{sup 2}H(e,e'p)n Reaction at High Recoil Momenta
The 2H(e,ep)n cross section was measured in Hall A of the Thomas Jefferson National Accelerator Facility near the top of the quasielastic peak (xBj = 0.964) at a four-momentum transfer squared, Q2 = 0.665 (GeV/c)2 (= 0.368GeV, W = 2.057GeV), and for recoil momenta up to 550MeV/c. The measured cross...
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| Veröffentlicht in: | Physical review letters 2002-08, Vol.89 |
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| creator | P. E. Ulmer K. A. Aniol H. Arenhoevel J.-P. Chen E. Chudakov D. Crovelli J. M. Finn K. G. Fissum O. Gayou J. Gomez J.-O. Hansen C. W. de Jager S. Jeschonnek M. K. Jones M. Kuss J. J. LeRose M. Liang R. A. Lindgren S. Malov D. Meekins R. Michaels J. Mitchell C. F. Perdrisat V. Punjabi R. Roche F. Sabatie A. Saha R. Suleiman L. Todor B. B. Wojtsekhowski |
| description | The 2H(e,ep)n cross section was measured in Hall A of the Thomas Jefferson National Accelerator Facility near the top of the quasielastic peak (xBj = 0.964) at a four-momentum transfer squared, Q2 = 0.665 (GeV/c)2 (= 0.368GeV, W = 2.057GeV), and for recoil momenta up to 550MeV/c. The measured cross section deviates by 1-2 from a state-of-the-art calculation at low recoil momenta. At high recoil momenta the cross section is well described by the same calculation; however, in this region, final-state interactions and interaction currents are predicted to be large, and alternative choices of nucleon-nucleon potential and nucleon current operator may result in significant spread in the calculations. |
| doi_str_mv | 10.1103/PhysRevLett.89.062301 |
| format | Article |
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Chudakov ; D. Crovelli ; J. M. Finn ; K. G. Fissum ; O. Gayou ; J. Gomez ; J.-O. Hansen ; C. W. de Jager ; S. Jeschonnek ; M. K. Jones ; M. Kuss ; J. J. LeRose ; M. Liang ; R. A. Lindgren ; S. Malov ; D. Meekins ; R. Michaels ; J. Mitchell ; C. F. Perdrisat ; V. Punjabi ; R. Roche ; F. Sabatie ; A. Saha ; R. Suleiman ; L. Todor ; B. B. Wojtsekhowski</creator><creatorcontrib>P. E. Ulmer ; K. A. Aniol ; H. Arenhoevel ; J.-P. Chen ; E. Chudakov ; D. Crovelli ; J. M. Finn ; K. G. Fissum ; O. Gayou ; J. Gomez ; J.-O. Hansen ; C. W. de Jager ; S. Jeschonnek ; M. K. Jones ; M. Kuss ; J. J. LeRose ; M. Liang ; R. A. Lindgren ; S. Malov ; D. Meekins ; R. Michaels ; J. Mitchell ; C. F. Perdrisat ; V. Punjabi ; R. Roche ; F. Sabatie ; A. Saha ; R. Suleiman ; L. Todor ; B. B. Wojtsekhowski ; Thomas Jefferson National Accelerator Facility, Newport News, VA (US)</creatorcontrib><description>The 2H(e,ep)n cross section was measured in Hall A of the Thomas Jefferson National Accelerator Facility near the top of the quasielastic peak (xBj = 0.964) at a four-momentum transfer squared, Q2 = 0.665 (GeV/c)2 (= 0.368GeV, W = 2.057GeV), and for recoil momenta up to 550MeV/c. The measured cross section deviates by 1-2 from a state-of-the-art calculation at low recoil momenta. At high recoil momenta the cross section is well described by the same calculation; however, in this region, final-state interactions and interaction currents are predicted to be large, and alternative choices of nucleon-nucleon potential and nucleon current operator may result in significant spread in the calculations.</description><identifier>ISSN: 0031-9007</identifier><identifier>EISSN: 1079-7114</identifier><identifier>DOI: 10.1103/PhysRevLett.89.062301</identifier><language>eng</language><publisher>United States</publisher><subject>CEBAF ACCELERATOR ; CROSS SECTIONS ; FINAL-STATE INTERACTIONS ; NUCLEON-NUCLEON POTENTIAL ; NUCLEONS ; PARTICLE ACCELERATORS</subject><ispartof>Physical review letters, 2002-08, Vol.89</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,780,784,885,27924,27925</link.rule.ids><backlink>$$Uhttps://www.osti.gov/biblio/801039$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>P. E. Ulmer</creatorcontrib><creatorcontrib>K. A. Aniol</creatorcontrib><creatorcontrib>H. Arenhoevel</creatorcontrib><creatorcontrib>J.-P. Chen</creatorcontrib><creatorcontrib>E. Chudakov</creatorcontrib><creatorcontrib>D. Crovelli</creatorcontrib><creatorcontrib>J. M. Finn</creatorcontrib><creatorcontrib>K. G. Fissum</creatorcontrib><creatorcontrib>O. Gayou</creatorcontrib><creatorcontrib>J. Gomez</creatorcontrib><creatorcontrib>J.