First observation of gravitational waves

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First observation of gravitational waves
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LIGO measurement of the gravitational waves at the Livingston (right) and Hanford (left) detectors, compared with the theoretical predicted values
Other designations Lua error in Module:Wikidata at line 446: attempt to index field 'wikibase' (a nil value).
Event type Lua error in Module:Wikidata at line 446: attempt to index field 'wikibase' (a nil value).
Detection
Date Lua error in Module:Wikidata at line 446: attempt to index field 'wikibase' (a nil value).
Duration 0.2 seconds
Instrument Lua error in Module:Wikidata at line 446: attempt to index field 'wikibase' (a nil value).
Location
Constellation Lua error in Module:Wikidata at line 446: attempt to index field 'wikibase' (a nil value).
Distance 410+160
−180 Mpc[1]
Redshift 0.09+0.03
−0.04[1]
Energetics
Total energy output 3.0+0.5
−0.5 M☉ × c2[1]
See also
Website <strong%20class= "error"><span%20class="scribunto-error"%20id="mw-scribunto-error-6">Lua%20error%20in%20Module:Wikidata%20at%20line%20446:%20attempt%20to%20index%20field%20'wikibase'%20(a%20nil%20value). http://<strong%20class="error"><span%20class="scribunto-error"%20id="mw-scribunto-error-6">Lua%20error%20in%20Module:Wikidata%20at%20line%20446:%20attempt%20to%20index%20field%20'wikibase'%20(a%20nil%20value).
Commons page [[Commons:Category:Lua error in Module:Wikidata at line 446: attempt to index field 'wikibase' (a nil value). |Related media on Wikimedia Commons]]

The first observation of gravitational waves occurred on 14 September 2015 and was announced by the LIGO and Virgo collaborations on 11 February 2016.[2][3][4] Previously, gravitational waves had been inferred only indirectly, via their effect on the timing of pulsars in binary star systems. The waveform, detected by both LIGO observatories,[5] matched the predictions of general relativity for a gravitational wave emanating from the inward spiral and merger of a pair of black holes of around 36 and 29 solar masses and the subsequent "ringdown" of the single resulting black hole.[note 1] The signal was named GW150914 (from "Gravitational Wave" and the date of observation).[2][7][note 2]

It was also the first observation of a binary black hole merger, demonstrating both the existence of binary stellar-mass black hole systems, and the fact that such mergers could occur within the current age of the universe.

This first observation was reported around the world as a remarkable accomplishment for many reasons. Efforts to directly prove the existence of such waves had been ongoing for over fifty years, and the waves are so minuscule that Albert Einstein himself doubted that they could ever be detected.[8][9] The waves given off by the cataclysmic merger of GW150914 reached Earth as a ripple in spacetime that changed the length of a 4-km LIGO arm by a thousandth of the width of a proton,[7] proportionally equivalent to changing the distance to the nearest star outside the Solar System by one hair's width.[10][note 3] The energy released by the binary as it spiralled together and merged was immense, with the energy of 3.0+0.5
−0.5 c2 solar masses (5.3+0.9
−0.8×1047 joules) in total radiated as gravitational waves, reaching a peak emission rate of about 3.6+0.5
−0.4×1049 watts – a level greater than the combined power of all light radiated by all the stars in the observable universe.[2][3][11][12][note 4]

The observation confirms the last remaining unproven prediction of general relativity and validates its predictions of space-time distortion in the context of large scale cosmic events (known as strong field tests). It was also heralded as inaugurating a new era of gravitational-wave astronomy, which will enable observations of violent astrophysical events that were not previously possible, and potentially allow the direct observation of the very earliest history of the universe.[2][14][15][16][17]

Gravitational waves

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Main article: Gravitational wave
Video simulation showing the warping of space-time and gravitational waves produced, during the final inspiral, merge, and ringdown of black hole binary system GW150914.[18]

