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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...
Autores principales: | , |
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Lenguaje: | eng |
Publicado: |
2016
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Acceso en línea: | https://dx.doi.org/10.1103/PhysRevD.93.094024 http://cds.cern.ch/record/2135044 |
_version_ | 1780949929867345920 |
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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. |
id | cern-2135044 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2016 |
record_format | invenio |
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 |
work_keys_str_mv | AT lebedrichardf chivphantomdaggerc03915asthelightestcbarcsbarsstate AT polosaantoniod chivphantomdaggerc03915asthelightestcbarcsbarsstate |