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Study of the $K^{+} \rightarrow \pi^{0} e^{+} \nu \gamma$ decay with NA62 experiment at CERN
I performed different measurements of $K^{+} \rightarrow \pi^{0} e^{+} \nu \gamma$ decay (Ke3$\gamma$) branching ratio normalized to $K^{+} \rightarrow \pi^{0} e^{+} \nu$ decay (Ke3) with the NA62 experiment at CERN. For $E^*_{\gamma}> 10 MeV$ and $\theta^*_{e,\gamma}> 10^\circ$, 12242 candid...
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Lenguaje: | eng |
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2017
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Acceso en línea: | http://cds.cern.ch/record/2277727 |
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author | Brizioli, Francesco |
author_facet | Brizioli, Francesco |
author_sort | Brizioli, Francesco |
collection | CERN |
description | I performed different measurements of $K^{+} \rightarrow \pi^{0} e^{+} \nu \gamma$ decay (Ke3$\gamma$) branching ratio normalized to $K^{+} \rightarrow \pi^{0} e^{+} \nu$ decay (Ke3) with the NA62 experiment at CERN. For $E^*_{\gamma}> 10 MeV$ and $\theta^*_{e,\gamma}> 10^\circ$, 12242 candidate events have been selected, with the estimated fraction of background at the level of $(3.5 \pm 1.4)\%$, and I obtained $\frac{BR(Ke3\gamma)}{BR(Ke3)} =(1.95 \pm 0.04)\%$. With the same selection the asymmetry $A_\xi = \frac{N_+ - N_-}{N_+ + N_-}$ of the T-odd observable $\xi = \frac{[\overrightarrow{p_{\gamma}} \cdot (\overrightarrow{p_e} \times \overrightarrow{p_\pi})]}{M_K^3}$ has been computed, and I measured $A_\xi = (0.016 \pm 0.017)$. The measurements are still dominated by statistical uncertainties, and they can be improved collecting and analysing more data. |
id | cern-2277727 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2017 |
record_format | invenio |
spelling | cern-22777272019-09-30T06:29:59Zhttp://cds.cern.ch/record/2277727engBrizioli, FrancescoStudy of the $K^{+} \rightarrow \pi^{0} e^{+} \nu \gamma$ decay with NA62 experiment at CERNParticle Physics - ExperimentI performed different measurements of $K^{+} \rightarrow \pi^{0} e^{+} \nu \gamma$ decay (Ke3$\gamma$) branching ratio normalized to $K^{+} \rightarrow \pi^{0} e^{+} \nu$ decay (Ke3) with the NA62 experiment at CERN. For $E^*_{\gamma}> 10 MeV$ and $\theta^*_{e,\gamma}> 10^\circ$, 12242 candidate events have been selected, with the estimated fraction of background at the level of $(3.5 \pm 1.4)\%$, and I obtained $\frac{BR(Ke3\gamma)}{BR(Ke3)} =(1.95 \pm 0.04)\%$. With the same selection the asymmetry $A_\xi = \frac{N_+ - N_-}{N_+ + N_-}$ of the T-odd observable $\xi = \frac{[\overrightarrow{p_{\gamma}} \cdot (\overrightarrow{p_e} \times \overrightarrow{p_\pi})]}{M_K^3}$ has been computed, and I measured $A_\xi = (0.016 \pm 0.017)$. The measurements are still dominated by statistical uncertainties, and they can be improved collecting and analysing more data.CERN-STUDENTS-Note-2017-014oai:cds.cern.ch:22777272017-08-09 |
spellingShingle | Particle Physics - Experiment Brizioli, Francesco Study of the $K^{+} \rightarrow \pi^{0} e^{+} \nu \gamma$ decay with NA62 experiment at CERN |
title | Study of the $K^{+} \rightarrow \pi^{0} e^{+} \nu \gamma$ decay with NA62 experiment at CERN |
title_full | Study of the $K^{+} \rightarrow \pi^{0} e^{+} \nu \gamma$ decay with NA62 experiment at CERN |
title_fullStr | Study of the $K^{+} \rightarrow \pi^{0} e^{+} \nu \gamma$ decay with NA62 experiment at CERN |
title_full_unstemmed | Study of the $K^{+} \rightarrow \pi^{0} e^{+} \nu \gamma$ decay with NA62 experiment at CERN |
title_short | Study of the $K^{+} \rightarrow \pi^{0} e^{+} \nu \gamma$ decay with NA62 experiment at CERN |
title_sort | study of the $k^{+} \rightarrow \pi^{0} e^{+} \nu \gamma$ decay with na62 experiment at cern |
topic | Particle Physics - Experiment |
url | http://cds.cern.ch/record/2277727 |
work_keys_str_mv | AT briziolifrancesco studyofthekrightarrowpi0enugammadecaywithna62experimentatcern |