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$\chi^{\vphantom\dagger}_{c0}(3915)$ As the Lightest $c\bar c s \bar s$ State

The state $\chi^{\vphantom\dagger}_{c0}(3915)$ has recently been demoted by the Particle Data Group from its previous status as the conventional $c\bar c$ $2 {}^3P_0$ state, largely due to the absence of expected $D\bar D$ decays. We propose that $\chi^{\vphantom\dagger}_{c0}(3915)$ is actually the...

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Detalles Bibliográficos
Autores principales: Lebed, Richard F., Polosa, Antonio D.
Lenguaje:eng
Publicado: 2016
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevD.93.094024
http://cds.cern.ch/record/2135044
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author Lebed, Richard F.
Polosa, Antonio D.
author_facet Lebed, Richard F.
Polosa, Antonio D.
author_sort Lebed, Richard F.
collection CERN
description The state $\chi^{\vphantom\dagger}_{c0}(3915)$ has recently been demoted by the Particle Data Group from its previous status as the conventional $c\bar c$ $2 {}^3P_0$ state, largely due to the absence of expected $D\bar D$ decays. We propose that $\chi^{\vphantom\dagger}_{c0}(3915)$ is actually the lightest $c\bar c s \bar s$ state, and calculate the spectrum of such states using the diquark model, identifying many of the observed charmoniumlike states that lack open-charm decay modes as $c\bar c s \bar s$. Among other results, we argue that $Y(4140)$ is a $J^{PC} = 1^{++}$ $c\bar c s \bar s$ state that has been not been seen in two-photon fusion largely as a consequence of the Landau-Yang theorem.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2016
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spelling cern-21350442021-05-03T20:22:39Zdoi:10.1103/PhysRevD.93.094024http://cds.cern.ch/record/2135044engLebed, Richard F.Polosa, Antonio D.$\chi^{\vphantom\dagger}_{c0}(3915)$ As the Lightest $c\bar c s \bar s$ StateParticle Physics - PhenomenologyNuclear Physics - TheoryParticle Physics - PhenomenologyThe state $\chi^{\vphantom\dagger}_{c0}(3915)$ has recently been demoted by the Particle Data Group from its previous status as the conventional $c\bar c$ $2 {}^3P_0$ state, largely due to the absence of expected $D\bar D$ decays. We propose that $\chi^{\vphantom\dagger}_{c0}(3915)$ is actually the lightest $c\bar c s \bar s$ state, and calculate the spectrum of such states using the diquark model, identifying many of the observed charmoniumlike states that lack open-charm decay modes as $c\bar c s \bar s$. Among other results, we argue that $Y(4140)$ is a $J^{PC} = 1^{++}$ $c\bar c s \bar s$ state that has been not been seen in two-photon fusion largely as a consequence of the Landau-Yang theorem.The state χc0(3915) has recently been demoted by the Particle Data Group from its previous status as the conventional cc¯ 23P0 state, largely due to the absence of expected DD¯ decays. We propose that χc0(3915) is actually the lightest cc¯ss¯ state, and calculate the spectrum of such states using the diquark model, identifying many of the observed charmoniumlike states that lack open-charm decay modes as cc¯ss¯. Among other results, we argue that Y(4140) is a JPC=1++ cc¯ss¯ state that has been not been seen in two-photon fusion largely as a consequence of the Landau-Yang theorem.The state $\chi^{\vphantom\dagger}_{c0}(3915)$ has recently been demoted by the Particle Data Group from its previous status as the conventional $c\bar c$ $2 {}^3P_0$ state, largely due to the absence of expected $D\bar D$ decays. We propose that $\chi^{\vphantom\dagger}_{c0}(3915)$ is actually the lightest $c\bar c s \bar s$ state, and calculate the spectrum of such states using the diquark model, identifying many of the observed charmoniumlike states that lack open-charm decay modes as $c\bar c s \bar s$. Among other results, we argue that $Y(4140)$ is a $J^{PC} = 1^{++}$ $c\bar c s \bar s$ state that has been not been seen in two-photon fusion largely as a consequence of the Landau-Yang theorem.arXiv:1602.08421oai:cds.cern.ch:21350442016-02-26
spellingShingle Particle Physics - Phenomenology
Nuclear Physics - Theory
Particle Physics - Phenomenology
Lebed, Richard F.
Polosa, Antonio D.
$\chi^{\vphantom\dagger}_{c0}(3915)$ As the Lightest $c\bar c s \bar s$ State
title $\chi^{\vphantom\dagger}_{c0}(3915)$ As the Lightest $c\bar c s \bar s$ State
title_full $\chi^{\vphantom\dagger}_{c0}(3915)$ As the Lightest $c\bar c s \bar s$ State
title_fullStr $\chi^{\vphantom\dagger}_{c0}(3915)$ As the Lightest $c\bar c s \bar s$ State
title_full_unstemmed $\chi^{\vphantom\dagger}_{c0}(3915)$ As the Lightest $c\bar c s \bar s$ State
title_short $\chi^{\vphantom\dagger}_{c0}(3915)$ As the Lightest $c\bar c s \bar s$ State
title_sort $\chi^{\vphantom\dagger}_{c0}(3915)$ as the lightest $c\bar c s \bar s$ state
topic Particle Physics - Phenomenology
Nuclear Physics - Theory
Particle Physics - Phenomenology
url https://dx.doi.org/10.1103/PhysRevD.93.094024
http://cds.cern.ch/record/2135044
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