Nuclear Transparency in Large Momentum Transfer Quasielastic Scattering
We measured simultaneously pp elastic and quasielastic (p,2p) scattering in hydrogen, deuterium, and carbon for momentum transfers of 4.8 to 6.2 (GeV/c)2 at incoming momenta of 5.9 and 7.5 GeV/c and center-of-mass scattering angles in the range θc.m.=83.7°–90°. The nuclear transparency is defined as...
Ausführliche Beschreibung
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E-Artikel |
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| Erschienen: |
1998 |
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Online-Ressource 4 |
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APS Digital Backfile Archive 1893-2003 |
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| Übergeordnetes Werk: |
Enthalten in: Physical review letters - College Park, Md. : APS, 1958, 81(1998), 23, Seite 5085-5088 |
| Übergeordnetes Werk: |
volume:81 ; year:1998 ; number:23 ; pages:5085-5088 ; extent:4 |
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NLEJ250715147 |
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| 520 | |a We measured simultaneously pp elastic and quasielastic (p,2p) scattering in hydrogen, deuterium, and carbon for momentum transfers of 4.8 to 6.2 (GeV/c)2 at incoming momenta of 5.9 and 7.5 GeV/c and center-of-mass scattering angles in the range θc.m.=83.7°–90°. The nuclear transparency is defined as the ratio of the quasielastic cross section to the free pp cross section. At incoming momentum of 5.9 GeV/c, the transparency of carbon decreases by a factor of 2 from θc.m.≃85° to θc.m.≃89°. At the largest angle the transparency of carbon increases from 5.9 to 7.5 GeV/c by more than 50%. The transparency in deuterium does not depend on incoming momentum nor on θc.m.. | ||
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| 700 | 1 | |a Mardor, I. |4 oth | |
| 700 | 1 | |a Durrant, S. |4 oth | |
| 700 | 1 | |a Aclander, J. |4 oth | |
| 700 | 1 | |a Alster, J. |4 oth | |
| 700 | 1 | |a Barton, D. |4 oth | |
| 700 | 1 | |a Bunce, G. |4 oth | |
| 700 | 1 | |a Carroll, A. |4 oth | |
| 700 | 1 | |a Christensen, N. |4 oth | |
| 700 | 1 | |a Courant, H. |4 oth | |
| 700 | 1 | |a Gushue, S. |4 oth | |
| 700 | 1 | |a Heppelmann, S. |4 oth | |
| 700 | 1 | |a Kosonovsky, E. |4 oth | |
| 700 | 1 | |a Mardor, Y. |4 oth | |
| 700 | 1 | |a Marshak, M. |4 oth | |
| 700 | 1 | |a Makdisi, Y. |4 oth | |
| 700 | 1 | |a Minor, E. D. |4 oth | |
| 700 | 1 | |a Navon, I. |4 oth | |
| 700 | 1 | |a Nicholson, H. |4 oth | |
| 700 | 1 | |a Piasetzky, E. |4 oth | |
| 700 | 1 | |a Roser, T. |4 oth | |
| 700 | 1 | |a Russell, J. |4 oth | |
| 700 | 1 | |a Sutton, C. S. |4 oth | |
| 700 | 1 | |a Tanaka, M. |4 oth | |
| 700 | 1 | |a White, C. |4 oth | |
| 700 | 1 | |a Wu, J.-Y. |4 oth | |
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(DE-627)NLEJ250715147 (DE-601)aps:74f7c5e4127d32d5f6ba98536e7aadcea8df9885 DE-627 ger DE-627 rakwb Nuclear Transparency in Large Momentum Transfer Quasielastic Scattering 1998 Online-Ressource 4 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We measured simultaneously pp elastic and quasielastic (p,2p) scattering in hydrogen, deuterium, and carbon for momentum transfers of 4.8 to 6.2 (GeV/c)2 at incoming momenta of 5.9 and 7.5 GeV/c and center-of-mass scattering angles in the range θc.m.=83.7°–90°. The nuclear transparency is defined as the ratio of the quasielastic cross section to the free pp cross section. At incoming momentum of 5.9 GeV/c, the transparency of carbon decreases by a factor of 2 from θc.m.