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Physicists observationally confirm Hawking’s black hole theorem for first time (news.mit.edu)
217 points by _Microft on July 1, 2021 | hide | past | favorite | 71 comments



Alright, I'm confused. How does this square with Hawking radiation? How can a black hole shrink without shrinking?

The article mentions both in the context that they are reconciled but not how they are reconciled.


They're not reconciled, it's just garbage reporting.

The 'area theorem' they are referring to was by Bekenstein and others, not Hawking. It's basically the equivalent of the second law of thermodynamics for black holes (dA/dt>=0 instead of dS/dt>=0). Hawking's insight was that this formula was wrong and the area could decrease due to radiation.


While I agree that the article should have mentioned black hole evaporation, I would like to point out that "dA/dt > 0" is commonly referred to as "Hawking's area theorem" as a quick online search can verify and Stephen Hawking certainly did publish on this topic.


It is a pity about the reporting.

But it is a fascinating area of research. I never expected that we could measure gravitational waves in our life time.


I'm amazed - to the point of skepticism - that with such minute forces they can extrapolate so much information and prove theories.

I mean I'm no astrophysicist, I like the "pop sci" bits, but when I look closer I'm seeing a lot of small numbers and statistics that imply something - e.g. exoplanets based on minute wobbles and brightness variations, water on said exoplanets based on spectrography. It's theories based on tiny but statistically significant data.

The pop sci then comes in and makes statements like "second Earth found!11", which is like, whoa hold on, when you look closer all they found is a wobble or dimness variation that kind of implies there might be a planet at a certain distance from its host star.

Anyway I don't dispute the findings or that there are exoplanets or whatever, I'm just impressed that they are able to make confident claims on what little information we can receive from here.


> e.g. exoplanets based on minute wobbles and brightness variations, water on said exoplanets based on spectrography.

The minute wobbles may be tiny, but they can plot a curve of those wobbles and see very clearly that it changes in a certain way that can only be caused by a planet (or something spherical and with a certain mass). If there was a competing theory of how you can get this exact curve in some other way, I am sure we would consider them as alternative possibilities and not be able to tell them apart, but as far as I know, there isn't any competing theories at all... so we can have very high confidence there's a planet there.

Regarding water detection: yeah, spectrography is just mind blowing, but again, given what we know, there's just nothing that could justify believing that when you detect radiation that fit exactly what you would expect from water molecules, that it could be something else instead... unless you come up with a convincing "something else", your only option is to conclude that the detection is accurate, otherwise you would need to stay open to the possibility of absolutely everything possibly having alternative explanations we haven't thought of yet (though every now and then, that indeed can happen and we need to adjust all our theories that are based on the changed body of knowledge), and progress would not be possible in any area (you need to accept something before you can build on top of it).


The problem is the 'pop sci' reporting. "Earth-like" or "second earth" could easily be swapped for "Venus-like" or "second venus" in 99% of cases where pop-sci uses "Earth like" and still be factually correct.

However, Wobbles and Transit photometry are done over time and plot trends which definitively show that something with a certain mass is orbiting with a certain period around the star. There isn't really anything else it could be except an exoplanet, unless our understanding of how physics works was way off, which we know it isn't.

as for Spectrography brabel sums it up in their comment very well.


I suppose Venus has a different enough thermal spectrum due to surface temperatures being 3x Earth's, roughly 900K vs 300K.

Also, Venus must have a big enough sulfur line in the atmosphere, which is absent in Earth atmosphere.

Probably Mars and Earth could be considered close, save for the oxygen line, but not Venus and Earth,


It's fascinating what's possible.

For example, we know more about the chemical composition of other galaxies than we know about the centre of the earth. Just because we can infer so much from their light spectrum.

(For empirical information about the centre of the earth, we are basically limited to seismic data and perhaps the magnetic field and bumps in gravity?)


Why not launch a probe and point its sensors at earth?


The Earth is opaque. I don’t have a source to cite for this, but I think you can check it easily enough.



We hardly resolve any individual stars in other galaxies (maybe some giant stars inside Andromeda?), so our idea of chemical composition of other galaxies is very... averaged.

We barely can resolve largest and closest exoplanets into a few pixels.


>We barely can resolve largest and closest exoplanets into a few pixels

For now...

https://arxiv.org/abs/1802.08421

https://www.youtube.com/watch?v=NQFqDKRAROI


This is seriously cool.