-O. Hansen</creatorcontrib><creatorcontrib>C. W. de Jager</creatorcontrib><creatorcontrib>S. Jeschonnek</creatorcontrib><creatorcontrib>M. K. Jones</creatorcontrib><creatorcontrib>M. Kuss</creatorcontrib><creatorcontrib>J. J. LeRose</creatorcontrib><creatorcontrib>M. Liang</creatorcontrib><creatorcontrib>R. A. Lindgren</creatorcontrib><creatorcontrib>S. Malov</creatorcontrib><creatorcontrib>D. Meekins</creatorcontrib><creatorcontrib>R. Michaels</creatorcontrib><creatorcontrib>J. Mitchell</creatorcontrib><creatorcontrib>C. F. 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At high recoil momenta the cross section is well described by the same calculation; however, in this region, final-state interactions and interaction currents are predicted to be large, and alternative choices of nucleon-nucleon potential and nucleon current operator may result in significant spread in the calculations.</description><subject>CEBAF ACCELERATOR</subject><subject>CROSS SECTIONS</subject><subject>FINAL-STATE INTERACTIONS</subject><subject>NUCLEON-NUCLEON POTENTIAL</subject><subject>NUCLEONS</subject><subject>PARTICLE ACCELERATORS</subject><issn>0031-9007</issn><issn>1079-7114</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2002</creationdate><recordtype>article</recordtype><recordid>eNotj8FKxDAURYMoWEc_QagrFWx9L0mbZCmDWqGiDLMf0uRpK2MykCiI-O8WdHXhLM7hMnaKUCOCuH4ev9KKPnvKudamhpYLwD1WIChTKUS5zwoAgZUBUIfsKKU3AEDe6oLBd_rYlfynu6ArOt9dhnJF1uUphtLmsptexxm4OG3Lx_hOIdtjdvBit4lO_nfB1ne362VX9U_3D8ubvopG5opb633bcOMGh42UoGmOE_jGKe-cl0iDNgMKzVGiGlrFOaEmQAXWE4kFO_vTxpSnTXJTJje6GAK5vNEw3zbiF7C9Rko</recordid><startdate>20020805</startdate><enddate>20020805</enddate><creator>P. 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Wojtsekhowski</creator><scope>OTOTI</scope></search><sort><creationdate>20020805</creationdate><title>{sup 2}H(e,e'p)n Reaction at High Recoil Momenta</title><author>P. E. Ulmer ; K. A. Aniol ; H. Arenhoevel ; J.-P. Chen ; E. Chudakov ; D. Crovelli ; J. M. Finn ; K. G. Fissum ; O. Gayou ; J. Gomez ; J.-O. Hansen ; C. W. de Jager ; S. Jeschonnek ; M. K. Jones ; M. Kuss ; J. J. LeRose ; M. Liang ; R. A. Lindgren ; S. Malov ; D. Meekins ; R. Michaels ; J. Mitchell ; C. F. Perdrisat ; V. Punjabi ; R. Roche ; F. Sabatie ; A. Saha ; R. Suleiman ; L. Todor ; B. B. 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Wojtsekhowski</creatorcontrib><creatorcontrib>Thomas Jefferson National Accelerator Facility, Newport News, VA (US)</creatorcontrib><collection>OSTI.GOV</collection><jtitle>Physical review letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>P. E. Ulmer</au><au>K. A. Aniol</au><au>H. Arenhoevel</au><au>J.-P. Chen</au><au>E. Chudakov</au><au>D. Crovelli</au><au>J. M. Finn</au><au>K. G. Fissum</au><au>O. Gayou</au><au>J. Gomez</au><au>J.-O. Hansen</au><au>C. W. de Jager</au><au>S. Jeschonnek</au><au>M. K. Jones</au><au>M. Kuss</au><au>J. J. LeRose</au><au>M. Liang</au><au>R. A. Lindgren</au><au>S. Malov</au><au>D. Meekins</au><au>R. Michaels</au><au>J. Mitchell</au><au>C. F. Perdrisat</au><au>V. Punjabi</au><au>R. Roche</au><au>F. Sabatie</au><au>A. Saha</au><au>R. Suleiman</au><au>L. Todor</au><au>B. B. 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At high recoil momenta the cross section is well described by the same calculation; however, in this region, final-state interactions and interaction currents are predicted to be large, and alternative choices of nucleon-nucleon potential and nucleon current operator may result in significant spread in the calculations.</abstract><cop>United States</cop><doi>10.1103/PhysRevLett.89.062301</doi></addata></record> |
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| ispartof | Physical review letters, 2002-08, Vol.89 |
| issn | 0031-9007 1079-7114 |
| language | eng |
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| source | American Physical Society Journals |
| subjects | CEBAF ACCELERATOR CROSS SECTIONS FINAL-STATE INTERACTIONS NUCLEON-NUCLEON POTENTIAL NUCLEONS PARTICLE ACCELERATORS |
| title | {sup 2}H(e,e'p)n Reaction at High Recoil Momenta |
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