Spin-parity analysis of pp¯ mass threshold structure in J/ψ and ψ(3686) radiative decays

A partial wave analysis of the pp¯ mass-threshold enhancement in the reaction J/ψ→γpp¯ is used to determine its J(PC) quantum numbers to be 0(-+), its peak mass to be below threshold at M=1832(-5)(+19)(stat)(-17)(+18)(syst)±19(model) MeV/c(2), and its total width to be Γ

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Veröffentlicht in:Physical review letters 2012-03, Vol.108 (11), p.112003-112003
Hauptverfasser: Ablikim, M, Achasov, M N, Alberto, D, Ambrose, D J, An, F F, An, Q, An, Z H, Bai, J Z, Baldini Ferroli, R B F, Ban, Y, Becker, J, Berger, N, Bertani, M B, Bian, J M, Boger, E, Bondarenko, O, Boyko, I, Briere, R A, Bytev, V, Cai, X, Calcaterra, A C, Cao, G F, Chang, J F, Chelkov, G, Chen, G, Chen, H S, Chen, J C, Chen, M L, Chen, S J, Chen, Y, Chen, Y B, Cheng, H P, Chu, Y P, Cronin-Hennessy, D, Dai, H L, Dai, J P, Dedovich, D, Deng, Z Y, Denysenko, I, Destefanis, M, Ding Ding, W L, Ding, Y, Dong, L Y, Dong, M Y, Du, S X, Fang, J, Fang, S S, Feng, C Q, Fu, C D, Fu, J L, Gao, Y, Geng, C, Goetzen, K, Gong, W X, Greco, M, Gu, M H, Gu, Y T, Guan, Y H, Guo, A Q, Guo, L B, Guo, Y P, Han, Y L, Hao, X Q, Harris, F A, He, K L, He, M, He, Z Y, Heng, Y K, Hou, Z L, Hu, H M, Hu, J F, Hu, T, Huang, B, Huang, G M, Huang, J S, Huang, X T, Huang, Y P, Hussain, T, Ji, C S, Ji, Q, Ji, X B, Ji, X L, Jia, L K, Jiang, L L, Jiang, X S, Jiao, J B, Jiao, Z, Jin, D P, Jin, S, Jing, F F, Kalantar-Nayestanaki, N, Kavatsyuk, M, Kuehn, W, Lai, W, Lange, J S, Leung, J K C, Li, C H, Li, Cheng, Li, Cui, Li, D M
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container_issue 11
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container_title Physical review letters
container_volume 108
creator Ablikim, M
Achasov, M N
Alberto, D
Ambrose, D J
An, F F
An, Q
An, Z H
Bai, J Z
Baldini Ferroli, R B F
Ban, Y
Becker, J
Berger, N
Bertani, M B
Bian, J M
Boger, E
Bondarenko, O
Boyko, I
Briere, R A
Bytev, V
Cai, X
Calcaterra, A C
Cao, G F
Chang, J F
Chelkov, G
Chen, G
Chen, H S
Chen, J C
Chen, M L
Chen, S J
Chen, Y
Chen, Y B
Cheng, H P
Chu, Y P
Cronin-Hennessy, D
Dai, H L
Dai, J P
Dedovich, D
Deng, Z Y
Denysenko, I
Destefanis, M
Ding Ding, W L
Ding, Y
Dong, L Y
Dong, M Y
Du, S X
Fang, J
Fang, S S
Feng, C Q
Fu, C D
Fu, J L
Gao, Y
Geng, C
Goetzen, K
Gong, W X
Greco, M
Gu, M H
Gu, Y T
Guan, Y H
Guo, A Q
Guo, L B
Guo, Y P
Han, Y L
Hao, X Q
Harris, F A
He, K L
He, M
He, Z Y
Heng, Y K
Hou, Z L
Hu, H M
Hu, J F
Hu, T
Huang, B
Huang, G M
Huang, J S
Huang, X T
Huang, Y P
Hussain, T
Ji, C S
Ji, Q
Ji, X B
Ji, X L
Jia, L K
Jiang, L L
Jiang, X S
Jiao, J B
Jiao, Z
Jin, D P
Jin, S
Jing, F F
Kalantar-Nayestanaki, N
Kavatsyuk, M
Kuehn, W
Lai, W
Lange, J S
Leung, J K C
Li, C H
Li, Cheng
Li, Cui
Li, D M
description A partial wave analysis of the pp¯ mass-threshold enhancement in the reaction J/ψ→γpp¯ is used to determine its J(PC) quantum numbers to be 0(-+), its peak mass to be below threshold at M=1832(-5)(+19)(stat)(-17)(+18)(syst)±19(model) MeV/c(2), and its total width to be Γ