This also requires a helluva lot of delta-V from the telescope to realign with another planet.


>water on said exoplanets based on spectrography

Even though from a theoretical perspective it should be way easier and more reasonable to detect particular molecules on distant planets via spectroscopy compared than to detect things on the mind-blowingly minuscule scale of gravitational waves, I think distant spectroscopy might actually be more prone to error, or at least more prone to false positives.

Just speculating since I have zero expertise in this area, but part of it may be because light from all sorts of sources is reaching us all the time, while gravitational waves significant enough to be feasibly detected pretty much only come from the top percentile of the most energetic events in the universe.

I think if you can discern a gravitational wave-induced spacetime wobble at least once and infer the motion that could've caused it (e.g. black holes/neutron stars merging) and see it matches theoretical expectations, you may continue to have a lot of false negatives, but you probably aren't at high risk of future false positives.

Whereas with spectroscopy, there seem to be a lot of things that can cause both false positives and false negatives even if you do have many prior detections that you believe are accurate. For spectroscopy, both error rates should go down over time as technology and techniques improve, but it seems like it may potentially be an inherently more "murky" observation technique, even if it's far simpler and far less expensive than gravitational wave detection.

(Someone please correct me if I'm wrong about any of this, because there's a pretty good chance I am.)


It is not just gravitational waves, they look at light, with telescopes (visible, infra and ultra), spectrographs, interferometers, radio signals, gamma rays...

Then they combine all that info to come up with cohesive theories. LIGO just by itself would be almost useless.


Sometimes I think the claims are overstating things, but since nobody can use the claim to actually do anything it gets a pass.


I think what they really meant in the article is that it can never decrease through processes other than the radiation. E.g., BH mergers and so on, the area always increases.


Yes, black holes shrink because of Hawking radiation, but in reality this doesn't really happen because black holes are much colder than their surrounding space. Actually they are the coldest objects in nature. Stellar black holes have a temperature of a few Nanokelvins and the average temperature of space is 2.7 K so there's a net gain of energy/mass from absorbed photons from CMB radiation vs emitted photons via Hawking radiation. In order to have a higher temperature than the CMB a black hole would have to be really small with a mass about half of that of the moon.


> In order to have a higher temperature than the CMB a black hole would have to be really small with a mass about half of that of the moon.

Either that, or you just wait a couple eternities for the CMB to cool down enough.


Or you make a smaller one and watch it shrink. It is theoretically possible to construct a smaller black hole by cramming the necessary mass/energy into a small enough space. (Plug a death star into the LHC's big brother.) Such a hole would be very hot and short-lived.


Or primordial black holes with such a small mass actually do exist, who knows...


how can the temperature of a black hole make sense? Is it the temperature of the singularity point? Is it the temperature of the space inside the event horizon (but it can't be, as that space is empty)?


"Temperature" in this case refers to the amount of energy they emit due to hawking radiation.

By comparing to a black-body curve, you can define a temperature for the hole. Obviously it's not a real object with a real temperature -- if it were, I believe the temperature might be infinite -- but this still works for the purposes of deciding whether it'll grow or shrink.


Temperature has several definitions that produce the same number under normal circumstances but may or may not be applicable in extreme circumstances. In this case, I imagine they could be using the thermodynamic definition (dE/dS, the marginal change in energy per marginal change in entropy - I’m not sure if a BH has well-defined entropy) or something to do with the emission curve of space around the black hole. I vaguely recall something about empty space behaving like a blackbody under a gravitational gradient, so maybe they can use that. You could also use amount of Hawking radiation per surface area. It’s possible that some of those produce the same number.


My understanding is it's the temperature of the event horizon: because it doesn't emit any blackbody radiation, other than the tiny amount from Hawking radiation, any heat measurement from it would be approximately 0k.


The Hawking radiation is exactly its black body radiation.


it is a phenomenon at the event horizon at with radiation is emitted in a way comparable to the radiation produced by every object according to temperature


It _will_ happen, but first dark energy needs to be strong enough to expand the universe fast enough (faster than light) so that CMB wouldn't be able to reach anything.