Albert Einstein originally predicted the existence of gravitational waves in 1916,[19][20] on the basis of his theory of general relativity.[21] General relativity interprets gravity as a consequence of distortions in space-time, caused by mass. Therefore, Einstein also predicted that events in the cosmos would cause "ripples" in space-time – distortions of space-time itself – which would spread outward, although they would be so minuscule that they would be nearly impossible to detect by any technology foreseen at that time.[9] It was also predicted that objects moving in an orbit would lose energy for this reason (a consequence of the law of conservation of energy), as some energy would be given off as gravitational waves, although this would be insignificantly small in all but the most extreme cases.[22]

One case where gravitational waves would be strongest is during the final moments of the merger of two compact objects such as neutron stars or black holes. Over a span of millions of years, binary neutron stars, and binary black holes lose energy, largely through gravitational waves, and as a result, they spiral in towards each other. At the very end of this process, the two objects will reach extreme velocities, and in the final fraction of a second of their merger a substantial amount of their mass would theoretically be converted into gravitational energy, and travel outward as gravitational waves,[23] allowing a greater than usual chance for detection. However, since little was known about the number of compact binaries in the universe and reaching that final stage can be very slow, there was little certainty as to how often such events might happen.[24]

Observation

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Main article: Gravitational-wave astronomy
Slow motion computer simulation of the black hole binary system GW150914 as seen by a nearby observer, during 0.33 s of its final inspiral, merge, and ringdown. The star field behind the black holes is being heavily distorted and appears to rotate and move, due to extreme gravitational lensing, as space-time itself is distorted and dragged around by the rotating black holes.[18]

Observations of gravitational waves can be made either indirectly, by observing the effects of waves on the distant objects, and deducing their likely cause, or directly by detecting and observing the effects of waves acting on instruments on Earth like LIGO, or in at least two decades by a spacecraft like eLISA.[25]

Indirect observation

Evidence of gravitational waves was first deduced in 1974 through the motion of the double neutron star system PSR B1913+16, in which one of the stars is a pulsar that emits pulses at radio frequencies at precise, regular intervals as it rotates. Russell Hulse and Joseph Taylor, who discovered the stars, also showed that over time, the frequency of pulses shortened, and that the stars were gradually spiralling towards each other with an energy loss that agreed closely with the predicted energy that would be radiated by gravitational waves.[26][27] For this work, Hulse and Taylor were awarded the Nobel Prize in Physics in 1993.[28] Further observations of this pulsar and others in multiple systems (such as the double pulsar system PSR J0737-3039) also agree with General Relativity to high precision.[29][30]

Direct observation

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Main articles: Gravitational-wave observatory and LIGO
File:Northern leg of LIGO interferometer on Hanford Reservation.JPG
Northern arm of the LIGO Hanford Gravitational-wave observatory.

Direct observation of gravitational waves was not possible for the many decades after they were predicted due to the minuscule effect that would need to be detected and separated from the background of vibrations present everywhere on Earth. A technique called interferometry was suggested in the 1960s and eventually technology developed sufficiently for this technique to become plausible.

In the present approach used by LIGO, a laser beam is split and the two halves are recombined after travelling different paths. Changes to the length of the paths or the time taken for the two split beams, caused by the effect of passing gravitational waves, to reach the point where they recombine are revealed as "beats". Such a technique is extremely sensitive to tiny changes in the distance or time taken to traverse the two paths. In theory, an interferometer with arms about 4 km long would be capable of revealing the change of space-time – a tiny fraction of the size of a single proton – as a gravitational wave of sufficient strength passed through Earth from elsewhere. This effect would be imperceptible to anybody and any other instrument on the planet (except for other interferometers of a similar size, such as the Virgo, GEO 600 and planned KAGRA and INDIGO detectors). In practice at least two interferometers would be needed, because any gravitational wave would be detected at both of these but other kinds of disturbance would generally not be present at both, allowing the sought-after signal to be distinguished from noise. This project was eventually founded in 1992 as the Laser Interferometer Gravitational-Wave Observatory (LIGO). The original instruments were upgraded between 2010 and 2015 (to Advanced LIGO), giving an increase of around 10 times their original sensitivity.[31]

LIGO operates two gravitational-wave observatories in unison, located 3,002 km (1,865 mi) apart: the LIGO Livingston Observatory (Lua error in package.lua at line 80: module 'strict' not found.) in Livingston, Louisiana, and the LIGO Hanford Observatory, on the DOE Hanford Site (Lua error in package.lua at line 80: module 'strict' not found.) near Richland, Washington. The tiny shifts in the length of their arms are continually compared and significant patterns which appear to arise synchronously are followed up to determine whether a gravitational wave may have been detected or if some other cause was responsible.

