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Black Holes and the Strong CP Problem
General Relativity and Quantum Cosmology · Submitted 6 May 2010
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We show that this problem disappears if one assumes the existence of at least one black hole somewhere in the universe.
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The abstract, sentence by sentence
The strong CP problem is that SU(3) gauge field instantons naturally induce a CP violating term in the QCD Lagrangian which is constrained by experiment to be very small for no obvious reason. We show that this problem disappears if one assumes the existence of at least one black hole somewhere in the universe. The argument is reminiscent of Dirac's argument for the quantization of charge, in which the existence of one monople anywhere in the universe suffices to require the quantization of electric charge everywhere.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The strong CP problem is that SU(3) gauge field instantons naturally induce a CP violating term in the QCD Lagrangian which is constrained by experiment to be very small for no obvious reason. | background 1.00 | 0.04 | 0.03 | asserted 1.00 |
| s1 | We show that this problem disappears if one assumes the existence of at least one black hole somewhere in the universe. | result 0.89 | 0.87 | 0.94 | asserted 1.00 |
| s2 | The argument is reminiscent of Dirac's argument for the quantization of charge, in which the existence of one monople anywhere in the universe suffices to require the quantization of electric charge everywhere. | interpretation 0.91 | 0.11 | 0.05 | asserted 0.88 |
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The paper
Original abstract
The strong CP problem is that SU(3) gauge field instantons naturally induce a CP violating term in the QCD Lagrangian which is constrained by experiment to be very small for no obvious reason. We show that this problem disappears if one assumes the existence of at least one black hole somewhere in the universe. The argument is reminiscent of Dirac's argument for the quantization of charge, in which the existence of one monople anywhere in the universe suffices to require the quantization of electric charge everywhere.
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How the literature uses it
3 arXiv papers cite this in 3 sentences
Papers citing it · 2 sentences without a confident label
Cites it as background 1 paper
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The strong CP problem has inspired theories of axions [ref] , and a variety of other possible solutions [ref] [See Refs. Diaz-Cruz:2016pmm,Swain:2010rr for brief lists of possible solutions to the strong CP problem.].
Bayesian naturalness, simplicity, and testability applied to the $B-L$ MSSM GUT · Introduction · 0.93
What it cites
Cites as background 1 paper
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In quantum chromodynamics (QCD) [ref] - the generally accepted theory of quarks and gluons - there was a prediction that there should be a light pseudoscalar particle associated with the conserved current associated with global chiral rotations of the quarks.
The Strong CP Problem and Axions · Introduction · 1.00
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