doi_str_mv 10.1103/PhysRevLett.108.112003
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Y</creatorcontrib><creatorcontrib>Heng, Y K</creatorcontrib><creatorcontrib>Hou, Z L</creatorcontrib><creatorcontrib>Hu, H M</creatorcontrib><creatorcontrib>Hu, J F</creatorcontrib><creatorcontrib>Hu, T</creatorcontrib><creatorcontrib>Huang, B</creatorcontrib><creatorcontrib>Huang, G M</creatorcontrib><creatorcontrib>Huang, J S</creatorcontrib><creatorcontrib>Huang, X T</creatorcontrib><creatorcontrib>Huang, Y P</creatorcontrib><creatorcontrib>Hussain, T</creatorcontrib><creatorcontrib>Ji, C S</creatorcontrib><creatorcontrib>Ji, Q</creatorcontrib><creatorcontrib>Ji, X B</creatorcontrib><creatorcontrib>Ji, X L</creatorcontrib><creatorcontrib>Jia, L K</creatorcontrib><creatorcontrib>Jiang, L L</creatorcontrib><creatorcontrib>Jiang, X S</creatorcontrib><creatorcontrib>Jiao, J B</creatorcontrib><creatorcontrib>Jiao, Z</creatorcontrib><creatorcontrib>Jin, D P</creatorcontrib><creatorcontrib>Jin, S</creatorcontrib><creatorcontrib>Jing, F F</creatorcontrib><creatorcontrib>Kalantar-Nayestanaki, N</creatorcontrib><creatorcontrib>Kavatsyuk, M</creatorcontrib><creatorcontrib>Kuehn, W</creatorcontrib><creatorcontrib>Lai, W</creatorcontrib><creatorcontrib>Lange, J S</creatorcontrib><creatorcontrib>Leung, J K C</creatorcontrib><creatorcontrib>Li, C H</creatorcontrib><creatorcontrib>Li, Cheng</creatorcontrib><creatorcontrib>Li, Cui</creatorcontrib><creatorcontrib>Li, D M</creatorcontrib><creatorcontrib>BESIII Collaboration</creatorcontrib><title>Spin-parity analysis of pp¯ mass threshold structure in J/ψ and ψ(3686) radiative decays</title><title>Physical review letters</title><addtitle>Phys Rev Lett</addtitle><description>A partial wave analysis of the pp¯ mass-threshold enhancement in the reaction J/ψ→γpp¯ is used to determine its J(PC) quantum numbers to be 0(-+), its peak mass to be below threshold at M=1832(-5)(+19)(stat)(-17)(+18)(syst)±19(model) MeV/c(2), and its total width to be Γ&lt;76 MeV/c(2) at the 90% C.L. The product of branching ratios is measured to be BR[J/ψ→γX(pp¯)]BR[X(pp¯)→pp¯]=[9.0(-1.1)(+0.4)(stat)(-5.0)(+1.5)(syst)±2.3(model)]×10(-5). A similar analysis performed on ψ(3686)→γpp¯ decays shows, for the first time, the presence of a corresponding enhancement with a production rate relative to that for J/ψ decays of R=[5.08(-0.45)(+0.71)(stat)(-3.58)(+0.67)(syst)±0.12(model)]%.</description><issn>0031-9007</issn><issn>1079-7114</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2012</creationdate><recordtype>article</recordtype><recordid>eNo10EtOwzAQBmALgWgpXKGyWJVF2vEjibNEiKcqgXisWESO4ypGaRJsp1Ju0NtwBy7QK2GpZTXSP9_M4kdoSmBOCLDFSzW4V71Zau_nBEQIKQA7QmMCaRalhPBjNA4JiTKAdITOnPsCAEITcYpGlMYceJKO0edbZ5qok9b4ActG1oMzDrcr3HW_P3gtncO-stpVbV1i522vfG81Ng1-Wuy24aLEu-2MJSK5wlaWRnqz0bjUSg7uHJ2sZO30xWFO0Mfd7fvNQ7R8vn-8uV5GLYmZjwgVScaFihkVqSokh6IkKgHGi2RFtVIUZJIJHTZEKEkVg4xnaZERzkVRUDZBl_u_rfMmd8p4rSrVNo1WPg9tcUpZQLM96mz73Wvn87VxSte1bHTbu5xAgBmPBQQ6PdC-WOsy76xZSzvk_62xP-T3cXM</recordid><startdate>20120316</startdate><enddate>20120316</enddate><creator>Ablikim, M</creator><creator>Achasov, M 