Initial LIGO operations between 2002 and 2010 did not detect any statistically significant events that could be confirmed as gravitational waves. This was followed by a multi-year shut-down while the detectors were replaced by much improved "Advanced LIGO" versions.[32]  In February 2015, the two advanced detectors were brought into engineering mode,[33] with formal science observations due to begin on 18 September 2015.[34]

Throughout the development and initial observations by LIGO, several "blind injections" of fake gravitational wave signals were introduced to test the ability of the researchers to identify such signals. To protect the efficacy of blind injections, only four LIGO scientists knew when such injections occurred, and that information was revealed only after a signal had been thoroughly analyzed by researchers.[35] No such tests were taking place in September 2015, however, when GW150914 was detected.[36]

The GW150914 event

Event detection

GW150914 was detected by the LIGO detectors in Hanford, Washington state, and Livingston, Louisiana, USA, at 09:50:45 UTC on 14 September 2015.[3][7] The LIGO detectors were operating in "engineering mode", meaning that they were operating fully but had not yet begun a formal "research" phase (which was due to commence three days later on 18 September), so initially there was a question as to whether the signals had been real detections or simulated data for testing purposes before it was ascertained that they were not tests.[37]

The chirp signal lasted over 0.2 seconds, and increased in frequency and amplitude in about 8 cycles from 35 Hz to 250 Hz.[2] The signal is in the audible range and has been described as resembling the "chirp" of a bird;[3] astrophysicists and other interested parties the world over excitedly responded by imitating the signal on social media upon the announcement of the discovery.[3][38][39][40] (The frequency increases because each orbit is noticeably faster than the one before during the final moments before merging.)

The trigger that indicated a possible detection was reported within three minutes of acquisition of the signal, using rapid ('online') search methods that provide a quick, initial analysis of the data from the detectors.[2] After the initial automatic alert at 09:54 UTC, a sequence of internal emails confirmed that no scheduled or unscheduled injections had been made, and that the data looked clean.[35][41] After this, the rest of the collaborating team was quickly made aware of the tentative detection and its parameters.[42]

More detailed statistical analysis of the signal, and of 16 days of surrounding data from 12 September to 20 October 2015, identified GW150914 as a real event, with a significance of over 5.1 sigma or a confidence level of 99.99994%.[43] Corresponding wave peaks were seen at Livingston seven milliseconds before they arrived at Hanford. Gravitational waves propagate at the speed of light, and the disparity is consistent with the light travel time between the two sites.[2] The waves had traveled at the speed of light for more than a billion years.[44]

At the time of the event, the Virgo gravitational wave detector (near Pisa, Italy) was offline and undergoing an upgrade; had it been online it would likely have been sensitive enough to also detect the signal, which would have greatly improved the positioning of the event.[3] GEO600 (near Hannover, Germany) was not sensitive enough to detect the signal.[2] Consequently, neither of those detectors was able to confirm the signal measured by the LIGO detectors.[3]

Astrophysical origin

File:MergingBlackHoles V2.jpg
Simulation of merging black holes radiating gravitational waves.

