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A realistic formulation of approximate CP
CP violation in the SM is naturally implemented as a small imaginary perturbation to real Yukawa couplings. For example, a large CP asymmetry in B_d decays can arise if the imaginary parts of quark mass matrices are of order 10^(-3)m_t,b or smaller. Applying the same principle of ``additive CP viola...
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Lenguaje: | eng |
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2002
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Acceso en línea: | https://dx.doi.org/10.1016/S0550-3213(03)00005-1 http://cds.cern.ch/record/558682 |
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author | Dent, Thomas Silva-Marcos, Joaquim |
author_facet | Dent, Thomas Silva-Marcos, Joaquim |
author_sort | Dent, Thomas |
collection | CERN |
description | CP violation in the SM is naturally implemented as a small imaginary perturbation to real Yukawa couplings. For example, a large CP asymmetry in B_d decays can arise if the imaginary parts of quark mass matrices are of order 10^(-3)m_t,b or smaller. Applying the same principle of ``additive CP violation'' to soft SUSY-breaking terms, the electric dipole moments of the neutron and mercury atom are predicted near current experimental limits; for nonuniversal A-terms, EDM bounds can be satisfied given certain flavour structures. The proposal is conveniently formulated in a democratic basis, with Yukawas and soft terms of the form const x (1+eps+i zeta) where eps<<1, zeta<~10^(-3), motivated by approximate permutation x CP symmetry. |
id | cern-558682 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2002 |
record_format | invenio |
spelling | cern-5586822019-09-30T06:29:59Zdoi:10.1016/S0550-3213(03)00005-1http://cds.cern.ch/record/558682engDent, ThomasSilva-Marcos, JoaquimA realistic formulation of approximate CPParticle Physics - PhenomenologyCP violation in the SM is naturally implemented as a small imaginary perturbation to real Yukawa couplings. For example, a large CP asymmetry in B_d decays can arise if the imaginary parts of quark mass matrices are of order 10^(-3)m_t,b or smaller. Applying the same principle of ``additive CP violation'' to soft SUSY-breaking terms, the electric dipole moments of the neutron and mercury atom are predicted near current experimental limits; for nonuniversal A-terms, EDM bounds can be satisfied given certain flavour structures. The proposal is conveniently formulated in a democratic basis, with Yukawas and soft terms of the form const x (1+eps+i zeta) where eps<<1, zeta<~10^(-3), motivated by approximate permutation x CP symmetry.CP violation in the SM is naturally implemented as a small imaginary perturbation to real Yukawa couplings. For example, a large CP asymmetry in B_d decays can arise if the imaginary parts of quark mass matrices are of order 10^(-3)m_t,b or smaller. Applying the same principle of ``additive CP violation'' to soft SUSY-breaking terms, the electric dipole moments of the neutron and mercury atom are predicted near current experimental limits: for nonuniversal A-terms, EDM bounds can be satisfied given certain flavour structures. The proposal is conveniently formulated in a democratic basis, with Yukawas and soft terms of the form const. x (1+eps+i zeta) where eps<<1, zeta<~10^(-3), motivated by approximate permutation x CP symmetry.CP violation in the SM is naturally implemented as a small imaginary perturbation to real Yukawa couplings. For example, a large CP asymmetry in B_d decays can arise if the imaginary parts of quark mass matrices are of order 10^(-3)m_t,b or smaller. Applying the same principle of ``additive CP violation'' to soft SUSY-breaking terms, the electric dipole moments of the neutron and mercury atom are predicted near current experimental limits: for nonuniversal A-terms, EDM bounds can be satisfied given certain flavour structures. The proposal is conveniently formulated in a democratic basis, with Yukawas and soft terms of the form const. x (1+eps+i zeta) where eps<<1, zeta<~10^(-3), motivated by approximate permutation x CP symmetry.CP violation in the SM is naturally implemented as a small imaginary perturbation to real Yukawa couplings. For example, a large CP asymmetry in B_d decays can arise if the imaginary parts of quark mass matrices are of order 10^(-3)m_t,b or smaller. Applying the same principle of ``additive CP violation'' to soft SUSY-breaking terms, the electric dipole moments of the neutron and mercury atom are predicted near current experimental limits: for nonuniversal A-terms, EDM bounds can be satisfied given certain flavour structures. The proposal is conveniently formulated in a democratic basis, with Yukawas and soft terms of the form const. x (1+eps+i zeta) where eps<<1, zeta<~10^(-3), motivated by approximate permutation x CP symmetry.CP violation in the SM is naturally implemented as a small imaginary perturbation to real Yukawa couplings. For example, a large CP asymmetry in B d decays can arise if the imaginary parts of quark mass matrices are of order 10 −3 m t , b or smaller. Applying the principle of “additive CP violation” to soft SUSY-breaking terms, the electric dipole moments of the neutron and mercury atom are predicted near current experimental limits; for nonuniversal A -terms, EDM bounds can be satisfied given certain flavour structures. The proposal may be formulated in a democratic basis, with Yukawas and soft terms of the form const·(1+ ϵ + iζ ) where | ϵ |⪡1, | ζ |≲10 −3 , motivated by approximate permutation × CP symmetry.hep-ph/0206086MCTP-02-30MCTP-2002-30oai:cds.cern.ch:5586822002-06-09 |
spellingShingle | Particle Physics - Phenomenology Dent, Thomas Silva-Marcos, Joaquim A realistic formulation of approximate CP |
title | A realistic formulation of approximate CP |
title_full | A realistic formulation of approximate CP |
title_fullStr | A realistic formulation of approximate CP |
title_full_unstemmed | A realistic formulation of approximate CP |
title_short | A realistic formulation of approximate CP |
title_sort | realistic formulation of approximate cp |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1016/S0550-3213(03)00005-1 http://cds.cern.ch/record/558682 |
work_keys_str_mv | AT dentthomas arealisticformulationofapproximatecp AT silvamarcosjoaquim arealisticformulationofapproximatecp AT dentthomas realisticformulationofapproximatecp AT silvamarcosjoaquim realisticformulationofapproximatecp |