Electromagnetic dipole moments and time reversal violating interactions for high energy charged baryons in bent crystals at LHC

Abstract Spin precession of channelled particles in bent crystals at the LHC gives unique possibility for measurements of constants determining T-odd, P-odd (CP) violating interactions and P-odd, T-even interactions of charm, beauty and strange charged baryons with electrons and nucleus (nucleons),...

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Main Author: V. G. Baryshevsky
Format: Article
Language:English
Published: SpringerOpen 2019-04-01
Series:European Physical Journal C: Particles and Fields
Online Access:http://link.springer.com/article/10.1140/epjc/s10052-019-6857-6
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spelling doaj-df96b14cadb2473f9b37a726159b81772020-11-25T02:01:04ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522019-04-0179411510.1140/epjc/s10052-019-6857-6Electromagnetic dipole moments and time reversal violating interactions for high energy charged baryons in bent crystals at LHCV. G. Baryshevsky0Research Institute for Nuclear Problems, Belarusian State UniversityAbstract Spin precession of channelled particles in bent crystals at the LHC gives unique possibility for measurements of constants determining T-odd, P-odd (CP) violating interactions and P-odd, T-even interactions of charm, beauty and strange charged baryons with electrons and nucleus (nucleons), similarly to the possibility of measuring their electric and magnetic moments. For a particle moving in a bent crystal new effects caused by non-elastic processes arise. In addition to the spin rotation around the effective magnetic field $$ {\varvec{B}} $$ B direction (the bending axis direction), due to electromagnetic interactions and leading to changes in spin direction in the plane orthogonal to $$ {\varvec{B}} $$ B , the spin acquires projection along the $$ {\varvec{B}} $$ B direction. Moreover, when spin rotates around the direction of the electric field $${\varvec{E}}$$ E or the particle momentum $${\varvec{k}}$$ k , a spin component along $${\varvec{E}}$$ E or $${\varvec{k}}$$ k , respectively, is induced.http://link.springer.com/article/10.1140/epjc/s10052-019-6857-6
collection DOAJ
language English
format Article
sources DOAJ
author V. G. Baryshevsky
spellingShingle V. G. Baryshevsky
Electromagnetic dipole moments and time reversal violating interactions for high energy charged baryons in bent crystals at LHC
European Physical Journal C: Particles and Fields
author_facet V. G. Baryshevsky
author_sort V. G. Baryshevsky
title Electromagnetic dipole moments and time reversal violating interactions for high energy charged baryons in bent crystals at LHC
title_short Electromagnetic dipole moments and time reversal violating interactions for high energy charged baryons in bent crystals at LHC
title_full Electromagnetic dipole moments and time reversal violating interactions for high energy charged baryons in bent crystals at LHC
title_fullStr Electromagnetic dipole moments and time reversal violating interactions for high energy charged baryons in bent crystals at LHC
title_full_unstemmed Electromagnetic dipole moments and time reversal violating interactions for high energy charged baryons in bent crystals at LHC
title_sort electromagnetic dipole moments and time reversal violating interactions for high energy charged baryons in bent crystals at lhc
publisher SpringerOpen
series European Physical Journal C: Particles and Fields
issn 1434-6044
1434-6052
publishDate 2019-04-01
description Abstract Spin precession of channelled particles in bent crystals at the LHC gives unique possibility for measurements of constants determining T-odd, P-odd (CP) violating interactions and P-odd, T-even interactions of charm, beauty and strange charged baryons with electrons and nucleus (nucleons), similarly to the possibility of measuring their electric and magnetic moments. For a particle moving in a bent crystal new effects caused by non-elastic processes arise. In addition to the spin rotation around the effective magnetic field $$ {\varvec{B}} $$ B direction (the bending axis direction), due to electromagnetic interactions and leading to changes in spin direction in the plane orthogonal to $$ {\varvec{B}} $$ B , the spin acquires projection along the $$ {\varvec{B}} $$ B direction. Moreover, when spin rotates around the direction of the electric field $${\varvec{E}}$$ E or the particle momentum $${\varvec{k}}$$ k , a spin component along $${\varvec{E}}$$ E or $${\varvec{k}}$$ k , respectively, is induced.
url http://link.springer.com/article/10.1140/epjc/s10052-019-6857-6
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