Observation of chicJ radiative decays to light vector mesons
Using a total of 2.74 x 10(7) decays of the psi(2S) collected with the CLEO-c detector, we present a study of chi(cJ)-->gammaV, where V=rho(0), omega, phi. The transitions chi(c1)-->gammarho(0 and chi(c1)-->gammaomega are observed with B(chi(c1)-->gammarho(0))=(2.43+/-0.19+/-0.22) x 10(-...
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Veröffentlicht in: | Physical review letters 2008-10, Vol.101 (15), p.151801-151801 |
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creator | Bennett, J V Mitchell, R E Shepherd, M R Besson, D Pedlar, T K Cronin-Hennessy, D Gao, K Y Hietala, J Kubota, Y Klein, T Lang, B W Poling, R Scott, A W Zweber, P Dobbs, S Metreveli, Z Seth, K K Tan, B J Y Tomaradze, A Libby, J Martin, L Powell, A Wilkinson, G Ecklund, K M Love, W Savinov, V Mendez, H Ge, J Y Miller, D H Shipsey, I P J Xin, B Adams, G S Hu, D Moziak, B Napolitano, J He, Q Insler, J Muramatsu, H Park, C S Thorndike, E H Yang, F Artuso, M Blusk, S Khalil, S Li, J Mountain, R Nisar, S Randrianarivony, K Sultana, N Skwarnicki, T Stone, S Wang, J C Zhang, L M Bonvicini, G Cinabro, D Dubrovin, M Lincoln, A Naik, P Rademacker, J Asner, D M Edwards, K W Reed, J Briere, R A Tatishvili, G Vogel, H Rosner, J L Alexander, J P Cassel, D G Duboscq, J E Ehrlich, R Fields, L Galik, R S Gibbons, L Gray, R Gray, S W Hartill, D L Heltsley, B K Hertz, D Hunt, J M Kandaswamy, J Kreinick, D L Kuznetsov, V E Ledoux, J Mahlke-Krüger, H Mohapatra, D Onyisi, P U E Patterson, J R Peterson, D Riley, D Ryd, A Sadoff, A J Shi, X Stroiney, S Sun, W M Wilksen, T Athar, S B Patel, R Yelton, J Rubin, P Eisenstein, B I |
description | Using a total of 2.74 x 10(7) decays of the psi(2S) collected with the CLEO-c detector, we present a study of chi(cJ)-->gammaV, where V=rho(0), omega, phi. The transitions chi(c1)-->gammarho(0 and chi(c1)-->gammaomega are observed with B(chi(c1)-->gammarho(0))=(2.43+/-0.19+/-0.22) x 10(-4) and B(chi(c1)-->gammaomega)=(8.3+/-1.5+/-1.2) x 10(-5). In the chi(c1)-->gammarho(0) transition, the final state meson is dominantly longitudinally polarized. Upper limits on the branching fractions of other chi(cJ) states to light vector mesons are presented. |
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The transitions chi(c1)-->gammarho(0 and chi(c1)-->gammaomega are observed with B(chi(c1)-->gammarho(0))=(2.43+/-0.19+/-0.22) x 10(-4) and B(chi(c1)-->gammaomega)=(8.3+/-1.5+/-1.2) x 10(-5). In the chi(c1)-->gammarho(0) transition, the final state meson is dominantly longitudinally polarized. Upper limits on the branching fractions of other chi(cJ) states to light vector mesons are presented.</description><identifier>ISSN: 0031-9007</identifier><identifier>PMID: 18999588</identifier><language>eng</language><publisher>United States</publisher><ispartof>Physical review letters, 2008-10, Vol.101 (15), p.151801-151801</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>315,782,786</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/18999588$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Bennett, J V</creatorcontrib><creatorcontrib>Mitchell, R E</creatorcontrib><creatorcontrib>Shepherd, M R</creatorcontrib><creatorcontrib>Besson, D</creatorcontrib><creatorcontrib>Pedlar, T 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S</creatorcontrib><creatorcontrib>Wang, J C</creatorcontrib><creatorcontrib>Zhang, L M</creatorcontrib><creatorcontrib>Bonvicini, G</creatorcontrib><creatorcontrib>Cinabro, D</creatorcontrib><creatorcontrib>Dubrovin, M</creatorcontrib><creatorcontrib>Lincoln, A</creatorcontrib><creatorcontrib>Naik, P</creatorcontrib><creatorcontrib>Rademacker, J</creatorcontrib><creatorcontrib>Asner, D M</creatorcontrib><creatorcontrib>Edwards, K W</creatorcontrib><creatorcontrib>Reed, J</creatorcontrib><creatorcontrib>Briere, R