The event happened at a luminosity distance of 410+160
−180 megaparsecs[1][2] (determined by the amplitude of the signal),[3] or 1.3±0.6 billion light years, corresponding to a cosmological redshift of 0.09+0.03
−0.04 (90% credible intervals). Analysis of the signal along with the inferred redshift suggested that it was produced by the merger of two black holes with masses of 36+5
−4 times and 29±4 times the mass of the Sun (in the source frame), resulting in a post-merger black hole of 62±4 solar masses.[1] The mass–energy of the missing 3.0±0.5 solar masses was radiated away in the form of gravitational waves.[2]

During the final 20 milliseconds of the merger, the power of the radiated gravitational waves peaked at about 3.6×1049 watts – 50 times greater[45] than the combined power of all light radiated by all the stars in the observable universe.[2][3][11][12]

Across the 0.2-second duration of the detectable signal, the relative tangential (orbiting) velocity of the black holes increased from 30% to 60% of the speed of light. The orbital frequency of 75 Hz (half the gravitational wave frequency) means that the objects were orbiting each other at a distance of only 350 km by the time they merged. The phase changes to the signal's polarization allowed calculation of the objects' orbital frequency, and taken together with the amplitude and pattern of the signal, allowed calculation of their masses and therefore their extreme final velocities and orbital separation (distance apart) when they merged. That information showed that the objects had to be black holes, as any other kind of known objects with these masses would have been physically larger and therefore merged before that point, or would not have reached such velocities in such a small orbit. The highest observed neutron star mass is two solar masses, with a conservative upper limit for the mass of a stable neutron star of three solar masses, so that a pair of neutron stars would not have had sufficient mass to account for the merger (unless exotic alternatives exist, for example, boson stars),[1][2] while a black hole-neutron star pair would have merged sooner, resulting in a final orbital frequency that was not so high.[2]

The decay of the waveform after it peaked was consistent with the damped oscillations of a black hole as it relaxed to a final merged configuration.[2] Although the inspiral motion of compact binaries can be described well from post-Newtonian calculations,[46] the strong gravitational field merger stage can only be solved in full generality by large-scale numerical relativity simulations.[47][48]

The post-merger object is thought to be a rotating Kerr black hole with a spin parameter of 0.67+0.05
−0.07,[2][23] i.e. one with 2/3 of the maximum possible angular momentum for its mass.

Location in the sky

Gravitational wave instruments are whole-sky monitors with little ability to spatially resolve signals. A network of such instruments is needed to locate the source in the sky through triangulation. With only the two LIGO instruments in observational mode, GW150914's source location could only be confined to an arc on the sky. This was done via analysis of the 6.9+0.5
−0.4 ms time-delay, along with amplitude and phase consistency across both detectors. This analysis produced a credible region of 140 deg2 with a probability of 50% or 590 deg2 with a probability of 90% located mainly in the Southern Celestial Hemisphere,[1] in the rough direction of (but much farther than) the Magellanic Clouds.[3][7]

Simultaneous gamma-ray observation

The Gamma-Ray Burst Monitor (GBM) instrument on the Fermi Gamma-ray Space Telescope detected a weak gamma-ray burst above 50 keV that started 0.4 seconds after the LIGO event and had a positional uncertainty region that overlapped that of the LIGO observation. Although it is not certain that the two observations are from the same event, and the GBM event may possibly be just noise, the Fermi team calculates the odds of that being a coincidence at only 0.22%.[49]

However, observations using the INTEGRAL telescope, through the all-sky SPI-ACS instrument, indicate that the amount of energy in gamma-ray and hard X-ray emission from the event was less than one part in a million of the energy emitted in the form of gravitational waves, concluding that "this limit excludes the possibility that the event is associated with substantial gamma-ray radiation, directed towards the observer." If the signal observed by the Fermi GBM was genuinely astrophysical, SPI-ACS would have detected it with a significance of 15 sigma above the background.[50] The AGILE space telescope also did not detect a gamma-ray counterpart of the event.[51]

Black hole mergers of the type thought to have produced the gravitational wave event are not expected to produce gamma-ray bursts, as stellar-mass black hole binaries are not expected to have large amounts of orbiting matter. Avi Loeb has theorised that if a massive star is rapidly rotating, the centrifugal force produced during its collapse will lead to the formation of a rotating bar that breaks into two dense clumps of matter with a dumbbell configuration that becomes a black hole binary, and at the end of the star's collapse it triggers a gamma-ray burst.[52][53] Loeb suggests that the 0.4 second delay is the time it took the gamma-ray burst to cross the star, relative to the gravitational waves.[53][54]

