2007
DOI: 10.1088/1751-8113/40/22/014
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Dipole transitions and Stark effect in the charge-dyon system

Abstract: We consider the dipole transitions and the linear and quadratic Stark effect in the MICZ-Kepler system interpreting as a charge-dyon system. We show, that while the linear Stark effect in the ground state is proportional to azimuth quantum number(and to the sign of monopole number), the quadratic Stark effect in the ground state is independent on the signs of azimuth and monopole numbers.

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Cited by 5 publications
(7 citation statements)
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References 26 publications
(33 reference statements)
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“…We obtained linear in E and B corrections to the unperturbed spectrum of the ordinary MICZ-Kepler problem. The Stark effect in the charge-dyon system was calculated within the perturbation theory up to second order earlier in series of papers [10,15]. Here we investigated the first order corrections corresponding to magnetic field effect (linear Zeeman effect).…”
Section: Resultsmentioning
confidence: 99%
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“…We obtained linear in E and B corrections to the unperturbed spectrum of the ordinary MICZ-Kepler problem. The Stark effect in the charge-dyon system was calculated within the perturbation theory up to second order earlier in series of papers [10,15]. Here we investigated the first order corrections corresponding to magnetic field effect (linear Zeeman effect).…”
Section: Resultsmentioning
confidence: 99%
“…Putting B = 0 one obtains the well-known result of purely Stark effect in the charge-dyon system [10,15]. The third term in the expression corresponds to the linear Zeeman effect.…”
Section: The Perturbative First Order Corrections and Linear Zeeman Smentioning
confidence: 91%
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“…For example, in the linear potential field eEr there is the linear Stark effect, similar to the hydrogen atom. However, in contrast with the latter one, the linear Stark effect completely removes the degeneracy on the azimuth quantum number [6,7], in contrast with the hydrogen atom. Particularly, the ground state is given by the expression…”
mentioning
confidence: 97%
“…This is consequence of the violation of P -parity by the magnetic monopole, and is the general feature of the quantum mechanical systems with monopoles (see [9,7] and the references in [10]). The specific effect of the choice of the Coulomb potential is hidden symmetry, essentially simplifying the analyses of the system.…”
mentioning
confidence: 99%