:21,950 sky for high-energy sources and has found many previously undetected 21 00:01:21,970 --> 00:01:26,130 gamma-ray emitters. Scientists have identified many of these, 22 00:01:26,150 --> 00:01:30,220 but for some, the source of the gamma rays remains unknown. 23 00:01:30,240 --> 00:01:34,320 Roger W. Romani: I got interested a couple years ago in trying to find the 24 00:01:34,340 --> 00:01:38,470 limits of what Fermi can discover, how extreme these objects can be, and 25 00:01:38,490 --> 00:01:42,530 in order to do that I focused on the set of objects that are 26 00:01:42,550 --> 00:01:46,640 relatively bright and well measured by Fermi and 27 00:01:46,660 --> 00:01:50,720 found that virtually all of them have now been identified. At present, when I started 28 00:01:50,740 --> 00:01:54,870 this project,there were only six objects which we hadn't figured out what they were yet. 29 00:01:54,890 --> 00:01:58,930 Despite intense searches, at radio, with radio wave lengths, 30 00:01:58,950 --> 00:02:03,070 which is the standard way in which people find pulsars--and also looking at the gamma rays 31 00:02:03,090 --> 00:02:07,130 themselves--no pulsations had been seen. So something was unique 32 00:02:07,150 --> 00:02:11,250 about these six objects and I thought, that's where the discovery space is going to be. 33 00:02:11,270 --> 00:02:15,270 If we can track down what those are, we will have a good chance of finding something new. 34 00:02:15,290 --> 00:02:19,330 We took this small set of six objects and attacked them 35 00:02:19,350 --> 00:02:23,390 with a number of wave bands, but I think the thing that helped us make the greatest progress 36 00:02:23,410 --> 00:02:27,490 was looking in the optical, in visible light. Now this may seem a little bit unusual 37 00:02:27,510 --> 00:02:31,580 for studying the high-energy gamma-ray universe, but, it turns out that 38 00:02:31,600 --> 00:02:35,750 many of these objects seem to have optical counterparts. And if you can figure out what the 39 00:02:35,770 --> 00:02:39,800 visible light counterpart of an object is, you're long ways along the 40 00:02:39,820 --> 00:02:43,870 track to understanding what it's all about. Paul Ray: It was Roger 41 00:02:43,890 --> 00:02:48,000 Romani's optical observations that discovered a counterpart 42 00:02:48,020 --> 00:02:52,120 to the gamma-ray source that showed a binary period that was 43 00:02:52,140 --> 00:02:56,180 indicative of this potentially being a binary millisecond pulsar. Alice Harding: It brightened, and it 44 00:02:56,200 --> 00:03:00,290 dimmed, and brightened, and so this looked like we were 45 00:03:00,310 --> 00:03:04,300 looking at possibly something which was 46 00:03:04,320 --> 00:03:08,350 irradiated by a companion pulsar. And that every 47 00:03:08,370 --> 00:03:12,420 time you're looking at the bright face you see a bright optical source and when 48 00:03:12,440 --> 00:03:16,510 it rotates away from you, and you see the dark face, you don't see anything. 49 00:03:16,530 --> 00:03:20,510 Roger Romani: We managed to get enough observations of the object to piece together its orbital 50 00:03:20,530 --> 00:03:24,560 period, and found, remarkably, that it was an incredibly 51 00:03:24,580 --> 00:03:28,660 heated object--blue white on one side, deep, deep red on the other-- 52 00:03:28,680 --> 00:03:32,750 that was orbiting around something invisible with an orbital period of about 53 00:03:32,770 --> 00:03:36,790 one and a half hours. Now, that's faster then any spin powered 54 00:03:36,810 --> 00:03:40,850 pulsar ever known, and indicates that it's a really, really tight system 55 00:03:40,870 --> 00:03:44,880 and that the gamma rays are blasting the companion at point-blank range. 