Observation of exotic meson production in the reaction {pi}{sup -} p {yields} {eta}{prime} {pi}{sup -} p at 18 GeV/c
An amplitude analysis of an exclusive sample of 5765 events from the reaction {pi}{sup -} p {yields} {eta}{prime}{pi}{sup -} p at 18 GeV/c is described. The {eta}{prime}{pi}{sup -} production is dominated by natural parity exchange and by three partial waves: those with J{sup PC} = 1{sup -+}, 2{sup...
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creator | Z. Bar-Yam Amiran Tomaradze A.A. Yershov Alexander Ostrovidov A.V. Popov C. Olchanski David Joffe D.B. White D.I. Ryabchikov Doran Stienike D.S. Brown Dennis Weygand E. King Gary Adams Hans Willutzki I.A. Kachaev I.N. Vardanian J.A. Smith James Bishop John LoSecco John P. Dowd James Napolitano Joachim Kuhn Joseph Manak John Cummings K. Danyo Kamal Seth Ludmilla Sarycheva M. Hayek M.A. Kostin Michael Witkowski Mina Nozar N. Shenhav N.B. Sinev Neal Cason O.L. Kodolova Paul Eugenio R.W. Hackenburg Sydney Taegar Sergey Denisov Suh-Urk Chung Todd Adams Todd Pedlar V.A. Bodyagin V.A. Dorofeev V.L. Korotkikh V.V. Lipaev W. Kern William Shephard Xiao Shen X.L. Fan |
description | An amplitude analysis of an exclusive sample of 5765 events from the reaction {pi}{sup -} p {yields} {eta}{prime}{pi}{sup -} p at 18 GeV/c is described. The {eta}{prime}{pi}{sup -} production is dominated by natural parity exchange and by three partial waves: those with J{sup PC} = 1{sup -+}, 2{sup ++}, and 4{sup ++}. A mass-dependent analysis of the partial-wave amplitudes indicates the production of the a{sub 2}(1320) meson as well as the a{sub 4}(2040) meson, observed for the first time decaying to {eta}{prime}{pi}{sup -}. The dominant, exotic (non-q{bar q}) 1{sup -+} partial wave is shown to be resonant with a mass of 1.597 {+-} 0.010{sub -0.010}{sup +0.045} GeV/c{sup 2} and a width of 0.340 {+-} 0.040 {+-} 0.050 GeV/c{sup 2}. This exotic state, the {pi}{sub 1}(1600), is produced with a t dependence which is different from that of the a{sub 2}(1320) meson, indicating differences between the production mechanisms for the two states. |
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White ; D.I. Ryabchikov ; Doran Stienike ; D.S. Brown ; Dennis Weygand ; E. King ; Gary Adams ; Hans Willutzki ; I.A. Kachaev ; I.N. Vardanian ; J.A. Smith ; James Bishop ; John LoSecco ; John P. Dowd ; James Napolitano ; Joachim Kuhn ; Joseph Manak ; John Cummings ; K. Danyo ; Kamal Seth ; Ludmilla Sarycheva ; M. Hayek ; M.A. Kostin ; Michael Witkowski ; Mina Nozar ; N. Shenhav ; N.B. Sinev ; Neal Cason ; O.L. Kodolova ; Paul Eugenio ; R.W. Hackenburg ; Sydney Taegar ; Sergey Denisov ; Suh-Urk Chung ; Todd Adams ; Todd Pedlar ; V.A. Bodyagin ; V.A. Dorofeev ; V.L. Korotkikh ; V.V. Lipaev ; W. Kern ; William Shephard ; Xiao Shen ; X.L. Fan</creator><creatorcontrib>Z. Bar-Yam ; Amiran Tomaradze ; A.A. Yershov ; Alexander Ostrovidov ; A.V. Popov ; C. Olchanski ; David Joffe ; D.B. White ; D.I. Ryabchikov ; Doran Stienike ; D.S. Brown ; Dennis Weygand ; E. King ; Gary Adams ; Hans Willutzki ; I.A. Kachaev ; I.N. Vardanian ; J.A. Smith ; James Bishop ; John LoSecco ; John P. Dowd ; James Napolitano ; Joachim Kuhn ; Joseph Manak ; John Cummings ; K. Danyo ; Kamal Seth ; Ludmilla Sarycheva ; M. Hayek ; M.A. Kostin ; Michael Witkowski ; Mina Nozar ; N. Shenhav ; N.B. Sinev ; Neal Cason ; O.L. Kodolova ; Paul Eugenio ; R.W. Hackenburg ; Sydney Taegar ; Sergey Denisov ; Suh-Urk Chung ; Todd Adams ; Todd Pedlar ; V.A. Bodyagin ; V.A. Dorofeev ; V.L. Korotkikh ; V.V. Lipaev ; W. Kern ; William Shephard ; Xiao Shen ; X.L. Fan ; Thomas Jefferson National Accelerator Facility, Newport News, VA (US)</creatorcontrib><description>An amplitude analysis of an exclusive sample of 5765 events from the reaction {pi}{sup -} p {yields} {eta}{prime}{pi}{sup -} p at 18 GeV/c is described. The {eta}{prime}{pi}{sup -} production is dominated by natural parity exchange and by three partial waves: those with J{sup PC} = 1{sup -+}, 2{sup ++}, and 4{sup ++}. A mass-dependent analysis of the partial-wave amplitudes indicates the production of the a{sub 2}(1320) meson as well as the a{sub 4}(2040) meson, observed for the first time decaying to {eta}{prime}{pi}{sup -}. The dominant, exotic (non-q{bar q}) 1{sup -+} partial wave is shown to be resonant with a mass of 1.597 {+-} 0.010{sub -0.010}{sup +0.045} GeV/c{sup 2} and a width of 0.340 {+-} 0.040 {+-} 0.050 GeV/c{sup 2}. 