WEBVTT FILE 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