56 00:03:44,900 --> 00:03:48,970 Our colleagues in Germany managed to use the orbital period 57 00:03:48,990 --> 00:03:53,100 that we measured to search in the gamma rays directly and, with a computational 58 00:03:53,120 --> 00:03:57,160 tour de force, managed to find the pulse signal of the pulsar 59 00:03:57,180 --> 00:04:01,210 directly in the gamma rays themself. Holger Pletsch: What I'm 60 00:04:01,230 --> 00:04:05,240 doing is blind searches for pulsars so that we 61 00:04:05,260 --> 00:04:09,330 try to find pulsars that have not been seen before. So you don't know 62 00:04:09,350 --> 00:04:13,370 how fast the pulsar is spinning, where exactly it is sitting in the sky. 63 00:04:13,390 --> 00:04:17,420 To do that, you have basically to try, every possible combination of 64 00:04:17,440 --> 00:04:21,510 parameters--if they match your data output stream. So the problem is 65 00:04:21,530 --> 00:04:25,530 that the number of possible combinations is tremendously high, so the 66 00:04:25,550 --> 00:04:29,590 straightforward brute force approach is impossible. The computation power you would 67 00:04:29,610 --> 00:04:33,640 need would be in excess of what is available in the whole planet. 68 00:04:33,660 --> 00:04:37,820 So our work is to invent more efficient methods to do that. 69 00:04:37,840 --> 00:04:41,850 The basic method is analogous to zooming. 70 00:04:41,870 --> 00:04:45,920 It's similar to changing your objectives 71 00:04:45,940 --> 00:04:49,990 of your microscope, in favor of one of higher magnification, so you look at 72 00:04:50,010 --> 00:04:54,020 one interesting point on the slide, and then you zoom in on that. 73 00:04:54,040 --> 00:04:58,110 And then you further zoom in if it still is interesting. To find the pulsations 74 00:04:58,130 --> 00:05:02,260 in the gamma ray data requires about 75 00:05:02,280 --> 00:05:06,300 5,000 cpu days. So if you do it 76 00:05:06,320 --> 00:05:10,420 on your laptop you need 5,000 days, but if you 77 00:05:10,440 --> 00:05:14,590 have 5,000 laptops, you only need one day. And so 78 00:05:14,610 --> 00:05:18,710 that is the path we took because we have a computing cluster that is called Atlas 79 00:05:18,730 --> 00:05:22,880 at the Albert Einstein Institute in Hannover and that computing facility 80 00:05:22,900 --> 00:05:26,960 we used for this analysis and it was immediately clear. 81 00:05:26,980 --> 00:05:31,090 This is a detection, so it's, it cannot be a noise fluctuation 82 00:05:31,110 --> 00:05:35,240 because it's so loud in the data. 83 00:05:35,260 --> 00:05:39,280 Narrator: A pulsar, that was a strong gamma ray source yet showed no radio signature 84 00:05:39,300 --> 00:05:43,380 intrigued researchers. Among them was Paul Ray of the 85 00:05:43,400 --> 00:05:47,530 Naval Research Laboratory. He and his team thought they might have a solution to the 86 00:05:47,550 --> 00:05:51,600 puzzling lack of radio emission. Paul Ray: When we first discovered the 87 00:05:51,620 --> 00:05:55,690 system I looked back at our archival radio observations and none of them 88 00:05:55,710 --> 00:05:59,800 showed detections of this pulsar. We think that nearly all pulsars do emit 89 00:05:59,820 --> 00:06:03,840 radio waves. The radio beam is emitted for most pulsars 90 00:06:03,860 --> 00:06:07,890 from a region above the polar cap of the star, and that means it's a tightly concentrated 91 00:06:07,910 --> 00:06:12,040 flashlight-type beam. In a system like this where there's wind being blown 92 00:06:12,060 --> 00:06:16,080 off the companion star, there's a lot of obscuring material along the line of sight. 93 00:06:16,100 --> 00:06:20,170 It might be that it is a radio pulsar and we just couldn't see it. 94 00:06:20,190 --> 00:06:24,230 And the one way to confront that is to use a higher radio frequency, 95 00:06:24,250 --> 00:06:28,360 that's more penetrating, that's less affected by the scattering in the intervening 96 00:06:28,380 --> 00:06:32,460 material. And so we went and made an observation with the Robert C. Byrd Green Bank 97 00:06:32,480 --> 00:06:36,650 Telescope run by the National Radio Astronomy Observatory in West Virginia, 98 00:06:36,670 --> 00:06:40,690 at a much higher frequency than typical radio observations. And it was in one 99 00:06:40,710 --> 00:06:44,750 of those observations that we first saw the signal from the system. And it 100 00:06:44,770 --> 00:06:48,770 appears