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radiative decays</title><author>Ablikim, M ; Achasov, M N ; Alberto, D ; Ambrose, D J ; An, F F ; An, Q ; An, Z H ; Bai, J Z ; Baldini Ferroli, R B F ; Ban, Y ; Becker, J ; Berger, N ; Bertani, M B ; Bian, J M ; Boger, E ; Bondarenko, O ; Boyko, I ; Briere, R A ; Bytev, V ; Cai, X ; Calcaterra, A C ; Cao, G F ; Chang, J F ; Chelkov, G ; Chen, G ; Chen, H S ; Chen, J C ; Chen, M L ; Chen, S J ; Chen, Y ; Chen, Y B ; Cheng, H P ; Chu, Y P ; Cronin-Hennessy, D ; Dai, H L ; Dai, J P ; Dedovich, D ; Deng, Z Y ; Denysenko, I ; Destefanis, M ; Ding Ding, W L ; Ding, Y ; Dong, L Y ; Dong, M Y ; Du, S X ; Fang, J ; Fang, S S ; Feng, C Q ; Fu, C D ; Fu, J L ; Gao, Y ; Geng, C ; Goetzen, K ; Gong, W X ; Greco, M ; Gu, M H ; Gu, Y T ; Guan, Y H ; Guo, A Q ; Guo, L B ; Guo, Y P ; Han, Y L ; Hao, X Q ; Harris, F A ; He, K L ; He, M ; He, Z Y ; Heng, Y K ; Hou, Z L ; Hu, H M ; Hu, J F ; Hu, T ; Huang, B ; Huang, G M ; Huang, J S ; Huang, X T ; Huang, Y P ; Hussain, T ; Ji, C S ; Ji, Q ; Ji, X B ; Ji, X L ; Jia, L K ; Jiang, L L ; Jiang, X S ; Jiao, J B ; Jiao, Z ; Jin, D P ; Jin, S ; Jing, F F ; Kalantar-Nayestanaki, N ; Kavatsyuk, M ; Kuehn, W ; Lai, W ; Lange, J S ; Leung, J K C ; Li, C H ; Li, Cheng ; Li, Cui ; Li, D M</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-o153t-1286948c53287cba40bd1c6034b6f2ecc20a698eba418ca2c309497b91448bb23</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2012</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Ablikim, M</creatorcontrib><creatorcontrib>Achasov, M N</creatorcontrib><creatorcontrib>Alberto, D</creatorcontrib><creatorcontrib>Ambrose, D J</creatorcontrib><creatorcontrib>An, F F</creatorcontrib><creatorcontrib>An, Q</creatorcontrib><creatorcontrib>An, Z H</creatorcontrib><creatorcontrib>Bai, J Z</creatorcontrib><creatorcontrib>Baldini Ferroli, R B F</creatorcontrib><creatorcontrib>Ban, Y</creatorcontrib><creatorcontrib>Becker, J</creatorcontrib><creatorcontrib>Berger, N</creatorcontrib><creatorcontrib>Bertani, M B</creatorcontrib><creatorcontrib>Bian, J M</creatorcontrib><creatorcontrib>Boger, E</creatorcontrib><creatorcontrib>Bondarenko, O</creatorcontrib><creatorcontrib>Boyko, I</creatorcontrib><creatorcontrib>Briere, R A</creatorcontrib><creatorcontrib>Bytev, V</creatorcontrib><creatorcontrib>Cai, X</creatorcontrib><creatorcontrib>Calcaterra, A C</creatorcontrib><creatorcontrib>Cao, G F</creatorcontrib><creatorcontrib>Chang, J F</creatorcontrib><creatorcontrib>Chelkov, G</creatorcontrib><creatorcontrib>Chen, G</creatorcontrib><creatorcontrib>Chen, H S</creatorcontrib><creatorcontrib>Chen, J C</creatorcontrib><creatorcontrib>Chen, M L</creatorcontrib><creatorcontrib>Chen, S J</creatorcontrib><creatorcontrib>Chen, Y</creatorcontrib><creatorcontrib>Chen, Y B</creatorcontrib><creatorcontrib>Cheng, H P</creatorcontrib><creatorcontrib>Chu, Y P</creatorcontrib><creatorcontrib>Cronin-Hennessy, D</creatorcontrib><creatorcontrib>Dai, H L</creatorcontrib><creatorcontrib>Dai, J P</creatorcontrib><creatorcontrib>Dedovich, D</creatorcontrib><creatorcontrib>Deng, Z