A</creatorcontrib><creatorcontrib>Tatishvili, G</creatorcontrib><creatorcontrib>Vogel, H</creatorcontrib><creatorcontrib>Rosner, J L</creatorcontrib><creatorcontrib>Alexander, J P</creatorcontrib><creatorcontrib>Cassel, D G</creatorcontrib><creatorcontrib>Duboscq, J E</creatorcontrib><creatorcontrib>Ehrlich, R</creatorcontrib><creatorcontrib>Fields, L</creatorcontrib><creatorcontrib>Galik, R S</creatorcontrib><creatorcontrib>Gibbons, L</creatorcontrib><creatorcontrib>Gray, R</creatorcontrib><creatorcontrib>Gray, S W</creatorcontrib><creatorcontrib>Hartill, D L</creatorcontrib><creatorcontrib>Heltsley, B K</creatorcontrib><creatorcontrib>Hertz, D</creatorcontrib><creatorcontrib>Hunt, J M</creatorcontrib><creatorcontrib>Kandaswamy, J</creatorcontrib><creatorcontrib>Kreinick, D L</creatorcontrib><creatorcontrib>Kuznetsov, V E</creatorcontrib><creatorcontrib>Ledoux, J</creatorcontrib><creatorcontrib>Mahlke-Krüger, H</creatorcontrib><creatorcontrib>Mohapatra, D</creatorcontrib><creatorcontrib>Onyisi, P U E</creatorcontrib><creatorcontrib>Patterson, J R</creatorcontrib><creatorcontrib>Peterson, D</creatorcontrib><creatorcontrib>Riley, D</creatorcontrib><creatorcontrib>Ryd, A</creatorcontrib><creatorcontrib>Sadoff, A J</creatorcontrib><creatorcontrib>Shi, X</creatorcontrib><creatorcontrib>Stroiney, S</creatorcontrib><creatorcontrib>Sun, W M</creatorcontrib><creatorcontrib>Wilksen, T</creatorcontrib><creatorcontrib>Athar, S B</creatorcontrib><creatorcontrib>Patel, R</creatorcontrib><creatorcontrib>Yelton, J</creatorcontrib><creatorcontrib>Rubin, P</creatorcontrib><creatorcontrib>Eisenstein, B I</creatorcontrib><creatorcontrib>CLEO Collaboration</creatorcontrib><title>Observation of chicJ radiative decays to light vector mesons</title><title>Physical review letters</title><addtitle>Phys Rev Lett</addtitle><description>Using a total of 2.74 x 10(7) decays of the psi(2S) collected with the CLEO-c detector, we present a study of chi(cJ)-->gammaV, where V=rho(0), omega, phi. The transitions chi(c1)-->gammarho(0 and chi(c1)-->gammaomega are observed with B(chi(c1)-->gammarho(0))=(2.43+/-0.19+/-0.22) x 10(-4) and B(chi(c1)-->gammaomega)=(8.3+/-1.5+/-1.2) x 10(-5). In the chi(c1)-->gammarho(0) transition, the final state meson is dominantly longitudinally polarized. Upper limits on the branching fractions of other chi(cJ) states to light vector mesons are presented.</description><issn>0031-9007</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2008</creationdate><recordtype>article</recordtype><recordid>eNo1j7tqwzAYRjW0NGnaVyiauhlkSbYk6FJCrwSyZDe6_GpUbMuVZEPevoGm04GPwwfnCq0JYXWlCBErdJvzNyGkpq28QataKqUaKdfoaW8ypEWXEEccPbbHYD9x0i6cpwWwA6tPGZeI-_B1LHgBW2LCA-Q45jt07XWf4f7CDTq8vhy279Vu__axfd5VU8NlJSgFK6hWnloO2gvSGi6pl9Q5abjVnlnJOfEWeK2pNsLRxivXMkqYaRTboMe_2ynFnxly6YaQLfS9HiHOuWuVEFQJchYfLuJsBnDdlMKg06n7z2W_-lZQWA</recordid><startdate>20081010</startdate><enddate>20081010</enddate><creator>Bennett, J V</creator><creator>Mitchell, R E</creator><creator>Shepherd, M R</creator><creator>Besson, D</creator><creator>Pedlar, T K</creator><creator>Cronin-Hennessy, D</creator><creator>Gao, K Y</creator><creator>Hietala, J</creator><creator>Kubota, Y</creator><creator>Klein, T</creator><creator>Lang, B W</creator><creator>Poling, 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L</creatorcontrib><creatorcontrib>Kuznetsov, V E</creatorcontrib><creatorcontrib>Ledoux, J</creatorcontrib><creatorcontrib>Mahlke-Krüger, H</creatorcontrib><creatorcontrib>Mohapatra, D</creatorcontrib><creatorcontrib>Onyisi, P U E</creatorcontrib><creatorcontrib>Patterson, J R</creatorcontrib><creatorcontrib>Peterson, D</creatorcontrib><creatorcontrib>Riley, D</creatorcontrib><creatorcontrib>Ryd, A</creatorcontrib><creatorcontrib>Sadoff, A J</creatorcontrib><creatorcontrib>Shi, X</creatorcontrib><creatorcontrib>Stroiney, S</creatorcontrib><creatorcontrib>Sun, W