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The effect of S-wave interference on the $B^0 \to K^{\ast 0}\ell^+\ell^-$ angular observables
The rare decay $B^0 \to K^{\ast 0}\ell^+\ell^-$ is a flavour changing neutral current decay with a high sensitivity to physics beyond the Standard Model. Nearly all theoretical predictions and all experimental measurements so far have assumed a $K^{\ast 0}$ P-wave that decays into the $K^+\pi^-$ fin...
Autores principales: | , , |
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Lenguaje: | eng |
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2012
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Acceso en línea: | https://dx.doi.org/10.1007/JHEP03(2013)027 http://cds.cern.ch/record/1489372 |
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author | Blake, Thomas Egede, Ulrik Shires, Alex |
author_facet | Blake, Thomas Egede, Ulrik Shires, Alex |
author_sort | Blake, Thomas |
collection | CERN |
description | The rare decay $B^0 \to K^{\ast 0}\ell^+\ell^-$ is a flavour changing neutral current decay with a high sensitivity to physics beyond the Standard Model. Nearly all theoretical predictions and all experimental measurements so far have assumed a $K^{\ast 0}$ P-wave that decays into the $K^+\pi^-$ final state. In this paper the addition of an S-wave within the $K^+\pi^-$ system of $B^0 \to K^{\ast 0}\ell^+\ell^-$ and the subsequent impact of this on the angular distribution of the final state particles is explored. The inclusion of the S-wave causes a distinction between the values of the angular observables obtained from counting experiments and those obtained from fits to the angular distribution. The effect of a non-zero S-wave on an angular analysis of $B^0 \to K^{\ast 0}\ell^+\ell^-$ is assessed as a function of dataset size and the relative size of the S-wave amplitude. An S-wave contribution, equivalent to what is measured in $B^0 \to J/\psi K^{\ast 0}$ at BaBar, leads to a significant bias on the angular observables for datasets of above 200 signal decays. Any future experimental analysis of the $K^+\pi^-\ell^+\ell^-$ final state will have to take the S-wave contribution into account. |
id | cern-1489372 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2012 |
record_format | invenio |
spelling | cern-14893722021-07-16T00:06:40Zdoi:10.1007/JHEP03(2013)027http://cds.cern.ch/record/1489372engBlake, ThomasEgede, UlrikShires, AlexThe effect of S-wave interference on the $B^0 \to K^{\ast 0}\ell^+\ell^-$ angular observablesParticle Physics - PhenomenologyThe rare decay $B^0 \to K^{\ast 0}\ell^+\ell^-$ is a flavour changing neutral current decay with a high sensitivity to physics beyond the Standard Model. Nearly all theoretical predictions and all experimental measurements so far have assumed a $K^{\ast 0}$ P-wave that decays into the $K^+\pi^-$ final state. In this paper the addition of an S-wave within the $K^+\pi^-$ system of $B^0 \to K^{\ast 0}\ell^+\ell^-$ and the subsequent impact of this on the angular distribution of the final state particles is explored. The inclusion of the S-wave causes a distinction between the values of the angular observables obtained from counting experiments and those obtained from fits to the angular distribution. The effect of a non-zero S-wave on an angular analysis of $B^0 \to K^{\ast 0}\ell^+\ell^-$ is assessed as a function of dataset size and the relative size of the S-wave amplitude. An S-wave contribution, equivalent to what is measured in $B^0 \to J/\psi K^{\ast 0}$ at BaBar, leads to a significant bias on the angular observables for datasets of above 200 signal decays. Any future experimental analysis of the $K^+\pi^-\ell^+\ell^-$ final state will have to take the S-wave contribution into account.The rare decay B ( )0( ) → K ( )∗0( ) ℓ ( )+( ) ℓ ( )−( ) is a flavour changing neutral current decay with a high sensitivity to physics beyond the Standard Model. Nearly all theoretical predictions and all experimental measurements so far have assumed a K (∗0) P-wave that decays into the K ( )+( ) π ( )−( ) final state. In this paper the addition of an S-wave within the K (+)π(−) system of B ( )0( ) → K ( )∗0( ) ℓ ( )+( ) ℓ ( )−( ) and the subsequent impact of this on the angular distribution of the final state particles is explored. The inclusion of the S-wave causes a distinction between the values of the angular observables obtained from counting experiments and those obtained from fits to the angular distribution. The effect of a non-zero S-wave on an angular analysis of B ( )0( ) → K ( )∗0( ) ℓ ( )+( ) ℓ ( )−( ) is assessed as a function of dataset size and the relative size of the S-wave amplitude. An S-wave contribution, equivalent to what is measured in B ( )0( ) → J/ψK ( )∗0( ) at BaBar, leads to a significant bias on the angular observables for datasets of above 200 signal decays. Any future experimental analysis of the K ( )+( ) π ( )−( ) ℓ ( )+( ) ℓ ( )−( ) final state will have to take the S-wave contribution into account.The rare decay $B^0 \to K^{\ast 0}\ell^+\ell^-$ is a flavour changing neutral current decay with a high sensitivity to physics beyond the Standard Model. Nearly all theoretical predictions and all experimental measurements so far have assumed a $K^{\ast 0}$ P-wave that decays into the $K^+\pi^-$ final state. In this paper the addition of an S-wave within the $K^+\pi^-$ system of $B^0 \to K^{\ast 0}\ell^+\ell^-$ and the subsequent impact of this on the angular distribution of the final state particles is explored. The inclusion of the S-wave causes a distinction between the values of the angular observables obtained from counting experiments and those obtained from fits to the angular distribution. The effect of a non-zero S-wave on an angular analysis of $B^0 \to K^{\ast 0}\ell^+\ell^-$ is assessed as a function of dataset size and the relative size of the S-wave amplitude. An S-wave contribution, equivalent to what is measured in $B^0 \to J/\psi K^{\ast 0}$ at BaBar, leads to a significant bias on the angular observables for datasets of above 200 signal decays. Any future experimental analysis of the $K^+\pi^-\ell^+\ell^-$ final state will have to take the S-wave contribution into account.arXiv:1210.5279IC-HEP-12-03IC-HEP-12-03oai:cds.cern.ch:14893722012-10-22 |
spellingShingle | Particle Physics - Phenomenology Blake, Thomas Egede, Ulrik Shires, Alex The effect of S-wave interference on the $B^0 \to K^{\ast 0}\ell^+\ell^-$ angular observables |
title | The effect of S-wave interference on the $B^0 \to K^{\ast 0}\ell^+\ell^-$ angular observables |
title_full | The effect of S-wave interference on the $B^0 \to K^{\ast 0}\ell^+\ell^-$ angular observables |
title_fullStr | The effect of S-wave interference on the $B^0 \to K^{\ast 0}\ell^+\ell^-$ angular observables |
title_full_unstemmed | The effect of S-wave interference on the $B^0 \to K^{\ast 0}\ell^+\ell^-$ angular observables |
title_short | The effect of S-wave interference on the $B^0 \to K^{\ast 0}\ell^+\ell^-$ angular observables |
title_sort | effect of s-wave interference on the $b^0 \to k^{\ast 0}\ell^+\ell^-$ angular observables |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1007/JHEP03(2013)027 http://cds.cern.ch/record/1489372 |
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