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Nonexistence of time-periodic solutions of the Dirac equation in an axisymmetric black hole geometry

โœ Scribed by Felix Finster; Niky Kamran; Joel Smoller; Shing-Tung Yau


Publisher
John Wiley and Sons
Year
2000
Tongue
English
Weight
174 KB
Volume
53
Category
Article
ISSN
0010-3640

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โœฆ Synopsis


We prove that in the nonextreme Kerr-Newman black hole geometry, the Dirac equation has no normalizable, time-periodic solutions. A key tool is Chandrasekhar's separation of the Dirac equation in this geometry. A similar nonexistence theorem is established in a more general class of stationary, axisymmetric metrics in which the Dirac equation is known to be separable. These results indicate that, in contrast to the classical situation of massive particle orbits, a quantum mechanical Dirac particle must either disappear into the black hole or escape to infinity.


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Erratum: Nonexistence of time-periodic s
โœ Felix Finster; Niky Kamran; Joel Smoller; Shing-Tung Yau ๐Ÿ“‚ Article ๐Ÿ“… 2000 ๐Ÿ› John Wiley and Sons ๐ŸŒ English โš– 9 KB ๐Ÿ‘ 2 views

The angular eigenvalue in equation (2.16) should not be an integer but a half odd integer. The reason is that the transformation V from the Dirac operator in the symmetric frame to the usual Dirac operator in polar coordinates given at the end of Section 2.1 has a change of sign at ฯ• = 0. Likewise,