Could Quantum Physics explain the singularity in a Black Hole?

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Discussion Overview

The discussion revolves around the potential role of quantum physics in explaining singularities within black holes, contrasting it with the explanations provided by general relativity. Participants explore theoretical implications, the nature of singularities, and the need for a theory of quantum gravity.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation

Main Points Raised

  • Some participants suggest that without a theory of quantum gravity, the question of whether quantum physics can explain singularities remains unanswered.
  • One participant argues that singularities are mathematical constructs rather than physical entities, comparing the existence of a singularity to the existence of a number in a physical context.
  • Another viewpoint posits that the goal should be to eliminate singularities through a theory that potentially incorporates quantum gravity, although definitive proof is lacking.
  • Some participants assert that general relativity provides explanations for singularities without the need for quantum theory, unless the aim is to demonstrate their non-existence.
  • A participant speculates on the role of quantum mechanics in addressing singularities, discussing the limitations of point-particle models in classical electromagnetism and suggesting that quantum descriptions may avoid singularities.
  • There is a mention of the need for a relativistic framework when discussing electromagnetic theory and its implications for understanding singularities in the context of quantum field theory.
  • One participant highlights that singularities can exist in vacuum space-times in general relativity, suggesting that they are not solely a consequence of inadequate matter models.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the nature of singularities and the adequacy of quantum physics versus general relativity in explaining them. The discussion remains unresolved, with no consensus reached on the role of quantum physics in this context.

Contextual Notes

Participants note limitations in current theoretical frameworks, including the absence of a comprehensive theory of quantum gravity and the challenges posed by mathematical singularities in both classical and quantum contexts.

zuz
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If a singularity exists in the center of a black hole, could quantum physics, instead of relativity , explain it?
 
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We have no way of answering this question without a theory of quantum gravity, which we do not presently have.
 
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I'll go further than Peter. A singularity is a mathematical concept, not a physical one. The statement "a singularity exists in the center of a black hole is a little like "a 7 exists in the center of a black hole."
 
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zuz said:
If a singularity exists in the center of a black hole, could quantum physics, instead of relativity , explain it?
Singularity does not need an explanation, it needs an ellimination. Namely, we want a theory that gets rid of the singularity. There are many indications, but not yet a definite proof, that quantum gravity can do that.
 
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Singularties are explain in relativity. For an explanation you don't need quantum theory. Unless by an explanation you mean something else, say to show that there are no singularities.
 
Well, I always like to first look at electrodynamics. I speculate here of course a bit, but I think that the point-particle concept is a mathematical simplification which works in some approximations well (motion of a point charge in an external em. field neglecting the radiation reaction; the retarded field solution of a point charge in given motion, again neglecting the back reaction of the own field to the charge's motion), but it's "a stranger" in electromagnetic theory, as Sommerfeld put it.

How can quantum mechanics help here? Take as the most simple case non-relativistic quantum theory and a single-particle as described by wave mechanics a la Schrödinger or more interestingly Pauli to include spin and generic magnetic moments. In QM you then have a field description for the particles, and thanks to the uncertainty relation a particle is not necessarily described by some singularity (a classical point particle is described in classical field theory by a Dirac ##\delta## distribution, which makes it simple in some cases but very uncomfortable in many others, because it's a singularity).

E.g., what's a quantum mechanical description of something like an electrostatic Coulomb field? Of course, a classical particle at rest in the origin of the coordinate system is described by the singular charge density ##\rho(\vec{r})=q \delta^{(3)}(\vec{r})## and the current density ##\vec{j}(\vec{r})=0##. The electromagnetic field is the singular Coulomb field (given in terms of the Lorenz-gauge em. postentials),
$$\Phi(\vec{r})=\frac{q}{4 \pi r}, \quad \vec{A}=0.$$
How about a quantum-theoretical model. Here you get an electrostatic situation if you have a true energy eigenstate, i.e., you have to put the particle in a trap, e.g., some harmonic-oscillator potential, where the ground state is a Gauß wave packet
$$\psi(\vec{x})=N \exp(-\frac{\vec{x}^2}{4 \sigma_x^2}, \quad \sigma_x=\text{const}.$$
Now you can argue semiclassically and calculate the electrostatic field with the corresponding charge-current density
$$\rho(\vec{x})=q |\psi(\vec{x})|^2, \quad \vec{j}(\vec{x})=0.$$
You get a nice and smooth electrostatic potential/field without any singularities. In some sense it's fitting much better the field concept than the classical-point particle model for the charge, which is singular to begin with.

If you want to make everything relativistic, as you should, because electromagnetism is a relativistic thing and gets inconsistent if you don't describe it relativistically. Then you are lead to quantum field theory and here QED. Then even the radiation-reaction problem gets tamed thanks to (perturbative) renormalization theory, which you cannot say about the classical-point particle concept, where the best one can do (and which is obviously sufficient FAPP, as working particle accelerators show) is to use the Landau-Lifshitz approximation of the Lorentz-Abraham-Dirac equation.
 
@vanhees71 I think that there is a difference. In GR you have singularities in vacuum space-times as well. So you cannot say that the singularities come from a bad matter model like the particles in EM.
 
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