by Natalie Wolchover
from
QuantaMagazine Website
Quanta Magazine point physicists toward the theory of quantum gravity,
or is it a red herring?
In a 1972 lecture at the University of Oxford, a young physicist named William Unruh asked the audience to imagine a fish screaming as it plunges over a waterfall.
The water falls so fast in this fictitious cascade that it exceeds the speed of sound at a certain point along the way. After the fish tumbles past this point, the water sweeps its screams downward faster than the sound waves can travel up, and the fish can no longer be heard by its friends in the river above.
Something similar happens, Unruh explained, when you fall into a black hole.
As you approach one of these superdense objects, the fabric of space and time becomes increasingly curved  equivalent to strengthening gravity, according to Albert Einstein's general theory of relativity.
At a point of no return known as the "event horizon," the spacetime curvature becomes so steep that signals can no longer climb to the outside world. Within the event horizon, even light is held captive by the black hole's gravity, rendering black holes invisible.
In the years following Unruh's talk, black holes  places where general relativity and quantum mechanics, the two pillars of modern physics, meet and crumble in paradox  rose from obscurity to become leitmotifs in the quest for an allencompassing theory of "quantum gravity."
Meanwhile, Unruh's acoustic analogy turned out to work even better than he first thought. In a seminal 1981 paper, he showed that black hole event horizons and sonic horizons in systems like his waterfall  which are now referred to as sonic black holes  can be described by identical equations.
Considering their "amazing mathematical similarities," Unruh, a professor at the University of British Columbia in Vancouver, said recently,
Researchers began plumbing the physics of sonic black holes for clues about actual black holes.
And in recent years, they've started creating sonic black holes in the lab and devising increasingly sophisticated analogue experiments.
This past summer, Jeff Steinhauer of the Technion in Haifa, Israel, reported the ultimate find:
Lucy ReadingIkkanda for Quanta Magazine
Hawking's prediction that black holes radiate heat and eventually evaporate completely gives rise to the profound "information paradox," which asks what happens to information about the stuff that fell into them.
Hawking's calculation suggests that this information is lost, essentially leaking out of the universe when it enters a black hole; in that case, the framework of quantum mechanics, which treats information as the universe's fundamental, indestructible currency, must be abandoned.
But if information is preserved, as most physicists believe, then Hawking's prediction is wrong, and the task for any theory of quantum gravity is to reveal the flaw in his logic.
The information paradox,
For all its importance, Hawking's calculation cannot be tested directly; the radiation from actual black holes is far too faint to detect.
The measurement of the analogous effect in a sonic black hole  in this case, quantum units of sound radiating outward from a sonic horizon  therefore brings a longstanding question to a head:
Some researchers see indirect evidence for Hawking radiation in Steinhauer's experiment.
In a paper (What Can We Learn From Analogue Experiments?) posted online last month, the physicistturnedphilosopher Karim Thebault of the University of Bristol in England argued that,
Others see a red herring...
Daniel Harlow, a theoretical physicist at Harvard University, deemed the experiment,
The question of which interpretation is correct comes down to what, exactly, Hawking's calculation 42 years ago revealed about the universe.
Surprisingly, he showed that black holes aren't black; random quantum jitter makes them glow (Shiny Darkness). Everywhere in spacetime, pairs of "virtual" particles are constantly arising and mutually annihilating.
Hawking realized that when these pairs arise straddling the horizon of a black hole, one virtual particle will get sucked in while its partner escapes, preventing their mutual destruction.
The escaped particle becomes real, stealing the energy needed for the upgrade from the black hole's gravitational field. Meanwhile the infalling particle acquires negative energy, lowering the energy of the black hole.
Thus, one radiated particle at a time, the black hole blinks out of existence, ultimately leaving no trace:
William Unruh, a physicist at the University of British Columbia, found an analogy connecting black holes and sonic black holes in a seminal 1981 paper. Courtesy of William Unruh
Therein lies the paradox...
