Number of the records: 1  

Lifetime of the hypertriton

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    SYSNO ASEP0568498
    Document TypeC - Proceedings Paper (int. conf.)
    R&D Document TypeConference Paper
    TitleLifetime of the hypertriton
    Author(s) Gazda, Daniel (UJF-V) RID, ORCID, SAI
    Pérez-Obiol, A. (ES)
    Gal, A. (IL)
    Friedman, E. (IL)
    Number of authors4
    Article number01002
    Source TitleEPJ Web of Conferences, HYP2022, 271. - Les Ulis : EDP Science, 2022
    Number of pages8 s.
    Publication formOnline - E
    Action14th International Conference on Hypernuclear and Strange Particle Physics (HYP2022)
    Event date27.06.2022 - 01.07.2022
    VEvent locationPrague
    CountryCZ - Czech Republic
    Event typeWRD
    Languageeng - English
    CountryFR - France
    Keywordsrelativistic heavy ion collision ; hypertrion lifetime
    OECD categoryNuclear physics
    R&D ProjectsGA19-19640S GA ČR - Czech Science Foundation (CSF)
    GA22-14497S GA ČR - Czech Science Foundation (CSF)
    Research Infrastructuree-INFRA CZ - 90140 - CESNET, zájmové sdružení právnických osob
    Institutional supportUJF-V - RVO:61389005
    DOI10.1051/epjconf/202227101002
    AnnotationConflicting values of the hypertriton lifetime τ(3ΛH) were derived in relativistic heavy ion (RHI) collision experiments over the last decade. A very recent ALICE Collaboration measurement is the only experiment where the reported τ(3ΛH) comes sufficiently close to the free-Λ lifetime τΛ, as expected naively for a very weakly bound Λ in 3ΛH. We revisited theoretically this 3ΛH lifetime puzzle [1], using 3ΛH and 3He wave functions computed within the ab initio no-core shell model employing interactions derived from chiral effective field theory to calculate the two-body decay rate Γ(3ΛH → 3He + π−). We found significant but opposing contributions arising from ΣNN admixtures in 3ΛH and from π− − 3He final-state interaction. To derive τ(3ΛH), we evaluated the inclusive π− decay rate Γπ− (3ΛH) by using the measured branching ratio Γ(3ΛH → 3He + π−)/Γπ− (3ΛH) and added the π0 contributions through the ΔI = 1/2rule. The resulting τ(3ΛH) varies strongly with the rather poorly known Λ separation energy Esep(3ΛH) and it is thus possible to associate each one of the distinct RHI τ(3ΛH) measurements with its own underlying value of Esep(3ΛH).
    WorkplaceNuclear Physics Institute
    ContactMarkéta Sommerová, sommerova@ujf.cas.cz, Tel.: 266 173 228
    Year of Publishing2023
Number of the records: 1  

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