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Testing supersymmetry in weak decays by means of time reversal invariance
The minimal supersymmetric extension of the standard model allows for some of the coupling strengths to be complex parameters. The presence of such imaginary phases can lead to violations of time reversal invariance, which can be tested if correlations in products of an odd number of polarizations a...
Autores principales: | , |
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Lenguaje: | eng |
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1993
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/0370-2693(93)90166-F http://cds.cern.ch/record/242705 |
_version_ | 1780885065607151616 |
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author | Christova, Ekaterina Fabbrichesi, Marco |
author_facet | Christova, Ekaterina Fabbrichesi, Marco |
author_sort | Christova, Ekaterina |
collection | CERN |
description | The minimal supersymmetric extension of the standard model allows for some of the coupling strengths to be complex parameters. The presence of such imaginary phases can lead to violations of time reversal invariance, which can be tested if correlations in products of an odd number of polarizations and momenta are measured and found to be different from zero. As an example, we consider the triple product $\mbox{\bf J} \cdot \left(\mbox{\bf p}_1 \times \mbox{\bf p}_ {2} \right)$ in the $\beta$-decay of the neutron, of the $\Sigma^-$, and in the decay $K^{+}_{3\mu}$. For these low-energy decays, we find that the present experimental precision is not enough to provide useful bounds on combinations of such phases and the masses of the supersymmetric particles. At higher energies, the same time reversal violating correlation in the semileptonic decay of the $t$ quark is of the order of $\alpha_s/\pi$, made bigger by the large mass of the decaying quark. |
id | cern-242705 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1993 |
record_format | invenio |
spelling | cern-2427052023-03-14T19:56:15Zdoi:10.1016/0370-2693(93)90166-Fhttp://cds.cern.ch/record/242705engChristova, EkaterinaFabbrichesi, MarcoTesting supersymmetry in weak decays by means of time reversal invarianceParticle Physics - PhenomenologyThe minimal supersymmetric extension of the standard model allows for some of the coupling strengths to be complex parameters. The presence of such imaginary phases can lead to violations of time reversal invariance, which can be tested if correlations in products of an odd number of polarizations and momenta are measured and found to be different from zero. As an example, we consider the triple product $\mbox{\bf J} \cdot \left(\mbox{\bf p}_1 \times \mbox{\bf p}_ {2} \right)$ in the $\beta$-decay of the neutron, of the $\Sigma^-$, and in the decay $K^{+}_{3\mu}$. For these low-energy decays, we find that the present experimental precision is not enough to provide useful bounds on combinations of such phases and the masses of the supersymmetric particles. At higher energies, the same time reversal violating correlation in the semileptonic decay of the $t$ quark is of the order of $\alpha_s/\pi$, made bigger by the large mass of the decaying quark.The minimal supersymmetric extension of the standard model allows for some of the coupling strengths to be complex parameters. The presence of such imaginary phases can lead to violations of time reversal invariance, which can be tested if correlations in products of an odd number of polarizations and momenta are measured and found to be different from zero. As an example, we consider the triple product $\mbox{\bf J}_n \cdot \left( \mbox{\bf p}_e \times \mbox{\bf p}_{\nu_e} \right)$ in the $\beta$-decay of the neutron and nuclei. An improvement of two orders of magnitude in the present experimental precision would provide useful bounds on combinations of such phases and the masses of the supersymmetric particles. Another low-energy process available is the decay $K~{+}_{3\mu}$. At higher energies, the same time reversal violating correlation in the semileptonic decay of the $t$ quark is made $10~4$ times bigger than in the $\beta$-decay, by the large mass of the decaying quark.The minimal supersymmetric extension of the standard model allows for some of the coupling strengths to be complex parameters. The presence of such imaginary phases can lead to violations of time reversal invariance, which can be tested if correlations in products of an odd number of polarizations and momenta are measured and found to be different from zero. As an example, we consider the triple product $\mbox{\bf J}_n \cdot \left( \mbox{\bf p}_e \times \mbox{\bf p}_{\nu_e} \right)$ in the $\beta$-decay of the neutron and nuclei. An improvement of two orders of magnitude in the present experimental precision would provide useful bounds on combinations of such phases and the masses of the supersymmetric particles. Another low-energy process available is the decay $K~{+}_{3\mu}$. At higher energies, the same time reversal violating correlation in the semileptonic decay of the $t$ quark is made $10~4$ times bigger than in the $\beta$-decay, by the large mass of the decaying quark.The minimal supersymmetric extension of the standard model allows for some of the coupling strengths to be complex parameters. The presence of such imaginary phases can lead to violations of time reversal invariance, which can be tested if correlations in products of an odd number of polarizations and momenta are measured and found to be different from zero. As an example, we consider the triple product J · ( p 1 × p 2 ) in the β -decay of the neutron, of the Σ − , and in the decay K + 3 μ . For these low-energy decays, we find that the present experimental precision is not enough to provide useful bounds on combinations of such phases and the masses of the supersymmetric particles. At higher energies, the same time reversal violating correlation in the semileptonic decay of the t quark is of the order of α S / π , made bigger by the large mass of the decaying quark.hep-ph/9302303CERN-TH-6688-92CERN-TH-6688-92oai:cds.cern.ch:2427051993 |
spellingShingle | Particle Physics - Phenomenology Christova, Ekaterina Fabbrichesi, Marco Testing supersymmetry in weak decays by means of time reversal invariance |
title | Testing supersymmetry in weak decays by means of time reversal invariance |
title_full | Testing supersymmetry in weak decays by means of time reversal invariance |
title_fullStr | Testing supersymmetry in weak decays by means of time reversal invariance |
title_full_unstemmed | Testing supersymmetry in weak decays by means of time reversal invariance |
title_short | Testing supersymmetry in weak decays by means of time reversal invariance |
title_sort | testing supersymmetry in weak decays by means of time reversal invariance |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1016/0370-2693(93)90166-F http://cds.cern.ch/record/242705 |
work_keys_str_mv | AT christovaekaterina testingsupersymmetryinweakdecaysbymeansoftimereversalinvariance AT fabbrichesimarco testingsupersymmetryinweakdecaysbymeansoftimereversalinvariance |