Other follow-up observations

The reconstructed source area was targeted by follow-up observations covering radio, optical, near infra-red, X-ray, and gamma-ray wavelengths along with searches for coincident neutrinos.[1] However, because LIGO had not yet started its science run, notice to other telescopes was delayed.[citation needed]

The ANTARES telescope detected no neutrino candidates within ±500 seconds of GW150914. The IceCube Neutrino Observatory detected three neutrino candidates within ±500 seconds of GW150914. One event was found in the southern sky and two in the northern sky. This was consistent with the expectation of background detection levels. None of the candidates were compatible with the 90% confidence area of the merger event.[55] Although no neutrinos were detected, the lack of such observations provided a limit on neutrino emission from this type of gravitational wave event.[55]

Observations by the Swift Gamma-Ray Burst Mission of nearby galaxies in the region of the detection, two days after the event, did not detect any new X-ray, optical or ultraviolet sources.[56]

Announcement

File:PhysRevLett.116.061102.pdf
GW150914 announcement paper —
click to access

The announcement of the detection was made on 11 February 2016[3] at a news conference in Washington, D.C. by David Reitze, the executive director of LIGO,[5] with a panel comprising Gabriela González, Rainer Weiss and Kip Thorne, of LIGO, and France A. Córdova, the director of NSF.[3] Barry Barish delivered the first presentation on this discovery to a scientific audience simultaneously with the public announcement.[57]

The initial announcement paper was published during the news conference in Physical Review Letters,[2] with further papers either published shortly afterwards[15] or immediately available in preprint form.[58]

Awards and recognition

In May 2016, the full collaboration, and in particular Ronald Drever, Kip Thorne, and Rainer Weiss, received the Special Breakthrough Prize in Fundamental Physics for the observation of gravitational waves.[59] Drever, Thorne, Weiss, and the LIGO discovery team also received the Gruber Prize in Cosmology.[60]

Implications

The observation was heralded as inaugurating a new era of gravitational-wave astronomy. Prior to this detection, astrophysicists and cosmologists have been able to make observations based upon electromagnetic radiation (including visible light, X-rays, microwave, radio waves, gamma rays), and particle-like entities (cosmic rays, stellar winds, neutrinos, and so on). These have significant limitations - light and other radiation may not be emitted by many kinds of objects, and can also be obscured or hidden behind other objects. Objects such as galaxies and nebulae can also absorb, re-emit, or modify light generated within or behind them, and compact stars or exotic stars may contain material which is dark and radio silent, and as a result there is little evidence of their presence other than through their gravitational interactions.[61][62]

Expectations for detection of future binary merger events

The Advanced LIGO is predicted to detect five more black hole mergers like GW150914 in its next observing campaign, and then 40 binary star mergers each year, in addition to an unknown number of more exotic gravitational wave sources, some of which may not be anticipated by current theory.[7]

Planned upgrades are expected to double the signal-to-noise ratio, expanding the volume of space in which events like GW150914 can be detected by a factor of ten. Additionally, Advanced Virgo, KAGRA, and a possible third LIGO detector in India will extend the network and significantly improve the position reconstruction and parameter estimation of sources.[2]

Evolved Laser Interferometer Space Antenna (eLISA) is a proposed space based observation mission to detect gravitational waves. With the proposed sensitivity range of eLISA, merging binaries like GW150914 would be detectable about 1000 years before they merge, providing for a class of previously unknown sources for this observatory if they exist within about 10 megaparsecs.[15] LISA Pathfinder, eLISA's technology development mission, was launched in December 2015.[44]

Lessons for stellar evolution and astrophysics

The masses of the two pre-merger black holes provide information about stellar evolution. Both black holes were more massive than previously discovered stellar-mass black holes, which were inferred from X-ray binary observations. This implies that the stellar winds from their progenitor stars must have been relatively weak, and therefore that the metallicity (mass fraction of chemical elements heavier than hydrogen and helium) must have been less than about half the solar value.[15]