Well there are already portions of space that are expanding faster than the speed of light relative to our position. (see cosmic horizon). The CMB is not just a glowing heat somewhere far away, it's everywhere in the universe in every volume of space. The moment when every point in space (on a Planck-lenght-scale i guess) will be expanding faster than the speed of light relative to one another, than space-time itself will rip apart and that's the end of our universe - at least that is what the Big-Rip theory proposes.


That's my point exactly. Maybe you misunderstood.


Finite speed of expansion is enough.

The temperature of the CMB just needs to drop below the temperature of the black hole.


From the outside they must look cold since they can't radiate heat any more than light. That doesnt imply anything about the inside.


What's "inside" of a black hole, meaning behind the event horizon is forever causally cut off from our universe. The Hawking radiation comes from the space around the event horizon. In theory black holes can become very hot if their mass is small. This happens at the end of their life which is in the order of 10^80 years for stellar black holes.

Here is a calculator to play with some values. https://www.vttoth.com/CMS/physics-notes/311-hawking-radiati...


Note that this evaporation time assumes a universe at absolute zero. That 10^80 years can't even begin until the CMBR cools enough, perhaps 10^40 years.

Admittedly that's an eyeblink compared to the evaporation time scale, but it does mean that we won't observe any evaporation until many orders of magnitude longer than the universe has existed.


Or unless you manufacture or discover a low–mass black hole


That's right. If we could create one in a supercollider, it would would be so small that it would be hot enough to evaporate instantly.

There might also be a range of primordial black holes formed directly out of pre-CMBR energy. They'd have to be small enough to be hotter than the CMBR, but not so hot that they'd already have evaporated in the last 14 billion years. That's a relatively narrow range, all things considered, but if primordial black holes exist at all then they could exist at any range.


The inside is empty space.


The inside is empty time, space waved you a goodbye at the event horizon.


Exactly what I came here to ask. Is Hawking's theory that the area never decreases or that it does not decrease in a black hole merger as was tested here. "central law for black holes predicts that the area of their event horizons — the boundary beyond which nothing can ever escape — should never shrink" this seems to imply the former to me.

Does that mean with Hawking radiation the black hole effectively evaporates by loosing mass (?) from the inside without the boundary area never shrinking?


This might help https://physics.stackexchange.com/questions/169886/black-hol...

A black hole merger of this size is unlikely to have any significant quantum aspect


If you drain your bathwater while also running the bath you can have a bathtub that's slowly filling up.


Note that by the time black hole evaporation would be significant the CMB will be long gone because of dark energy (universe expanding). All this means that evaporation is delayed till there is nothing else left apart from black holes (because of the faster than light recession of space itself).



Thank you! It drives me crazy that news articles about a paper never link to the actual damn paper.


So black holes can't evaporate? How does Hawking radiation works if the back hole are has to stay the same?


Black holes can't evaporate now because the cosmic background radiation is too hot. The black holes are colder the CMBR, so they absorb heat and grow (albeit very, very slightly).

Eventually the CMBR will cool down and the holes will be able to evaporate, but not for an insanely long time.


I imagine this holds only for black holes that are massive enough to be stable?

All those itsy bitsy ones created by the LHC, they've evaporated, yes?


I believe that LHC has no chance ever to harvest enough energy to create a sensible-sized black hole. It’s still mc-squared (give or take an order of magnitude and my layman mistakes), so 1g BH takes about 1e14 joules or 5 minutes of average EU electricity output. Also, there is no sea nearby to cool it off afterwards. Also, a planck-sized BH weighs 1e-5 g.

A mass similar to Mount Everest[13][note 1] has a Schwarzschild radius much smaller than a nanometre.[note 2] Its average density at that size would be so high that no known mechanism could form such extremely compact objects

It seems that at energies available to us they are basically either virtual or non-existent. This contradicts the common notion that cosmic rays create microbhs occasionally, but I guess we have to wait for a physicist to clarify this.


In theory, it might have made a black hole. It would have lasted a ridiculously small period of time, but be quite recognizable by the energy it gave off. Instead of the usual decay patterns, it would give off a spray just of photons, like a black body at a recognizable (and very high) temperature.

We didn't see that, and in fact theory predicted that it was insanely unlikely that we would. But there's nothing wrong with the possibility of a black hole much, much, much smaller than a gram, with a radius smaller than the Planck length.

If we had seen it, it would have been insanely informative. But it wasn't ever gonna happen.


Do you know what theory that might be?

