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Astrophysics: 3 recent discoveries that illuminate our vision of the universe

Gravitational waves : a new era for astronomy

with Isabelle Dumé, Science journalist
On November 3rd, 2021 |
4min reading time
Paul Ramond modifiée
Paul Ramond
Post-doctoral Fellow in Astrophysics at Université Paris Dauphine-PSL
Key takeaways
  • Predicted by Albert Einstein in 1916, gravitational waves can only be produced by accelerating very massive objects (such as black holes) at close to the speed of light.
  • Gravitational waves from a “binary system”, or pair of black holes, were first observed in 2015, thanks to the LIGO observatory in the USA.
  • Since this first observation, about 50 more coalescence events have been detected, advancing many fields of research and the emergence of “gravitational astronomy”.
  • LIGO is a collaborative project involving more than 1,000 researchers and engineers in over 20 countries.
  • The next most promising future project is the European Laser Interferometer Space Antenna (LISA) observatory which should be operational in 2034.

The first ever direct obser­va­tion of gra­vi­ta­tio­nal waves in 2015 by the LIGO Scien­ti­fic Col­la­bo­ra­tion in the US is undoub­ted­ly one of the big­gest scien­ti­fic dis­co­ve­ries of the last decade, or even this cen­tu­ry. Six years later, what can we say about these waves, and why is it so impor­tant to stu­dy them ?

Gra­vi­ta­tio­nal waves (GWs), first pre­dic­ted to exist by Albert Ein­stein in 1916, allow for a brand-new way of loo­king at the uni­verse. Before their detec­tion, astro­no­mers could only observe the sky using visible light, and other types of elec­tro­ma­gne­tic radia­tion (inclu­ding infra­red, ultra­vio­let and gam­ma rays). 

While light is the pro­pa­ga­tion of elec­tro­ma­gne­tic fields vibra­ting in space and time, GWs are com­ple­te­ly dif­ferent : they are ripples in the very fabric of space-time itself. They can thus be emit­ted by non-lumi­nous objects.

Studying black hole mergers

Crea­ting such ripples in the (rather rigid) fabric of space-time is not easy though. Indeed, GWs can only be pro­du­ced by acce­le­ra­ting very small and extre­me­ly mas­sive objects close to the speed of light. The best can­di­dates are the­re­fore black holes (which are the most com­pact objects in the uni­verse), and cer­tain very dense stars known as neu­tron stars (which are bet­ween 1.4 and 2.4 solar masses with a dia­me­ter of less than 20 km). To com­pare, the Sun has a dia­me­ter of 1.39 mil­lion kilometres.

In gene­ral, an iso­la­ted black hole does not pro­duce GWs. It needs a com­pa­nion to which it remains bound for a long time (much like Earth is bound to the Moon) to form what is cal­led a bina­ry sys­tem. As they are extre­me­ly dense, the black holes deform space-time in their vici­ni­ty as they orbit each other, gene­ra­ting GW ripples that pro­pa­gate across the uni­verse at the speed of light.

As it emits these GWs, the bina­ry loses some of the ener­gy that binds the black holes, which end up spi­ral­ling ever clo­ser to each other. This infer­nal waltz pro­duces more and more intense GWs (that can tra­vel bil­lions of light-years across the uni­verse) until the black holes even­tual­ly merge. From time to time, one of these bina­ries pro­duces GWs with an ampli­tude that is just large enough to be detec­ted when it reaches Earth, even though the signal is extre­me­ly weak.

The LIGO detection

The first signal from such a bina­ry black-hole coa­les­cence, which occur­red approxi­ma­te­ly 1.3 bil­lion light-years from Earth, was detec­ted in Sep­tem­ber 2015 by an ins­tru­ment cal­led LIGO (for Laser Inter­fe­ro­me­ter Gra­vi­ta­tio­nal-Wave Obser­va­to­ry)12. The coa­les­cence includes the “ins­pi­ral” (when the black holes become clo­ser), the “mer­ger” (when they touch) and the “ring­down” (when the new­ly for­med, big­ger black hole relaxes into a stea­dy state). 

a single black hole of 62 solar masses. The 3 solar mass dif­fe­rence was enti­re­ly conver­ted into gra­vi­ta­tio­nal ener­gy car­ried by the GWs.

LIGO is a col­la­bo­ra­tive pro­ject with over 1000 scien­tists and engi­neers from more than 20 coun­tries, and three of its mem­bers were awar­ded the 2017 Nobel Prize in Phy­sics3. It took near­ly 50 years of intense research to build the GW detec­tors, and in June 2016 the resear­chers announ­ced that they had obser­ved a secon­da­ry bina­ry black hole coa­les­cence4. The obser­va­tion was made on 26 Decem­ber 2015, and this time, the black holes were about 1.4 bil­lion light-years away. Rough­ly 50 such mer­ger events have been detec­ted since this time. All these dis­co­ve­ries great­ly advan­ced many research fields and kicked off the era of gra­vi­ta­tio­nal-wave astronomy.