The fact that the pre-merger black holes were present in a binary star system, as well as the fact that the system was compact enough to merge within the age of the universe, constrains either binary star evolution or dynamical formation scenarios, depending on how the black hole binary was formed. A significant number of black holes must receive low natal kicks (the velocity a black hole gains at its formation in a core-collapse supernova event), otherwise the black hole forming in a binary star system would be ejected before and an event like GW would be prevented.[15] The survival of such binaries, through common envelope phases of high rotation in massive progenitor stars, may be necessary for their survival.[clarification needed] The majority of the latest black hole model predictions comply with these added constraints.[citation needed]

The discovery of the GW merger event increases the lower limit on the rate of such events, and rules out certain theoretical models that predicted very low rates of less than 1 Gpc−3yr−1 (one event per cubic gigaparsec per year).[2][15] Analysis resulted in lowering the previous upper limit rate on events like GW150914 from ~140 Gpc−3yr−1 to 17+39
−13 Gpc−3yr−1.[63]

Impact on future cosmological observation

Measurement of the waveform and amplitude of the gravitational waves from a black hole merger event makes possible accurate determination of its distance. The accumulation of black hole merger data from cosmologically distant events may help to create more precise models of the history of the expansion of the universe and the nature of the dark energy that influences it.[64][65]

The earliest universe is opaque since the cosmos was so energetic then that most matter was ionized and photons were scattered by free electrons.[66] However, this opacity would not affect gravitational waves from that time (if they are capable of being detected), allowing a window to observe the cosmos prior to the earliest time that we can presently view. Gravitational-wave astronomy therefore may some day allow direct observation of the earliest history of the universe before observation based upon light, radio and other electromagnetic waves became possible.[2][14][15][16][17]

Tests of general relativity

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Main article: Tests of general relativity

The inferred fundamental properties, mass and spin, of the post-merger black hole were consistent with those of the two pre-merger black holes, following the predictions of general relativity. This is the first test of general relativity in the very strong-field regime.[2][14] No evidence could be established against the predictions of general relativity.[14]

The opportunity was limited in this signal to investigate the more complex general relativity interactions, such as tails produced by interactions between the gravitational wave and curved space-time background. Although a moderately strong signal, it is much smaller than that produced by binary-pulsar systems. In the future stronger signals, in conjunction with more sensitive detectors, could be used to explore the intricate interactions of gravitational waves as well as to improve the constraints on deviations from general relativity.[14]

Speed of gravitational waves and limit on possible mass of graviton

The speed of gravitational waves (vg) is predicted by general relativity to be the speed of light (c). The extent of any deviation from this relationship can be parameterized in terms of the mass of the hypothetical graviton. The graviton is an elementary particle that plays the role of force carrier in speculative quantum theories about gravity. It is expected to be massless if, as it appears, gravitation has an infinite range. (This is because the more massive a gauge boson is, the shorter is the range of the associated force; as with the infinite range of electromagnetism, which is due to the massless photon, the infinite range of gravity implies that any associated force-carrying particle would also be massless.) If the graviton were not massless, gravitational waves would propagate below lightspeed, with lower frequencies (ƒ) being slower than higher frequencies, leading to dispersion of the waves from the merger event.[14] No such dispersion was observed.[14][23] The observations of the inspiral slightly improve (lower) the upper limit on the mass of the graviton from Solar System observations to 2.1×10−58 kg, corresponding to 1.2×10−22 eV/c2 or a Compton wavelength (λg) of greater than 1013 km, roughly 1 light-year.[2][14] Using the lowest observed frequency of 35 Hz, this translates to a lower limit on vg such that the upper limit on 1-vg /c is ~ 4×10−19.[note 5]

