# Black hole electron

In physics, there is a speculative notion that if there were a black hole with the same mass, charge and angular momentum as an electron, it would share some of the properties of the electron. Most notably, Brandon Carter showed in 1968 that the magnetic moment of such an object would match that of an electron.^{[1]} This is interesting because calculations ignoring special relativity and treating the electron as a small rotating sphere of charge give a magnetic moment that is off by roughly a factor of 2, the so-called gyromagnetic ratio.

However, Carter's calculations also show that a would-be black hole with these parameters would be 'super-extremal'. Thus, unlike a true black hole, this object would display a naked singularity, meaning a singularity in spacetime not hidden behind an event horizon. It would also give rise to closed timelike curves.

Standard quantum electrodynamics (QED) treats the electron as a point particle, a view completely supported by experiment.^{[citation needed]} There is no evidence that the electron is a black hole (or naked singularity). Furthermore, since the electron is quantum mechanical in nature,^{[citation needed]} any description purely in terms of general relativity is inadequate.

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## DetailsEdit

A paper published in 1938 by Albert Einstein, Leopold Infeld and Banesh Hoffmann showed that if elementary particles are treated as singularities in spacetime, it is unnecessary to postulate geodesic motion as part of general relativity.^{[2]} The electron may be treated as such a singularity.

If one ignores the electron's angular momentum and charge, as well as the effects of quantum mechanics, one can treat the electron as a black hole and attempt to compute its radius. The Schwarzschild radius r_{s} of a mass m is the radius of the event horizon for a non-rotating, uncharged black hole of that mass. It is given by

- ,

where G is Newton's gravitational constant and c is the speed of light. For the electron,

- m = ×10
^{−31}kg, 9.109

so

- r
_{s}= ×10^{−57}m. 1.353

Thus, if we ignore the electric charge and angular momentum of the electron, and naively apply general relativity on this very small length scale without taking quantum theory into account, a black hole of the electron's mass would have this radius.

In reality, physicists expect quantum gravity effects to become significant even at much larger length scales, comparable to the Planck length

- m

So, the above purely classical calculation cannot be trusted. Furthermore, even classically, electric charge and angular momentum affect the properties of a black hole. To take them into account, while still ignoring quantum effects, one should use the Kerr–Newman metric. If we do, we find the angular momentum and charge of the electron are too large for a black hole of the electron's mass: a Kerr-Newman object with such a large angular momentum and charge would instead be 'super-extremal', displaying a naked singularity, meaning a singularity not shielded by an event horizon.

To see that this is so, it suffices to consider the electron's charge and neglect its angular momentum. In the Reissner–Nordström metric, which describes electrically charged but non-rotating black holes, there is a quantity r_{q}, defined by

where q is the electron's charge and *ε*_{0} is the vacuum permittivity. For an electron with q = −e = ×10^{−19} C, this gives a value
−1.602

- r
_{q}= ×10^{−36}m. 1.3807

Since this (vastly) exceeds the Schwarzschild radius, the Reissner–Nordström metric has a naked singularity.

If we include the effects of the electron's rotation using the Kerr-Newman metric, there is still a naked singularity, which is now a ring singularity, and spacetime also has closed timelike curves. The size of this ring singularity is on the order of

- ,

where as before m is the electron's mass and c is the speed of light, but J = is the spin angular momentum of the electron. This gives

- r
_{a}= ×10^{−13}m 1.9295

which is much larger than the length scale r_{q} associated to the electron's charge. As noted by Carter,^{[3]} this length r_{a} is on the order of the electron's Compton wavelength. Unlike the Compton wavelength, it is not quantum-mechanical in nature.

More recently, Alexander Burinskii has pursued the idea of treating the electron as a Kerr–Newman naked singularity.^{[4]}^{[5]}. Interesting quantum implications of this idea, combined with EPR like thought experiments, suggest additional black hole electron models.^{[6]}

## See alsoEdit

## ReferencesEdit

**^**Carter, B. (25 October 1968). "Global structure of the Kerr family of gravitational fields".*Physical Review*.**174**(5): 1559–1571. Bibcode:1968PhRv..174.1559C. doi:10.1103/physrev.174.1559.**^**Einstein, A.; Infeld, L.; Hoffmann, B. (January 1938). "The gravitational equations and the problem of motion".*Annals of Mathematics*. Second Series.**39**(1): 65–100. doi:10.2307/1968714. JSTOR 1968714.**^**Carter, B. (25 October 1968). "Global structure of the Kerr family of gravitational fields".*Physical Review*.**174**(5): 1559–1571. Bibcode:1968PhRv..174.1559C. doi:10.1103/physrev.174.1559.**^**Burinskii, Alexander (April 2008). "The Dirac-Kerr-Newman electron".*Gravitation and Cosmology*.**14**(2): 109–122. arXiv:hep-th/0507109. Bibcode:2008GrCo...14..109B. doi:10.1134/S0202289308020011.**^**Burinskii, Alexander (2007). "Kerr geometry as space–time structure of the Dirac electron". arXiv:0712.0577.**^**Nemirovsky, J.; Cohen, E.; Kaminer, I. (30 Dec 2018). "Spin Spacetime Censorship". arXiv:1812.11450v1 [gr-qc].

## Further readingEdit

- Duff, Michael (1994). "Kaluza–Klein theory in perspective". arXiv:hep-th/9410046.
- Hawking, Stephen (1971). "Gravitationally collapsed objects of very low mass".
*Monthly Notices of the Royal Astronomical Society*.**152**: 75. Bibcode:1971MNRAS.152...75H. doi:10.1093/mnras/152.1.75. - Penrose, Roger (2004).
*The Road to Reality: A Complete Guide to the Laws of the Universe*. London: Jonathan Cape. - Salam, Abdus. "Impact of quantum gravity theory on particle physics". In Isham, C. J.; Penrose, Roger; Sciama, Dennis William.
*Quantum Gravity: an Oxford Symposium*. Oxford University Press. - 't Hooft, Gerard (1990). "The black hole interpretation of string theory".
*Nuclear Physics B*.**335**: 138–154. Bibcode:1990NuPhB.335..138T. doi:10.1016/0550-3213(90)90174-C.

### Popular literatureEdit

- Brian Greene,
*The Elegant Universe: Superstrings, Hidden Dimensions, and the Quest for the Ultimate Theory*(1999),*(See chapter 13)* - John A. Wheeler,
*Geons, Black Holes & Quantum Foam*(1998),*(See chapter 10)*