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Bar-Yam</creatorcontrib><creatorcontrib>Amiran Tomaradze</creatorcontrib><creatorcontrib>A.A. Yershov</creatorcontrib><creatorcontrib>Alexander Ostrovidov</creatorcontrib><creatorcontrib>A.V. Popov</creatorcontrib><creatorcontrib>C. Olchanski</creatorcontrib><creatorcontrib>David Joffe</creatorcontrib><creatorcontrib>D.B. White</creatorcontrib><creatorcontrib>D.I. Ryabchikov</creatorcontrib><creatorcontrib>Doran Stienike</creatorcontrib><creatorcontrib>D.S. Brown</creatorcontrib><creatorcontrib>Dennis Weygand</creatorcontrib><creatorcontrib>E. King</creatorcontrib><creatorcontrib>Gary Adams</creatorcontrib><creatorcontrib>Hans Willutzki</creatorcontrib><creatorcontrib>I.A. Kachaev</creatorcontrib><creatorcontrib>I.N. Vardanian</creatorcontrib><creatorcontrib>J.A. Smith</creatorcontrib><creatorcontrib>James Bishop</creatorcontrib><creatorcontrib>John LoSecco</creatorcontrib><creatorcontrib>John P. Dowd</creatorcontrib><creatorcontrib>James Napolitano</creatorcontrib><creatorcontrib>Joachim Kuhn</creatorcontrib><creatorcontrib>Joseph Manak</creatorcontrib><creatorcontrib>John Cummings</creatorcontrib><creatorcontrib>K. Danyo</creatorcontrib><creatorcontrib>Kamal Seth</creatorcontrib><creatorcontrib>Ludmilla Sarycheva</creatorcontrib><creatorcontrib>M. Hayek</creatorcontrib><creatorcontrib>M.A. Kostin</creatorcontrib><creatorcontrib>Michael Witkowski</creatorcontrib><creatorcontrib>Mina Nozar</creatorcontrib><creatorcontrib>N. Shenhav</creatorcontrib><creatorcontrib>N.B. Sinev</creatorcontrib><creatorcontrib>Neal Cason</creatorcontrib><creatorcontrib>O.L. Kodolova</creatorcontrib><creatorcontrib>Paul Eugenio</creatorcontrib><creatorcontrib>R.W. Hackenburg</creatorcontrib><creatorcontrib>Sydney Taegar</creatorcontrib><creatorcontrib>Sergey Denisov</creatorcontrib><creatorcontrib>Suh-Urk Chung</creatorcontrib><creatorcontrib>Todd Adams</creatorcontrib><creatorcontrib>Todd Pedlar</creatorcontrib><creatorcontrib>V.A. Bodyagin</creatorcontrib><creatorcontrib>V.A. Dorofeev</creatorcontrib><creatorcontrib>V.L. Korotkikh</creatorcontrib><creatorcontrib>V.V. Lipaev</creatorcontrib><creatorcontrib>W. Kern</creatorcontrib><creatorcontrib>William Shephard</creatorcontrib><creatorcontrib>Xiao Shen</creatorcontrib><creatorcontrib>X.L. Fan</creatorcontrib><creatorcontrib>Thomas Jefferson National Accelerator Facility, Newport News, VA (US)</creatorcontrib><title>Observation of exotic meson production in the reaction {pi}{sup -} p {yields} {eta}{prime} {pi}{sup -} p at 18 GeV/c</title><title>Physical review letters</title><description>An amplitude analysis of an exclusive sample of 5765 events from the reaction {pi}{sup -} p {yields} {eta}{prime}{pi}{sup -} p at 18 GeV/c is described. The {eta}{prime}{pi}{sup -} production is dominated by natural parity exchange and by three partial waves: those with J{sup PC} = 1{sup -+}, 2{sup ++}, and 4{sup ++}. A mass-dependent analysis of the partial-wave amplitudes indicates the production of the a{sub 2}(1320) meson as well as the a{sub 4}(2040) meson, observed for the first time decaying to {eta}{prime}{pi}{sup -}. The dominant, exotic (non-q{bar q}) 1{sup -+} partial wave is shown to be resonant with a mass of 1.597 {+-} 0.010{sub -0.010}{sup +0.045} GeV/c{sup 2} and a width of 0.340 {+-} 0.040 {+-} 0.050 GeV/c{sup 2}. This exotic state, the {pi}{sub 1}(1600), is produced with a t dependence which is different from that of the a{sub 2}(1320) meson, indicating differences between the production mechanisms for the two states.