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Supplemental figures: $^{3}_{\Lambda}\mathrm{H}$ and $^{3}_{\overline{\Lambda}}\mathrm{\overline{H}}$ lifetime measurement in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = $ 5.02 TeV via two-body decay

The following note presents supplemental figures for the paper: $^{3}_{\Lambda}\mathrm{H}$ and $^{3}_{\overline{\Lambda}}\mathrm{\overline{H}}$ lifetime measurement in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = $ 5.02 TeV via two-body decay \cite{Acharya:2019tauh3l}. The (anti-)\hyptriton lifetim...

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Lenguaje:eng
Publicado: 2019
Materias:
Acceso en línea:http://cds.cern.ch/record/2682029
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collection CERN
description The following note presents supplemental figures for the paper: $^{3}_{\Lambda}\mathrm{H}$ and $^{3}_{\overline{\Lambda}}\mathrm{\overline{H}}$ lifetime measurement in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = $ 5.02 TeV via two-body decay \cite{Acharya:2019tauh3l}. The (anti-)\hyptriton lifetime has been measured by analyzing the data sample of Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = $ 5.02 TeV with two methods: the exponential fit to the d$N$/d($ct$) spectrum and the unbinned fit. The results obtained with the two methods are compatible as reported in \cite{Acharya:2019tauh3l}. In this note two additional figures related to unbinned fit method are presented.
id cern-2682029
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2019
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spelling cern-26820292021-12-21T09:32:57Zhttp://cds.cern.ch/record/2682029engSupplemental figures: $^{3}_{\Lambda}\mathrm{H}$ and $^{3}_{\overline{\Lambda}}\mathrm{\overline{H}}$ lifetime measurement in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = $ 5.02 TeV via two-body decayNuclear Physics - ExperimentThe following note presents supplemental figures for the paper: $^{3}_{\Lambda}\mathrm{H}$ and $^{3}_{\overline{\Lambda}}\mathrm{\overline{H}}$ lifetime measurement in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = $ 5.02 TeV via two-body decay \cite{Acharya:2019tauh3l}. The (anti-)\hyptriton lifetime has been measured by analyzing the data sample of Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = $ 5.02 TeV with two methods: the exponential fit to the d$N$/d($ct$) spectrum and the unbinned fit. The results obtained with the two methods are compatible as reported in \cite{Acharya:2019tauh3l}. In this note two additional figures related to unbinned fit method are presented.ALICE-PUBLIC-2019-003oai:cds.cern.ch:26820292019
spellingShingle Nuclear Physics - Experiment
Supplemental figures: $^{3}_{\Lambda}\mathrm{H}$ and $^{3}_{\overline{\Lambda}}\mathrm{\overline{H}}$ lifetime measurement in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = $ 5.02 TeV via two-body decay
title Supplemental figures: $^{3}_{\Lambda}\mathrm{H}$ and $^{3}_{\overline{\Lambda}}\mathrm{\overline{H}}$ lifetime measurement in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = $ 5.02 TeV via two-body decay
title_full Supplemental figures: $^{3}_{\Lambda}\mathrm{H}$ and $^{3}_{\overline{\Lambda}}\mathrm{\overline{H}}$ lifetime measurement in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = $ 5.02 TeV via two-body decay
title_fullStr Supplemental figures: $^{3}_{\Lambda}\mathrm{H}$ and $^{3}_{\overline{\Lambda}}\mathrm{\overline{H}}$ lifetime measurement in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = $ 5.02 TeV via two-body decay
title_full_unstemmed Supplemental figures: $^{3}_{\Lambda}\mathrm{H}$ and $^{3}_{\overline{\Lambda}}\mathrm{\overline{H}}$ lifetime measurement in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = $ 5.02 TeV via two-body decay
title_short Supplemental figures: $^{3}_{\Lambda}\mathrm{H}$ and $^{3}_{\overline{\Lambda}}\mathrm{\overline{H}}$ lifetime measurement in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = $ 5.02 TeV via two-body decay
title_sort supplemental figures: $^{3}_{\lambda}\mathrm{h}$ and $^{3}_{\overline{\lambda}}\mathrm{\overline{h}}$ lifetime measurement in pb-pb collisions at $\sqrt{s_{\mathrm{nn}}} = $ 5.02 tev via two-body decay
topic Nuclear Physics - Experiment
url http://cds.cern.ch/record/2682029