that it is most of the time obscured by the material 101 00:06:48,790 --> 00:06:52,880 from its companion. Narrator: A combination of radio 102 00:06:52,900 --> 00:06:56,900 optical, and gamma-ray data allowed astronomers to assemble a 103 00:06:56,920 --> 00:07:00,980 complete picture of the system. It turned out to be a rare black widow 104 00:07:01,000 --> 00:07:05,140 binary where a rejuvenated pulsar is gradually evaporating a low 105 00:07:05,160 --> 00:07:09,170 mass companion star. Alice Harding: They get this name because they are in 106 00:07:09,190 --> 00:07:13,270 very close systems, with the companion star being close enough to the 107 00:07:13,290 --> 00:07:17,450 neutron star, that the neutron star is irradiating the companion. 108 00:07:17,470 --> 00:07:21,500 So the neutron star is producing a wind of energetic particles and 109 00:07:21,520 --> 00:07:25,610 magnetic fields, and also all the gamma rays that are radiated. All this 110 00:07:25,630 --> 00:07:29,790 hits the companion star and heats it up to very 111 00:07:29,810 --> 00:07:33,840 high temperatures, but only on one side. So the side that's 112 00:07:33,860 --> 00:07:37,940 towards the neutron star gets blasted by this pulsar wind. 113 00:07:37,960 --> 00:07:42,080 Paul Ray: And it has been whittled away over billions of years to where it now is 114 00:07:42,100 --> 00:07:46,140 only about 8 times the mass of Jupiter. Alice Harding: This whole system is about the size 115 00:07:46,160 --> 00:07:50,250 of the Earth-Moon system, so it's very compact. 116 00:07:50,270 --> 00:07:54,280 Paul Ray: We see the pulsar at the center, spinning, and emitting beams of 117 00:07:54,300 --> 00:07:58,350 radio and gamma rays. The radio waves are represented by the green, 118 00:07:58,370 --> 00:08:02,480 and the gamma rays are represented by the magenta. That radiation that 119 00:08:02,500 --> 00:08:06,510 impinges on the star is blowing off clouds of ionized material 120 00:08:06,530 --> 00:08:10,600 that are collecting around the system, and that's what obscures the radio emission. 121 00:08:10,620 --> 00:08:14,760 So we see that most of the time, the radio represented in green only 122 00:08:14,780 --> 00:08:18,800 makes it to that obscuring material, and not through it. While the gamma rays 123 00:08:18,820 --> 00:08:22,890 which are much more penetrating go right through. 124 00:08:22,910 --> 00:08:27,010 Roger W. Romani: It turns out that in as far as it's a pulsar, it's not so very unusual. 125 00:08:27,030 --> 00:08:31,040 What's unusual about it is this binary system, and the binary 126 00:08:31,060 --> 00:08:35,130 system seems to have--through its history--allowed this neutron star 127 00:08:35,150 --> 00:08:39,210 pulsar to accrete enormous amounts of mass. The measurements to date 128 00:08:39,230 --> 00:08:43,340 suggest that it is very heavy indeed, and heavy neutron stars push 129 00:08:43,360 --> 00:08:47,380 the absolute extreme of the densest matter in our visible universe. I say 130 00:08:47,400 --> 00:08:51,440 this because many people think of black holes as being exotic and the most extreme objects 131 00:08:51,460 --> 00:08:55,550 known, but after all, a black hole has collapsed to the point where 132 00:08:55,570 --> 00:08:59,680 nothing is visible, it's black. A neutron star is an object that's 133 00:08:59,700 --> 00:09:03,710 on the hairy edge of becoming a black hole, yet is still visible in our universe. 134 00:09:03,730 --> 00:09:07,780 Hence the study of the these ultra-massive neutron stars 135 00:09:07,800 --> 00:09:11,830 gives us the opportunity to study the most extreme matter in our visible universe. 136 00:09:11,850 --> 00:09:15,930 If this fellow is as heavy as he seems, he pushes 137 00:09:15,950 --> 00:09:20,090 that study to a new horizon, to a region of density 138 00:09:20,110 --> 00:09:24,150 and pressure which has never previously been seen. 139 00:09:24,170 --> 00:09:28,230 [music] 140 00:09:28,250 --> 00:09:32,390 [beeping] 141 00:09:32,410 --> 00:09:36,450 [beeping] 142 00:09:36,470 --> 00:09:40,394