PeterDonis said:
Sure it is; they reference singularity-free BH models and various papers that discuss them. Those models all have dark energy inside--that's the only way to get a singularity free model. But, as I have already pointed out, ordinary matter, which is what collapses to form BHs in the first place is not dark energy, so the dark energy has to form by some sort of phase transition during the collapse process. Various papers discussing the singularity free models differ in how much they discuss this fact, but that doesn't make it any less a fact.
I see your point, black holes with vacuum energy interiors are an attractive way to get k=3, and that does seem to be what they have in mind. Since they don't form from vacuum energy, some kind of transition is required in there. So the issue of vacuum energy is not actually removed or resolved, merely confined to within black holes. It's a bit like intentionally leaving the keys somewhere out of the streetlight, which would be unattractive except that they feel k=3 has some theoretical attractiveness. Then by removing vacuum energy from the rest of the universe, they are saying it would have to be something that is only possible due to the kind of phase change you are talking about.
PeterDonis said:
That's the observational claim that is used to focus on a particular class of BH models, yes. But the overall claim of the paper depends on those models, not just on the observations.
The claims are certainly inspired by those models, though the actual results of the paper do not need to even mention models. They claim to have a result that gets k=3 without knowing any GR at all, though we all agree the observations require corroboration because others have looked at this kind of data without it jumping out at them that black holes have gained an order of magnitude in mass in galaxies experiencing little accretion.
PeterDonis said:
I'm not sure the authors of the paper would agree with this.
I got it straight from the paper:
"As described in Section
1, there are known exact solutions with each of the following properties: strong spin, arbitrary RW asymptotics, dynamical mass, and interior vacuum energy equation of state. Our result implies the existence, within GR, of an exact solution with all of these properties. Currently, there is no known solution that possesses all four, though there are known solutions with various combinations of two (e.g., Guariento et al.
2012; Dymnikova & Galaktionov
2016). Finding solutions that feature all four properties is an important theoretical step forward."
So their perspective is they have an observational result that is intended to stimulate a GR solution that does not yet exist.
PeterDonis said:
This particular paper does not go into such things itself; it references other papers that do. See above. The paper does take it as given that BH models with dark energy inside are required; for example, on p. 3 it says "Vacuum energy interior solutions with cosmological boundaries have been predicted to produce" the coupling value that the paper claims to see in the observational data.
Yes, you are right that they very much are picturing black holes with vacuum energy interiors, as part of the interpretation of their observational results that do not, by themselves, require that to be the case. So although it might turn out that black holes have k=3 for other reasons than internal dark energy, that is not what is currently expected, and you are justified in focusing on that situation.
PeterDonis said:
No, that alone is not sufficient to "act like dark energy". You also need a dark energy equation of state. That involves the pressure, not just the mass density.
The way this has always been explained to me is that a general way to think about pressure is the negative of the energy change per volume change. Hence anything that attributes energy in proportion to volume is going to have negative pressure, and produce the gravitational consequences of that. If the vacuum everywhere in the universe has a constant energy density, then energy is proportional to volume, but you get the same effect if you have a discrete set of black holes that are increasing in energy (increasing their mass-energy) proportional to the volume increase, it works the same way to produce a negative gravitational pressure. So you get the necessary equation of state automatically. Perhaps I am wrong that just increasing the mass would do that, but it only seems to require associating energy with the black hole mass.
PeterDonis said:
That's because they accept that observations show that the expansion is accelerated. They are taking that as a given, and adding to it their observational claim about masses of BHs coupling to the expansion, in order to account for the accelerated expansion.
Yes, I agree.
PeterDonis said:
I mean a black hole solution in which ordinary matter collapses, and because it's ordinary matter and no phase transition occurs, the singularity theorems guarantee that there will be a singularity inside.
Right, that is the part I did not understand until now, thank you.
PeterDonis said:
Note that this does not require the solution to be asymptotically flat; there is a singularity in the Schwarzschild-de Sitter solution, for example, which is a Schwarzschild BH with a de Sitter boundary, not an asymptotically flat boundary. (I'm not sure the authors of the paper fully realize this.)
It might be the issue of spin. They realize that kind of thing is possible, but they expect black holes to spin, so they think something is missing.
PeterDonis said:
What does "pure GR" mean? Dark energy is perfectly within the scope of GR.
Yes, they still need dark energy, they just need it inside the black hole, which they are hoping will turn out to be something that emerges naturally from the necessary black hole solution. But it could be argued that without black holes, we already had dark energy emerging as a solution to the accelerated expansion, so I was wrong they they are trying to circumvent that completely. Instead, they think it is a step forward to just quarantine it to within black holes. It's not so obvious that really is much of a step forward, but they can always argue that we have no choice, if k really turns out to be 3.
PeterDonis said:
The authors of the paper might believe this, but they are wrong. The Schwarzschild-de Sitter solution is such a solution. See above. There is also a Kerr-de Sitter solution if one wants a more realistic hole with spin.
That last point seems to be the key issue, they don't think it has been done with strong spin in a way that has the black hole mass increase with k=3. So they are saying, they think their observations require k=3 (many are not yet convinced), so any solution that doesn't have that property will be found wanting, and other solutions must still be sought.