The nucleus as a source in Kerr-Newman geometry

Details The nucleus as a source in Kerr-Newman geometry The nucleus as a source in Kerr-Newman geometry

Jan 1987

adsabs.harvard.edu/cgi-bin/nph-data_query?bibcode=1987phrva..35...14p&link_type=abstract

Physical Review A (General Physics), Volume 35, Issue 1, January 1, 1987, pp.14-17

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Other Topics In General Relativity And Gravitation, Hyperfine Interactions And Isotope Effects, Jahn-Teller Effect, Theory Of Electronic Structure, Electronic Transitions, And Chemical Binding

Scientific paper

The nucleus is treated as a source in Kerr-Newman geometry, under the assumption that the angular momentum of the source is equal to the intrinsic spin angular momentum of the nucleus. The spin radius a of the nucleus, which figures in the Kerr-Newman metric, is of the order of the Compton wavelength of the nucleus. The radial functions in Chandrasekhar's separated Dirac equation in Kerr geometry, are transformed so as to yield a pair of simultaneous first-order differential equations with real coefficients, as in flat space. The magnetic quantum number m appears explicitly in the differential equations, thus lifting the hyperfine splitting degeneracy of Dirac's equation in flat space.

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