Y</creatorcontrib><creatorcontrib>Denysenko, I</creatorcontrib><creatorcontrib>Destefanis, M</creatorcontrib><creatorcontrib>Ding Ding, W L</creatorcontrib><creatorcontrib>Ding, Y</creatorcontrib><creatorcontrib>Dong, L Y</creatorcontrib><creatorcontrib>Dong, M Y</creatorcontrib><creatorcontrib>Du, S X</creatorcontrib><creatorcontrib>Fang, J</creatorcontrib><creatorcontrib>Fang, S S</creatorcontrib><creatorcontrib>Feng, C Q</creatorcontrib><creatorcontrib>Fu, C D</creatorcontrib><creatorcontrib>Fu, J L</creatorcontrib><creatorcontrib>Gao, Y</creatorcontrib><creatorcontrib>Geng, C</creatorcontrib><creatorcontrib>Goetzen, K</creatorcontrib><creatorcontrib>Gong, W X</creatorcontrib><creatorcontrib>Greco, M</creatorcontrib><creatorcontrib>Gu, M H</creatorcontrib><creatorcontrib>Gu, Y T</creatorcontrib><creatorcontrib>Guan, Y H</creatorcontrib><creatorcontrib>Guo, A Q</creatorcontrib><creatorcontrib>Guo, L B</creatorcontrib><creatorcontrib>Guo, Y P</creatorcontrib><creatorcontrib>Han, Y L</creatorcontrib><creatorcontrib>Hao, X Q</creatorcontrib><creatorcontrib>Harris, F A</creatorcontrib><creatorcontrib>He, K L</creatorcontrib><creatorcontrib>He, M</creatorcontrib><creatorcontrib>He, Z Y</creatorcontrib><creatorcontrib>Heng, Y K</creatorcontrib><creatorcontrib>Hou, Z L</creatorcontrib><creatorcontrib>Hu, H M</creatorcontrib><creatorcontrib>Hu, J F</creatorcontrib><creatorcontrib>Hu, T</creatorcontrib><creatorcontrib>Huang, B</creatorcontrib><creatorcontrib>Huang, G M</creatorcontrib><creatorcontrib>Huang, J S</creatorcontrib><creatorcontrib>Huang, X T</creatorcontrib><creatorcontrib>Huang, Y P</creatorcontrib><creatorcontrib>Hussain, T</creatorcontrib><creatorcontrib>Ji, C S</creatorcontrib><creatorcontrib>Ji, Q</creatorcontrib><creatorcontrib>Ji, X B</creatorcontrib><creatorcontrib>Ji, X L</creatorcontrib><creatorcontrib>Jia, L K</creatorcontrib><creatorcontrib>Jiang, L L</creatorcontrib><creatorcontrib>Jiang, X S</creatorcontrib><creatorcontrib>Jiao, J B</creatorcontrib><creatorcontrib>Jiao, Z</creatorcontrib><creatorcontrib>Jin, D P</creatorcontrib><creatorcontrib>Jin, S</creatorcontrib><creatorcontrib>Jing, F F</creatorcontrib><creatorcontrib>Kalantar-Nayestanaki, N</creatorcontrib><creatorcontrib>Kavatsyuk, M</creatorcontrib><creatorcontrib>Kuehn, W</creatorcontrib><creatorcontrib>Lai, W</creatorcontrib><creatorcontrib>Lange, J S</creatorcontrib><creatorcontrib>Leung, J K C</creatorcontrib><creatorcontrib>Li, C H</creatorcontrib><creatorcontrib>Li, Cheng</creatorcontrib><creatorcontrib>Li, Cui</creatorcontrib><creatorcontrib>Li, D M</creatorcontrib><creatorcontrib>BESIII Collaboration</creatorcontrib><collection>PubMed</collection><collection>MEDLINE - Academic</collection><collection>OSTI.GOV</collection><jtitle>Physical review letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Ablikim, M</au><au>Achasov, M N</au><au>Alberto, D</au><au>Ambrose, D J</au><au>An, F F</au><au>An, Q</au><au>An, Z H</au><au>Bai, J Z</au><au>Baldini Ferroli, R B F</au><au>Ban, Y</au><au>Becker, J</au><au>Berger, N</au><au>Bertani, M B</au><au>Bian, J