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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://​journ​als​.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://​journ​als​.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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