Search for Lepton Flavour Violating Decays Tau- to L- Ks with the BaBar Experiment

Search for Lepton Flavour Violating Decays Tau- to L- Ks with the BaBar Experiment

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Published: 2009

Total Pages: 9

ISBN-13:

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A search for the lepton flavor violating decays?− → l− K{sub S}° (l = e or?) has been performed using a data sample corresponding to an integrated luminosity of 469 fb−1, collected with the BABAR detector at the SLAC PEP-II ee− asymmetric energy collider. No statistically significant signal has been observed in either channel and the estimated upper limits on branching fractions are?(?− → e− K{sub S}°)


Search for Lepton Flavour Violating Decays ? {u2192} L K0s with the BABAR Detector

Search for Lepton Flavour Violating Decays ? {u2192} L K0s with the BABAR Detector

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Publisher:

Published: 2009

Total Pages: 171

ISBN-13:

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We present the search for the lepton flavour violating decay ???????? lK0s with the BaBar experiment data. This process and many other lepton flavour violating ? decays, like ???????? ?? and ???????? lll, are one of the most promising channel to search for evidence of new physics. According to the Standard Model and the neutrino mixing parameters, branching fractions are estimated well below 10-14, but many models of new physics allow for branching fractions values close to the present experimental sensitivity. This analysis is based on a data sample of 469fb-1 collected by BABAR detector at the PEP-II storage ring from 1999 to 2007, equivalent to 431 millions of ? pairs. the BABAR experiment, initially designed for studying CP violation in B mesons, has demonstrated to be one of the most suitable environments for studying ? decays. The tracking system, the calorimeter and the particle identification of BABAR, together with the knowledge of the ? initial energy, allow an extremely powerful rejection of background events that, for this analysis, is better than 10-9. Being ????????lK0s a decay mode without neutrinos, the signal ? decay can be fully reconstructed. Kinematical constraints are used in a fit that provides a decay tree reconstruction with a high resolution. For this analysis MC simulated events play a decisive role for estimating the signal efficiency and study the residual background. High statistics MC sample are produced simulating detector conditions for different periods of data collection, in order to reduce any discrepancies with the data. When discrepancies can not be removed, we perform studies to compute a correction factor or an estimation of systematic errors that need to be included in the final measurement. A significant improvement of the current result can be reached only with a higher statistics and, therefore, with a new collider providing a luminosity from 10 to 100 times more than PEP-II. A new detector, with improved performance and able to collect data in a high background environment, is also requested to fully exploit the capability of such amount of data. In fact, only keeping the efficiency and the background as similar as possible to present ones, we will be able to scale almost linearly the estimated upper limit according to the luminosity. The strong potential of improvement for the search of lepton flavour violation ? decays makes the building of such a machine highly desirable.


Search for the Lepton Flavour Violating Decay in Upsilon(3S) ->emu

Search for the Lepton Flavour Violating Decay in Upsilon(3S) ->emu

Author: Nafisa Tasneem

Publisher:

Published: 2017

Total Pages:

ISBN-13:

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Charged lepton flavour violating processes are highly suppressed in the standard model, but they are predicted to be enhanced in several new physics extensions including supersymmetry and models with leptoquarks or compositeness. Data collected with the BaBar detector at the SLAC PEP-II e$^+$e$^-$ asymmetric collider at a centre-of-mass energy of 10.36~GeV were used to search for electron-muon flavor violation in $\Upsilon (3S)\rightarrow e^{\pm}\mu^{\pm}$ decays. The search was conducted using a data sample in which 118 million $\Upsilon (3S)$ mesons were produced, corresponding to an integrated luminosity of 27~$fb^{-1}$. There is no evidence of a signal in the $\Upsilon (3S)$ data and we report our results as upper limits on $\mathcal{B}(\Upsilon(3S)\rightarrow e^{\pm}\mu^{\mp})