The difficulty in producing a black hole is getting the energy density high enough. We have no known mechanism to get an energy density that's even close the right order of magnitude.

Maybe you meant that in theory quantum fluctuations might do it? Unfortunately, this is really a non-answer. The probability is so ridiculously low that it's not practicably distinguishable from zero. (It's _vastly_ more likely that every measurement ever taken and that _will_ be ever taken is wrong, than that the event actually happened).


I have to use "theory" loosely here, because there isn't any known or suspected way to do it. The energy, as you observer, is off by orders of magnitude.

It's just that it's "merely" orders of magnitude. The odds were ludicrously low, but with a whole lot of particles being collided. So maybe, ridiculous outside chance, they might see one event out of the 10^20 events to be observed.

But almost certainly not. So it was never worth talking about. But people loved to talk about black holes, so the math got done.


Correct. It's not so much that the small ones are unstable, but just that there's a continuous curve of lifetimes that's a function of mass.

For the LHC, the lifetime of a black hole it could conceivably create would be 10^-86 seconds. It didn't even do that, but if it had, it would have evaporated before it moved the diameter of an electron. There's no functional difference between that black hole and a vastly bigger one besides the mass... but it's a difference of many, many, many orders of magnitude.


I'm not trying to nitpick, just trying to get my head around your original claim, which I'm tempted to amend:

> Black holes [above a certain mass] can't evaporate now because the cosmic background radiation is too hot

And that mass--the Stable-Black-Hole-In-A-Vacuum mass--it's decreasing. And whatever it is at a given time, more massive holes grow, and less massive holes shrink. Do I have that right?

----

I'm trying to extrapolate backwards to a time when the universe was hotter and the SBHIAV mass was smaller. It seems like there ought to have been a point when the universe was so hot that holes expanded greedily, perhaps to the point where the expanding universe couldn't escape. Golly I wish they taught cosmology at my local university...


I think it's more a case of the press release people wanting to call it a unqualified "law", as far as we know black holes do evaporate slowly.

But there remains is a statement about how the final area relates to the area of the two merging black holes.


They _do_ evaporate, but they also absorb CMB, and right now CMB > evaporation. Later, when CMB fully dissipated they can evaporate in practice.


> Later, when CMB fully dissipated

That's one of the most understated uses of "later" I've heard.


Hehe, true.


According to https://en.wikipedia.org/wiki/Timeline_of_the_far_future, that may be around 150 billion years from now.

Also, I have a hard time reading that page without a sense of existential dread.


> There are certain rules that even the most extreme objects in the universe must obey.

A strange way to put it. The more object is extreme the harder it would be for it to disobey laws. If we try to imagine what forces are involved, all we'll find is that our imagination has it's limits. I'd be less surprised if some quark disobeyed laws, because it small, forces are minuscule and... who is to notice? Maybe they disobey laws all the time, just scientists fail to catch them red handed.


I don’t think the quote is saying objects have to obey laws because they are extreme (and therefore easy to notice) I think it’s saying all objects have to follow the established rules of physics, regardless of how unusual they are. It’s an interesting idea though! Known, “extreme” objects may be less fruitful places to study unknown forces because they have qualities that overwhelming drown out smaller less known forces.


If you have BH evaporation you cannot keep the horizon surface constant.


so they're 95% sure.. how do they even come up with a figure like that? they didn't bother saying. might be equivalent to 'give or take a few trillion tonnes'


https://www.zmescience.com/science/what-5-sigma-means-042342... 95% means 2-sigma, when it comes things like the Higgs boson, they announced the results with 5-sigma certainty, which is a very good indication of statistical significance and confidence.


It’s more that p-value is a bad indication of anything (since it’s vulnerable to p-hacking and all kinds of other issues), so physics just picks a really extreme publication threshold to avoid getting inundated with spurious developments.


It will say in the paper how they went about the error analysis.

These estimates are however, subjective. There is a good paper on this called "Bayesian methods in particle physics" (something like that).


Anyone can think of any practical effect this might have or is this something that at the moment seems to have only scientific relevance.


Well, if the result had turned out the other way, we might have seen some practical effects, because it would overturn some well-established theories that we also use for predicting more practical things.


I’m waiting for a Greg Egan short story to explain this better.


Looks like he already has one on BH boundaries: https://www.gregegan.net/PLANCK/Planck.html




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