See also

Notes

  1. ↑ The ringdown phase is the settling down of the merged black hole into a sphere.[6]
  2. ↑ The name format is the initials of "Gravitational Wave" plus the date format yy-mm-dd of 2015-09-14 making the name GW150914.
  3. ↑ Diameter of a proton ~ 1.68–1.74 femtometer (1.68–1.74×10-15m); ratio of proton/1000/4000 m = ~4×10-22; width of a human hair ~ 0.02–0.04 millimeter (0.02–0.04×10-3m); distance to Proxima Centauri ~ 4.423 light-years (4.184×1016 m); ratio of hair/distance to star = 5–10×10-22
  4. ↑ Despite the tremendous energy emission, the effects of the gravitational waves on a human located only one AU from the merger event would have been minor and survivable.[13]
  5. ↑ Based on v_g^2/c^2 = 1-\tfrac{c^2}{\lambda_g^2 f^2}, obtainable from the "Tests of general relativity …" paper (p. 13, "Thus, we have...") and the Planck–Einstein relation.[14]

References

  1. ↑ 1.0 1.1 1.2 1.3 1.4 1.5 1.6 1.7 Lua error in package.lua at line 80: module 'strict' not found.
  2. ↑ 2.00 2.01 2.02 2.03 2.04 2.05 2.06 2.07 2.08 2.09 2.10 2.11 2.12 2.13 2.14 2.15 2.16 2.17 2.18 2.19 2.20 Lua error in package.lua at line 80: module 'strict' not found.
  3. ↑ 3.00 3.01 3.02 3.03 3.04 3.05 3.06 3.07 3.08 3.09 3.10 3.11 Lua error in package.lua at line 80: module 'strict' not found.
  4. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  5. ↑ 5.0 5.1 Lua error in package.lua at line 80: module 'strict' not found.
  6. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  7. ↑ 7.0 7.1 7.2 7.3 7.4 Lua error in package.lua at line 80: module 'strict' not found.
  8. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  9. ↑ 9.0 9.1 Lua error in package.lua at line 80: module 'strict' not found.
  10. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  11. ↑ 11.0 11.1 Lua error in package.lua at line 80: module 'strict' not found.
  12. ↑ 12.0 12.1 Lua error in package.lua at line 80: module 'strict' not found.
  13. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  14. ↑ 14.0 14.1 14.2 14.3 14.4 14.5 14.6 14.7 14.8 Lua error in package.lua at line 80: module 'strict' not found.
  15. ↑ 15.0 15.1 15.2 15.3 15.4 15.5 15.6 Lua error in package.lua at line 80: module 'strict' not found.
  16. ↑ 16.0 16.1 CNN quoting Prof. Martin Hendry (University of Glasgow, LIGO) - "Detecting gravitational waves will help us to probe the most extreme corners of the cosmos -- the event horizon of a black hole, the innermost heart of a supernova, the internal structure of a neutron star: regions that are completely inaccessible to electromagnetic telescopes."
  17. ↑ 17.0 17.1 Lua error in package.lua at line 80: module 'strict' not found.
  18. ↑ 18.0 18.1 Lua error in package.lua at line 80: module 'strict' not found.
  19. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  20. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  21. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  22. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  23. ↑ 23.0 23.1 23.2 Lua error in package.lua at line 80: module 'strict' not found.
  24. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  25. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  26. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  27. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  28. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  29. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  30. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  31. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  32. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  33. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  34. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  35. ↑ 35.0 35.1 Lua error in package.lua at line 80: module 'strict' not found.
  36. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  37. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  38. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  39. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  40. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  41. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  42. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  43. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  44. ↑ 44.0 44.1 Lua error in package.lua at line 80: module 'strict' not found.
  45. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  46. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  47. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  48. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  49. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  50. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  51. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  52. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  53. ↑ 53.0 53.1 Lua error in package.lua at line 80: module 'strict' not found.
  54. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  55. ↑ 55.0 55.1 Lua error in package.lua at line 80: module 'strict' not found.
  56. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  57. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  58. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  59. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  60. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  61. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  62. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  63. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  64. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  65. ↑ Lua error in package.lua at line 80: module 'strict' not found.
  66. ↑ Lua error in package.lua at line 80: module 'strict' not found.

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