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Precision flavour physics with $B\to K\nu\bar\nu$ and $B\to Kl^+l^-$
We discuss how the combined analysis of $B\to K\nu\bar\nu$ and $B\to Kl^+l^-$ can provide us with new physics tests practically free of form factor uncertainties. Residual theory errors are at the level of several percent. This study underlines the excellent motivation for measuring these modes at a...
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Lenguaje: | eng |
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2010
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Acceso en línea: | https://dx.doi.org/10.1016/j.nuclphysbps.2010.12.023 http://cds.cern.ch/record/1300101 |
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author | Buchalla, Gerhard |
author_facet | Buchalla, Gerhard |
author_sort | Buchalla, Gerhard |
collection | CERN |
description | We discuss how the combined analysis of $B\to K\nu\bar\nu$ and $B\to Kl^+l^-$ can provide us with new physics tests practically free of form factor uncertainties. Residual theory errors are at the level of several percent. This study underlines the excellent motivation for measuring these modes at a Super Flavour Factory, or, in the case of $B\to Kl^+l^-$, also at a hadron collider. |
id | cern-1300101 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2010 |
record_format | invenio |
spelling | cern-13001012023-03-15T19:12:03Zdoi:10.1016/j.nuclphysbps.2010.12.023http://cds.cern.ch/record/1300101engBuchalla, GerhardPrecision flavour physics with $B\to K\nu\bar\nu$ and $B\to Kl^+l^-$Particle Physics - PhenomenologyWe discuss how the combined analysis of $B\to K\nu\bar\nu$ and $B\to Kl^+l^-$ can provide us with new physics tests practically free of form factor uncertainties. Residual theory errors are at the level of several percent. This study underlines the excellent motivation for measuring these modes at a Super Flavour Factory, or, in the case of $B\to Kl^+l^-$, also at a hadron collider.We discuss how the combined analysis of $B\to K\nu\bar\nu$ and $B\to Kl^+l^-$ can provide us with new physics tests practically free of form factor uncertainties. Residual theory errors are at the level of several percent. This study underlines the excellent motivation for measuring these modes at a Super Flavour Factory, or, in the case of $B\to Kl^+l^-$, also at a hadron collider.arXiv:1010.2674CERN-PH-TH-2010-232CERN-PH-TH-2010-232oai:cds.cern.ch:13001012010-10-14 |
spellingShingle | Particle Physics - Phenomenology Buchalla, Gerhard Precision flavour physics with $B\to K\nu\bar\nu$ and $B\to Kl^+l^-$ |
title | Precision flavour physics with $B\to K\nu\bar\nu$ and $B\to Kl^+l^-$ |
title_full | Precision flavour physics with $B\to K\nu\bar\nu$ and $B\to Kl^+l^-$ |
title_fullStr | Precision flavour physics with $B\to K\nu\bar\nu$ and $B\to Kl^+l^-$ |
title_full_unstemmed | Precision flavour physics with $B\to K\nu\bar\nu$ and $B\to Kl^+l^-$ |
title_short | Precision flavour physics with $B\to K\nu\bar\nu$ and $B\to Kl^+l^-$ |
title_sort | precision flavour physics with $b\to k\nu\bar\nu$ and $b\to kl^+l^-$ |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1016/j.nuclphysbps.2010.12.023 http://cds.cern.ch/record/1300101 |
work_keys_str_mv | AT buchallagerhard precisionflavourphysicswithbtoknubarnuandbtokll |