First branching fraction measurement of the suppressed decay Ξ c 0 → π − Λ c +

© 2020 CERN. The Ξc0 baryon is unstable and usually decays into charmless final states by the c→sud¯ transition. It can, however, also disintegrate into a π- meson and a Λc+ baryon via s quark decay or via cs→dc weak scattering. The interplay between the latter two processes governs the size of the...

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Main Author: Williams, Michael
Other Authors: Massachusetts Institute of Technology. Department of Physics
Format: Article
Language:English
Published: American Physical Society (APS) 2022
Online Access:https://hdl.handle.net/1721.1/142464
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author Williams, Michael
author2 Massachusetts Institute of Technology. Department of Physics
author_facet Massachusetts Institute of Technology. Department of Physics
Williams, Michael
author_sort Williams, Michael
collection MIT
description © 2020 CERN. The Ξc0 baryon is unstable and usually decays into charmless final states by the c→sud¯ transition. It can, however, also disintegrate into a π- meson and a Λc+ baryon via s quark decay or via cs→dc weak scattering. The interplay between the latter two processes governs the size of the branching fraction B(Ξc0→π-Λc+), first measured here to be (0.55±0.02±0.18)%, where the first uncertainty is statistical and second systematic. This result is compatible with the larger of the theoretical predictions that connect models of hyperon decays using partially conserved axial currents and SU(3) symmetry with those involving the heavy-quark expansion and heavy-quark symmetry. In addition, the branching fraction of the normalization channel, B(Ξc+→pK-π+)=(1.135±0.002±0.387)% is measured.
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spelling mit-1721.1/1424642023-06-26T19:32:34Z First branching fraction measurement of the suppressed decay Ξ c 0 → π − Λ c + Williams, Michael Massachusetts Institute of Technology. Department of Physics © 2020 CERN. The Ξc0 baryon is unstable and usually decays into charmless final states by the c→sud¯ transition. It can, however, also disintegrate into a π- meson and a Λc+ baryon via s quark decay or via cs→dc weak scattering. The interplay between the latter two processes governs the size of the branching fraction B(Ξc0→π-Λc+), first measured here to be (0.55±0.02±0.18)%, where the first uncertainty is statistical and second systematic. This result is compatible with the larger of the theoretical predictions that connect models of hyperon decays using partially conserved axial currents and SU(3) symmetry with those involving the heavy-quark expansion and heavy-quark symmetry. In addition, the branching fraction of the normalization channel, B(Ξc+→pK-π+)=(1.135±0.002±0.387)% is measured. 2022-05-11T13:43:49Z 2022-05-11T13:43:49Z 2020 2022-05-11T13:41:01Z Article http://purl.org/eprint/type/JournalArticle https://hdl.handle.net/1721.1/142464 Williams, Michael. 2020. "First branching fraction measurement of the suppressed decay Ξ c 0 → π − Λ c +." Physical Review D, 102 (7). en 10.1103/PHYSREVD.102.071101 Physical Review D Creative Commons Attribution 4.0 International License https://creativecommons.org/licenses/by/4.0 application/pdf American Physical Society (APS) APS
spellingShingle Williams, Michael
First branching fraction measurement of the suppressed decay Ξ c 0 → π − Λ c +
title First branching fraction measurement of the suppressed decay Ξ c 0 → π − Λ c +
title_full First branching fraction measurement of the suppressed decay Ξ c 0 → π − Λ c +
title_fullStr First branching fraction measurement of the suppressed decay Ξ c 0 → π − Λ c +
title_full_unstemmed First branching fraction measurement of the suppressed decay Ξ c 0 → π − Λ c +
title_short First branching fraction measurement of the suppressed decay Ξ c 0 → π − Λ c +
title_sort first branching fraction measurement of the suppressed decay ξ c 0 π λ c
url https://hdl.handle.net/1721.1/142464
work_keys_str_mv AT williamsmichael firstbranchingfractionmeasurementofthesuppresseddecayxc0plc