Authors: Davide Gerosa, Emanuele Berti
First Author’s Institution: Institute for Gravitational Wave Astronomy, University of Birmingham, Birmingham, B15 2TT, UK
It is common knowledge that nothing in the universe can escape a Black Hole. But are there places in the universe from which a Black Hole cannot escape?
This seemingly silly conundrum is important to explain another mystery, born out of a recent LIGO-Virgo discovery. “These Black Holes Shouldn’t Exist, but There They Are”, quoted the New York Times. The Los Angeles Times called it the ‘Impossible Black Hole’. The event making news was GW190521: the most dramatic collision of two black holes ever seen by the gravitational wave observatories. The two black holes weighed around 85 and 66 times the mass of the Sun, before colliding to form a gargantuan black hole weighing a whopping 142 times the mass of the Sun. The remaining deficit, totalling 9 solar masses, was released as gravitational wave energy, making it the most energetic event in the universe that we’ve ever detected.
The reason why many astrophysicists believed that such massive black holes shouldn’t exist is a feature of core-collapse supernovae that give birth to them. These explosions occur when very massive stars (heavier than about 8 times the mass of the Sun) run out of fuel to sustain nuclear fusion, and collapse under their own gravity. A large amount of mass is ejected, while the rest implodes uncontrollably to form the black hole. How heavy this remnant black hole is depends on the mass of the initial star. Supernova models easily predict the formation of stellar-mass black holes in the mass range from 5 solar masses up to around 60 solar masses.
Producing even heavier black holes requires the initial star to be heavier than around 130 solar masses. The collapse of these stars leads to the creation of free electron and positron pairs out of collisions of atomic nuclei with gamma rays. This partially stops the collapse and leads to a runaway thermonuclear fusion reaction that completely blows the star away—leaving no remnant black hole behind. The resultant explosion, called a pair-instability supernova, prevents the formation of black holes between the mass range of around 60 to 150 solar masses. This is termed as the ‘upper mass gap’ of stellar-mass black holes.
A hint of how such ‘upper mass gap’ black holes could form was already given to us by GW150914, the first-ever gravitational wave detection. That event was a merger of a 36 solar mass black hole with a 29 solar mass black hole, forming a ‘second-generation’ (2g) black hole weighing 62 solar masses. This just about clears the lower end of the upper mass gap weight category. Other events, like GW170729, GW170823, and GW170818 have been observed to leave behind 2g black holes with masses touching the upper mass gap. Could these black holes in turn participate in future mergers and form remnants that populate the upper mass gap?
This is viable but with an important caveat that takes us back to our opening conundrum: We need places from which black holes cannot escape!
A big characteristic of binary black hole mergers is that the gravitational radiation they emit is not uniform in all directions. As a result, the conservation of linear momentum imparts a ‘kick’ to the newly formed 2g black hole. There are a number of fascinating things that we can study about these kicks, but when it comes to filling in the upper-mass gap, what matters is how fast the remnant black hole is flung off.
Just like a rocket needs a sufficiently high thrust to move it fast enough to escape the Earth’s gravity, a black hole getting a high enough recoil can escape its stellar environment into the void. Whether it escapes or not depends on the escape velocity of the environment, which typically depends on how dense an environment is. Relatively less dense stellar clusters have escape speeds around 10 km/s, while the denser globular clusters have escape speeds of around 50 km/s. Nuclear star clusters, which exist at the cores of galaxies and form one of the densest stellar environments, have much stricter escape speed limits of greater than 100 km/s.
The authors of today’s paper simulated multiple mergers over time from an initial population of black holes in an environment characterized by a given escape speed. Their main objective was to estimate how many second generation black holes, remnants of previous mergers in the environment, got retained because their kicks did not exceed the escape velocity. These black holes could hence participate in future mergers detectable by LIGO-Virgo, thereby forming even heavier black holes which populate the upper mass gap.
Figure 1 shows that environments with higher escape speeds are more likely to retain 2g black holes, and hence harbor a larger population of black holes in the upper mass gap. Figure 2 confirms that any detection made in the upper mass gap contains black holes which are themselves remnants of a previous merger. Even though theoretical models predict that no black hole can be formed in the upper mass gap, a single detection of such an object would point to the existence of environments that prevent their black holes from escaping the dance floor of gravity.
That is why GW190521 is so tantalizing: not only is its remnant the heaviest black hole we’ve seen through gravitational waves, but each of the component black holes is heavy enough to be a part of the upper mass gap. This makes it quite likely that one of them, if not both, were second generation black holes retained in a dense enough environment. It is only the first piece of the puzzle that is the upper mass gap, but simulations like the one in today’s paper help us prepare for the other pieces that future LIGO-Virgo observing runs will inevitably shower.
Astrobite edited by: Luna Zagorac
Featured image credit: Arstechnica