The g factor of the bound muon in medium-Z muonic atoms

We consider a theory of the g factor of a bound muon in a three-body atomic system, which consists of a spinless nucleus, a muon, and an electron in the medium range of Z=10–30. We show that the calculation at the one-ppm level of accuracy can be separated into a consideration of an internal subsyst...

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Main Authors: Savely G. Karshenboim, Vladimir G. Ivanov
Format: Article
Language:English
Published: Elsevier 2018-11-01
Series:Physics Letters B
Online Access:http://www.sciencedirect.com/science/article/pii/S037026931830755X
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spelling doaj-e016076883094d8bac33ef478ca0cb9f2020-11-25T01:16:07ZengElsevierPhysics Letters B0370-26932018-11-01786485490The g factor of the bound muon in medium-Z muonic atomsSavely G. Karshenboim0Vladimir G. Ivanov1Ludwig-Maximilians-Universität, Fakultät für Physik, 80799 München, Germany; Max-Planck-Institut für Quantenoptik, Garching, 85748, Germany; Pulkovo Observatory, St. Petersburg, 196140, Russia; Corresponding author.Pulkovo Observatory, St. Petersburg, 196140, RussiaWe consider a theory of the g factor of a bound muon in a three-body atomic system, which consists of a spinless nucleus, a muon, and an electron in the medium range of Z=10–30. We show that the calculation at the one-ppm level of accuracy can be separated into a consideration of an internal subsystem μ−N (with a muon at the ground state) and an external subsystem with an electron and a compound μ−N nucleus.We discuss the most important contributions to the g factor of the bound muon in the μ−N system in the medium-Z approximation. In this range the list of relevant contributions contains kinematic pure Coulomb contributions, the finite-nuclear-size ones, and muonic-atom-specific contributions with closed electron loops. In the case of the medium Z one can apply a double limit Zα≪1 and Zαmμ/me≫1, at which a number of specific contributions is simplified. Special attention is paid to non-potential contributions, i.e., those which cannot be expressed in terms of an effective potential.We also consider the electron shielding of the magnetic moment of the compound nucleus, focusing on the corrections which are enhanced or suppressed comparing to the shielding of ordinary nuclei. In conclusion we discuss a generalization of our result for muonic atoms with a few electrons.http://www.sciencedirect.com/science/article/pii/S037026931830755X
collection DOAJ
language English
format Article
sources DOAJ
author Savely G. Karshenboim
Vladimir G. Ivanov
spellingShingle Savely G. Karshenboim
Vladimir G. Ivanov
The g factor of the bound muon in medium-Z muonic atoms
Physics Letters B
author_facet Savely G. Karshenboim
Vladimir G. Ivanov
author_sort Savely G. Karshenboim
title The g factor of the bound muon in medium-Z muonic atoms
title_short The g factor of the bound muon in medium-Z muonic atoms
title_full The g factor of the bound muon in medium-Z muonic atoms
title_fullStr The g factor of the bound muon in medium-Z muonic atoms
title_full_unstemmed The g factor of the bound muon in medium-Z muonic atoms
title_sort g factor of the bound muon in medium-z muonic atoms
publisher Elsevier
series Physics Letters B
issn 0370-2693
publishDate 2018-11-01
description We consider a theory of the g factor of a bound muon in a three-body atomic system, which consists of a spinless nucleus, a muon, and an electron in the medium range of Z=10–30. We show that the calculation at the one-ppm level of accuracy can be separated into a consideration of an internal subsystem μ−N (with a muon at the ground state) and an external subsystem with an electron and a compound μ−N nucleus.We discuss the most important contributions to the g factor of the bound muon in the μ−N system in the medium-Z approximation. In this range the list of relevant contributions contains kinematic pure Coulomb contributions, the finite-nuclear-size ones, and muonic-atom-specific contributions with closed electron loops. In the case of the medium Z one can apply a double limit Zα≪1 and Zαmμ/me≫1, at which a number of specific contributions is simplified. Special attention is paid to non-potential contributions, i.e., those which cannot be expressed in terms of an effective potential.We also consider the electron shielding of the magnetic moment of the compound nucleus, focusing on the corrections which are enhanced or suppressed comparing to the shielding of ordinary nuclei. In conclusion we discuss a generalization of our result for muonic atoms with a few electrons.
url http://www.sciencedirect.com/science/article/pii/S037026931830755X
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