M</au><au>Boger, E</au><au>Bondarenko, O</au><au>Boyko, I</au><au>Briere, R A</au><au>Bytev, V</au><au>Cai, X</au><au>Calcaterra, A C</au><au>Cao, G F</au><au>Chang, J F</au><au>Chelkov, G</au><au>Chen, G</au><au>Chen, H S</au><au>Chen, J C</au><au>Chen, M L</au><au>Chen, S J</au><au>Chen, Y</au><au>Chen, Y B</au><au>Cheng, H P</au><au>Chu, Y P</au><au>Cronin-Hennessy, D</au><au>Dai, H L</au><au>Dai, J P</au><au>Dedovich, D</au><au>Deng, Z Y</au><au>Denysenko, I</au><au>Destefanis, M</au><au>Ding Ding, W L</au><au>Ding, Y</au><au>Dong, L Y</au><au>Dong, M Y</au><au>Du, S X</au><au>Fang, J</au><au>Fang, S S</au><au>Feng, C Q</au><au>Fu, C D</au><au>Fu, J L</au><au>Gao, Y</au><au>Geng, C</au><au>Goetzen, K</au><au>Gong, W X</au><au>Greco, M</au><au>Gu, M H</au><au>Gu, Y T</au><au>Guan, Y H</au><au>Guo, A Q</au><au>Guo, L B</au><au>Guo, Y P</au><au>Han, Y L</au><au>Hao, X Q</au><au>Harris, F A</au><au>He, K L</au><au>He, M</au><au>He, Z Y</au><au>Heng, Y K</au><au>Hou, Z L</au><au>Hu, H M</au><au>Hu, J F</au><au>Hu, T</au><au>Huang, B</au><au>Huang, G M</au><au>Huang, J S</au><au>Huang, X T</au><au>Huang, Y P</au><au>Hussain, T</au><au>Ji, C S</au><au>Ji, Q</au><au>Ji, X B</au><au>Ji, X L</au><au>Jia, L K</au><au>Jiang, L L</au><au>Jiang, X S</au><au>Jiao, J B</au><au>Jiao, Z</au><au>Jin, D P</au><au>Jin, S</au><au>Jing, F F</au><au>Kalantar-Nayestanaki, N</au><au>Kavatsyuk, M</au><au>Kuehn, W</au><au>Lai, W</au><au>Lange, J S</au><au>Leung, J K C</au><au>Li, C H</au><au>Li, Cheng</au><au>Li, Cui</au><au>Li, D M</au><aucorp>BESIII Collaboration</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Spin-parity analysis of pp¯ mass threshold structure in J/ψ and ψ(3686) radiative decays</atitle><jtitle>Physical review letters</jtitle><addtitle>Phys Rev Lett</addtitle><date>2012-03-16</date><risdate>2012</risdate><volume>108</volume><issue>11</issue><spage>112003</spage><epage>112003</epage><pages>112003-112003</pages><issn>0031-9007</issn><eissn>1079-7114</eissn><abstract>A partial wave analysis of the pp¯ mass-threshold enhancement in the reaction J/ψ→γpp¯ is used to determine its J(PC) quantum numbers to be 0(-+), its peak mass to be below threshold at M=1832(-5)(+19)(stat)(-17)(+18)(syst)±19(model) MeV/c(2), and its total width to be Γ&lt;76 MeV/c(2) at the 90% C.L. The product of branching ratios is measured to be BR[J/ψ→γX(pp¯)]BR[X(pp¯)→pp¯]=[9.0(-1.1)(+0.4)(stat)(-5.0)(+1.5)(syst)±2.3(model)]×10(-5). A similar analysis performed on ψ(3686)→γpp¯ decays shows, for the first time, the presence of a corresponding enhancement with a production rate relative to that for J/ψ decays of R=[5.08(-0.45)(+0.71)(stat)(-3.58)(+0.67)(syst)±0.12(model)]%.</abstract><cop>United States</cop><pub>American Physical Society</pub><pmid>22540467</pmid><doi>10.1103/PhysRevLett.108.112003</doi><tpages>1</tpages></addata></record>
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source American Physical Society Journals
title Spin-parity analysis of pp¯ mass threshold structure in J/ψ and ψ(3686) radiative decays
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