According to quantum mechanics, the probabilities of all possible states of particles in the universe must respect "unitarity," evolving in such a way that the universe's past states can in principle always be uniquely determined by rewinding from its present state.
But if information is lost when a black hole evaporates into a featureless gas of Hawking radiation, then the universe's past can't be gleaned from the present, and quantum mechanics breaks down.
Or perhaps Hawking erred...
To do his calculation, he made a key assumption:
Physicists believe that this is an approximation; zoom in far enough on Einstein's spacetime continuum, and a more fundamental, quantum form of gravity emerges.
But whereas quantum gravity surely becomes important near a black hole's superdense center, known as its "singularity," Hawking assumed that he could gloss over this shortdistance physics in his description of quantum fluctuations at the horizon, where gravity is comparatively mild.
According to general relativity, the slope of spacetime is gentle enough at the horizon of a typical supermassive black hole (like those at the centers of many galaxies) that an astronaut floating past it wouldn't even notice.
In 1981, Unruh discovered that Hawking's approximation scheme can also be applied to fluids.
Like spacetime, fluids appear continuous on large scales even though deep down they're made of discrete atoms. Unruh showed that, just as pairs of particles fluctuate in and out of spacetime, vibrations called "phonons," the quantum units of sound, should surface throughout fluids.
And when pairs of phonons arise near the sonic horizon of a sonic black hole, they should get wrenched apart and rendered permanent, producing the sonic analogue of Hawking radiation.
This is the phenomenon that Jeff Steinhauer reported in August in Nature Physics, after toiling over his experiment since 2009,
He created an exotic fluid called a "BoseEinstein condensate" out of supercooled rubidium atoms.
He then got it flowing, and zapped the fluid partway along its flow path with a laser, accelerating it to a supersonic speed and creating a sonic horizon. Finally, Steinhauer measured quantum entanglement between pairs of phonons on either side of this horizon, consistent with sonic Hawking radiation.
The finding confirms that the fluid approximation works in the case of sonic black holes.
Jeff Steinhauer, a physicist at the Technion in Haifa, Israel, claims to have detected the acoustic analogue of Hawking radiation in a sonic black hole. Courtesy of Jeff Steinhauer
Unruh believes Hawking's approximation is correct...
In 2005, he and Ralf Schützhold of the University of DuisburgEssen in Germany showed that Hawking radiation consistently came out as a robust theoretical prediction in both sonic black holes and actual black holes, no matter what theoretical assumptions they made about the details of the shortdistance physics.
The smallscale properties of spacetime or fluids never affected the outcome of the calculation, suggesting that Hawking's approximation wasn't glossing over anything important.
Unruh interprets this to mean that effects from quantum gravity aren't capable of modifying Hawking radiation and rescuing information.
In his opinion, Steinhauer's result adds to the evidence that,
However, most quantum gravity researchers believe that information is preserved  including Hawking, who switched camps in the 2000s.
From their perspective, an analogue to Hawking radiation in sonic black holes says nothing about true black holes because the two are categorically different; whereas the fluid approximation is accurate in the case of sonic black holes, spacetime must not be approximately smooth at black hole event horizons.
Somehow, quantum gravity modifies horizons  and it must do so in an extreme way, to get around Unruh and Schutzhold's argument about the robustness of Hawking radiation.
Some thought experiments suggest that black holes might be empty shells that carry all their information plastered on their horizons and project it outward to the rest of the universe like holograms.
In that case, falling into a black hole would be less like a fish plunging over a waterfall and more like a bug going splat on a window.
In the majority opinion, the comparison with sonic black holes only reinforces how strange black holes and the theory of quantum gravity must be. Harlow, who takes this view, sees sonic black holes not as black hole analogues, but more like computer simulations that are running the wrong equations.
If you were to simulate the equations of quantum gravity,
by David Kaplan, Petr Stepanek and MK12
Music by
Steven Gutheinz from QuantaMagazine Website
explores black hole physics
and the problem of quantum
gravity.