</description><subject>AMPLITUDES</subject><subject>MESONS</subject><subject>PARITY</subject><subject>PARTIAL WAVES</subject><subject>PHYSICS OF ELEMENTARY PARTICLES AND FIELDS</subject><subject>PRODUCTION</subject><issn>0031-9007</issn><issn>1079-7114</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2001</creationdate><recordtype>article</recordtype><recordid>eNqNisFqAjEQQIO04Nb6D9MPWDpxi7t7lmpvXqTXJWZHTNEk7IyihPx7S-3JU0-Px3sjVWis27LW-u1BFYiVLlvEeqyemL8QUc_mTaFkvWUazkZc8BB2QJcgzsKR-MfjEPqT_U3Og-wJBjI3T9HlxKcIZYYI6ero0HOGRGJyioM7Ur57jIBuYEWfr_ZZPe7MgWn6x4l6Wb5vFh9lYHEdWydk9zZ4T1a6pmqxqqv_PN92aU00</recordid><startdate>20010401</startdate><enddate>20010401</enddate><creator>Z. Bar-Yam</creator><creator>Amiran Tomaradze</creator><creator>A.A. 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Fan</creatorcontrib><creatorcontrib>Thomas Jefferson National Accelerator Facility, Newport News, VA (US)</creatorcontrib><collection>OSTI.GOV - Hybrid</collection><collection>OSTI.GOV</collection><jtitle>Physical review letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Z. Bar-Yam</au><au>Amiran Tomaradze</au><au>A.A. Yershov</au><au>Alexander Ostrovidov</au><au>A.V. Popov</au><au>C. Olchanski</au><au>David Joffe</au><au>D.B. White</au><au>D.I. Ryabchikov</au><au>Doran Stienike</au><au>D.S. Brown</au><au>Dennis Weygand</au><au>E. King</au><au>Gary Adams</au><au>Hans Willutzki</au><au>I.A. Kachaev</au><au>I.N. Vardanian</au><au>J.A. Smith</au><au>James Bishop</au><au>John LoSecco</au><au>John P. Dowd</au><au>James Napolitano</au><au>Joachim Kuhn</au><au>Joseph Manak</au><au>John Cummings</au><au>K. Danyo</au><au>Kamal Seth</au><au>Ludmilla Sarycheva</au><au>M. Hayek</au><au>M.A. Kostin</au><au>Michael Witkowski</au><au>Mina Nozar</au><au>N. Shenhav</au><au>N.B. Sinev</au><au>Neal Cason</au><au>O.L. Kodolova</au><au>Paul Eugenio</au><au>R.W. Hackenburg</au><au>Sydney Taegar</au><au>Sergey Denisov</au><au>Suh-Urk Chung</au><au>Todd Adams</au><au>Todd Pedlar</au><au>V.A. Bodyagin</au><au>V.A. Dorofeev</au><au>V.L. Korotkikh</au><au>V.V. Lipaev</au><au>W. Kern</au><au>William Shephard</au><au>Xiao Shen</au><au>X.L. Fan</au><aucorp>Thomas Jefferson National Accelerator Facility, Newport News, VA (US)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Observation of exotic meson production in the reaction {pi}{sup -} p {yields} {eta}{prime} {pi}{sup -} p at 18 GeV/c</atitle><jtitle>Physical review letters</jtitle><date>2001-04-01</date><risdate>2001</risdate><volume>86</volume><issn>0031-9007</issn><eissn>1079-7114</eissn><abstract>An amplitude analysis of an exclusive sample of 5765 events from the reaction {pi}{sup -} p {yields} {eta}{prime}{pi}{sup -} p at 18 GeV/c is described. The {eta}{prime}{pi}{sup -} production is dominated by natural parity exchange and by three partial waves: those with J{sup PC} = 1{sup -+}, 2{sup ++}, and 4{sup ++}. A mass-dependent analysis of the partial-wave amplitudes indicates the production of the a{sub 2}(1320) meson as well as the a{sub 4}(2040) meson, observed for the first time decaying to {eta}{prime}{pi}{sup -}. The dominant, exotic (non-q{bar q}) 1{sup -+} partial wave is shown to be resonant with a mass of 1.597 {+-} 0.010{sub -0.010}{sup +0.045} GeV/c{sup 2} and a width of 0.340 {+-} 0.040 {+-} 0.050 GeV/c{sup 2}. This exotic state, the {pi}{sub 1}(1600), is produced with a t dependence which is different from that of the a{sub 2}(1320) meson, indicating differences between the production mechanisms for the two states.</abstract><cop>United States</cop><oa>free_for_read</oa></addata></record> |
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source | American Physical Society Journals |
subjects | AMPLITUDES MESONS PARITY PARTIAL WAVES PHYSICS OF ELEMENTARY PARTICLES AND FIELDS PRODUCTION |
title | Observation of exotic meson production in the reaction {pi}{sup -} p {yields} {eta}{prime} {pi}{sup -} p at 18 GeV/c |
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