Tiny length changes

Ins­tru­ments like LIGO and other ground-based GW detec­tors, such as Vir­go in Ita­ly and Kagra in Japan, rely on an advan­ced sen­sing method cal­led laser inter­fe­ro­me­try. This tech­nique has long been used to detect dif­ferent sorts of signals, but it had never been pushed to the limit nee­ded to detect the very weak signals that GWs produce. 

The LIGO faci­li­ty basi­cal­ly works by sen­ding twin laser beams down two 4 km-long “arms” arran­ged in an L‑shape and kept under a near-per­fect vacuum. The beams are reflec­ted by mir­rors pre­ci­se­ly posi­tio­ned at the ends of each arm.  As a GW passes through the obser­va­to­ry, it causes extre­me­ly tiny dis­tor­tions in the dis­tance tra­vel­led by each laser beam. The ins­tru­ment is thus able to mea­sure the local contrac­tion and expan­sion of space-time cau­sed by the GW.

The extreme sen­si­ti­vi­ty of the ins­tru­ment means that it is prey to all sorts of exter­nal vibra­tions (such as those from planes flying by and waves on a dis­tant shore). LIGO engi­neers the­re­fore had to desi­gn seve­ral inge­nious noise-reduc­tion sys­tems that not only great­ly enhance the pre­ci­sion of the detec­tors, but also allow them to dif­fe­ren­tiate bet­ween ter­res­trial arte­facts and the pre­cious GW signals.

By mea­su­ring how long it takes for the laser beams to tra­vel along an arm, resear­chers can extract infor­ma­tion such as the fre­quen­cy and ampli­tude of the GW from the signal. These quan­ti­ties are of major impor­tance since they contain key phy­si­cal infor­ma­tion about the source of the wave, such as its dis­tance from Earth and its posi­tion in the sky, as well its mass and whe­ther it is a black hole or a neu­tron star.

Future detectors

The cha­rac­te­ris­tics of inter­fe­ro­me­ters like LIGO makes them sen­si­tive only to gra­vi­ta­tio­nal waves within a cer­tain fre­quen­cy band, from about 10 Hz to 10 kHz, which cor­res­ponds to black holes of about 10 to 100 solar masses. 

To extend this fre­quen­cy range, the most pro­mi­sing future pro­ject is the Laser Inter­fe­ro­me­ter Space Anten­na (LISA)5. This Euro­pean space-based obser­va­to­ry, due to come online in 2034, will tar­get fre­quen­cies in the lower mil­li­hertz range to detect waves from the mer­ger of much big­ger black holes. These “super­mas­sive” objects are found at the centres of most galaxies – inclu­ding our Mil­ky Way – and have masses that are mil­lions or even bil­lions of times that of the Sun.

LISA should also be able to observe “asym­me­tric” pairs, such as a neu­tron star orbi­ting a super­mas­sive black hole, and even the so-cal­led “cos­mic gra­vi­ta­tio­nal-wave back­ground”, which is very impor­tant for cos­mo­lo­gy since it contains infor­ma­tion about the pri­mor­dial GW crea­ted right after the Big-Bang6. Far more pre­cise than its ter­res­trial cou­sins, LISA will be a mil­lions-of-kilo­metre-long ins­tru­ment consis­ting of three tiny robots posi­tio­ned in an equi­la­te­ral tri­angle pat­tern in solar orbit just behind Earth.

1https://​jour​nals​.aps​.org/​p​r​l​/​a​b​s​t​r​a​c​t​/​1​0​.​1​1​0​3​/​P​h​y​s​R​e​v​L​e​t​t​.​1​1​6​.​0​61102
2https://​www​.ligo​.cal​tech​.edu
3https://​www​.nobel​prize​.org/​p​r​i​z​e​s​/​p​h​y​s​i​c​s​/​2​0​1​7​/​p​r​e​s​s​-​r​e​l​ease/
4https://​jour​nals​.aps​.org/​p​r​l​/​a​b​s​t​r​a​c​t​/​1​0​.​1​1​0​3​/​P​h​y​s​R​e​v​L​e​t​t​.​1​1​6​.​2​41103
5https://​sci​.esa​.int/​w​e​b​/​lisa/
6https://link.springer.com/article/10.1007%2Fs10714-020–02691‑1

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