M</creatorcontrib><creatorcontrib>Wilksen, T</creatorcontrib><creatorcontrib>Athar, S B</creatorcontrib><creatorcontrib>Patel, R</creatorcontrib><creatorcontrib>Yelton, J</creatorcontrib><creatorcontrib>Rubin, P</creatorcontrib><creatorcontrib>Eisenstein, B I</creatorcontrib><creatorcontrib>CLEO Collaboration</creatorcontrib><collection>PubMed</collection><collection>MEDLINE - Academic</collection><jtitle>Physical review letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Bennett, J V</au><au>Mitchell, R E</au><au>Shepherd, M R</au><au>Besson, D</au><au>Pedlar, T K</au><au>Cronin-Hennessy, D</au><au>Gao, K Y</au><au>Hietala, J</au><au>Kubota, Y</au><au>Klein, T</au><au>Lang, B W</au><au>Poling, R</au><au>Scott, A W</au><au>Zweber, P</au><au>Dobbs, S</au><au>Metreveli, Z</au><au>Seth, K K</au><au>Tan, B J Y</au><au>Tomaradze, A</au><au>Libby, J</au><au>Martin, L</au><au>Powell, A</au><au>Wilkinson, G</au><au>Ecklund, K M</au><au>Love, W</au><au>Savinov, V</au><au>Mendez, H</au><au>Ge, J Y</au><au>Miller, D H</au><au>Shipsey, I P J</au><au>Xin, B</au><au>Adams, G S</au><au>Hu, D</au><au>Moziak, B</au><au>Napolitano, J</au><au>He, Q</au><au>Insler, J</au><au>Muramatsu, H</au><au>Park, C S</au><au>Thorndike, E H</au><au>Yang, F</au><au>Artuso, M</au><au>Blusk, S</au><au>Khalil, S</au><au>Li, J</au><au>Mountain, R</au><au>Nisar, S</au><au>Randrianarivony, K</au><au>Sultana, N</au><au>Skwarnicki, T</au><au>Stone, S</au><au>Wang, J C</au><au>Zhang, L M</au><au>Bonvicini, G</au><au>Cinabro, D</au><au>Dubrovin, M</au><au>Lincoln, A</au><au>Naik, P</au><au>Rademacker, J</au><au>Asner, D M</au><au>Edwards, K W</au><au>Reed, J</au><au>Briere, R A</au><au>Tatishvili, G</au><au>Vogel, H</au><au>Rosner, J L</au><au>Alexander, J P</au><au>Cassel, D G</au><au>Duboscq, J E</au><au>Ehrlich, R</au><au>Fields, L</au><au>Galik, R S</au><au>Gibbons, L</au><au>Gray, R</au><au>Gray, S W</au><au>Hartill, D L</au><au>Heltsley, B K</au><au>Hertz, D</au><au>Hunt, J M</au><au>Kandaswamy, J</au><au>Kreinick, D L</au><au>Kuznetsov, V E</au><au>Ledoux, J</au><au>Mahlke-Krüger, H</au><au>Mohapatra, D</au><au>Onyisi, P U E</au><au>Patterson, J R</au><au>Peterson, D</au><au>Riley, D</au><au>Ryd, A</au><au>Sadoff, A J</au><au>Shi, X</au><au>Stroiney, S</au><au>Sun, W M</au><au>Wilksen, T</au><au>Athar, S B</au><au>Patel, R</au><au>Yelton, J</au><au>Rubin, P</au><au>Eisenstein, B I</au><aucorp>CLEO Collaboration</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Observation of chicJ radiative decays to light vector mesons</atitle><jtitle>Physical review letters</jtitle><addtitle>Phys Rev Lett</addtitle><date>2008-10-10</date><risdate>2008</risdate><volume>101</volume><issue>15</issue><spage>151801</spage><epage>151801</epage><pages>151801-151801</pages><issn>0031-9007</issn><abstract>Using a total of 2.74 x 10(7) decays of the psi(2S) collected with the CLEO-c detector, we present a study of chi(cJ)-->gammaV, where V=rho(0), omega, phi. The transitions chi(c1)-->gammarho(0 and chi(c1)-->gammaomega are observed with B(chi(c1)-->gammarho(0))=(2.43+/-0.19+/-0.22) x 10(-4) and B(chi(c1)-->gammaomega)=(8.3+/-1.5+/-1.2) x 10(-5). In the chi(c1)-->gammarho(0) transition, the final state meson is dominantly longitudinally polarized. Upper limits on the branching fractions of other chi(cJ) states to light vector mesons are presented.</abstract><cop>United States</cop><pmid>18999588</pmid><tpages>1</tpages></addata></record> |
fulltext | fulltext |
identifier | ISSN: 0031-9007 |
ispartof | Physical review letters, 2008-10, Vol.101 (15), p.151801-151801 |
issn | 0031-9007 |
language | eng |
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source | American Physical Society Journals |
title | Observation of chicJ radiative decays to light vector mesons |
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