≃85° to θc.m.≃89°. At the largest angle the transparency of carbon increases from 5.9 to 7.5 GeV/c by more than 50%. The transparency in deuterium does not depend on incoming momentum nor on θc.m.. APS Digital Backfile Archive 1893-2003 Mardor, I. oth Durrant, S. oth Aclander, J. oth Alster, J. oth Barton, D. oth Bunce, G. oth Carroll, A. oth Christensen, N. oth Courant, H. oth Gushue, S. oth Heppelmann, S. oth Kosonovsky, E. oth Mardor, Y. oth Marshak, M. oth Makdisi, Y. oth Minor, E. D. oth Navon, I. oth Nicholson, H. oth Piasetzky, E. oth Roser, T. oth Russell, J. oth Sutton, C. S. oth Tanaka, M. oth White, C. oth Wu, J.-Y. oth Enthalten in Physical review letters College Park, Md. : APS, 1958 81(1998), 23, Seite 5085-5088 Online-Ressource (DE-627)NLEJ248237888 (DE-600)1472655-5 1079-7114 nnns volume:81 year:1998 number:23 pages:5085-5088 extent:4 https://www.tib.eu/de/suchen/id/aps%3A74f7c5e4127d32d5f6ba98536e7aadcea8df9885 Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 81 1998 23 5085-5088 4 |
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(DE-627)NLEJ250715147 (DE-601)aps:74f7c5e4127d32d5f6ba98536e7aadcea8df9885 DE-627 ger DE-627 rakwb Nuclear Transparency in Large Momentum Transfer Quasielastic Scattering 1998 Online-Ressource 4 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We measured simultaneously pp elastic and quasielastic (p,2p) scattering in hydrogen, deuterium, and carbon for momentum transfers of 4.8 to 6.2 (GeV/c)2 at incoming momenta of 5.9 and 7.5 GeV/c and center-of-mass scattering angles in the range θc.m.=83.7°–90°. The nuclear transparency is defined as the ratio of the quasielastic cross section to the free pp cross section. At incoming momentum of 5.9 GeV/c, the transparency of carbon decreases by a factor of 2 from θc.m.≃85° to θc.m.≃89°. At the largest angle the transparency of carbon increases from 5.9 to 7.5 GeV/c by more than 50%. The transparency in deuterium does not depend on incoming momentum nor on θc.m.. APS Digital Backfile Archive 1893-2003 Mardor, I. oth Durrant, S. oth Aclander, J. oth Alster, J. oth Barton, D. oth Bunce, G. oth Carroll, A. oth Christensen, N. oth Courant, H. oth Gushue, S. oth Heppelmann, S. oth Kosonovsky, E. oth Mardor, Y. oth Marshak, M. oth Makdisi, Y. oth Minor, E. D. oth Navon, I. oth Nicholson, H. oth Piasetzky, E. oth Roser, T. oth Russell, J. oth Sutton, C. S. oth Tanaka, M. oth White, C. oth Wu, J.-Y. oth Enthalten in Physical review letters College Park, Md. : APS, 1958 81(1998), 23, Seite 5085-5088 Online-Ressource (DE-627)NLEJ248237888 (DE-600)1472655-5 1079-7114 nnns volume:81 year:1998 number:23 pages:5085-5088 extent:4 https://www.tib.eu/de/suchen/id/aps%3A74f7c5e4127d32d5f6ba98536e7aadcea8df9885 Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 81 1998 23 5085-5088 4 |
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(DE-627)NLEJ250715147 (DE-601)aps:74f7c5e4127d32d5f6ba98536e7aadcea8df9885 DE-627 ger DE-627 rakwb Nuclear Transparency in Large Momentum Transfer Quasielastic Scattering 1998 Online-Ressource 4 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We measured simultaneously pp elastic and quasielastic (p,2p) scattering in hydrogen, deuterium, and carbon for momentum transfers of 4.8 to 6.2 (GeV/c)2 at incoming momenta of 5.9 and 7.5 GeV/c and center-of-mass scattering angles in the range θc.m.=83.7°–90°. The nuclear transparency is defined as the ratio of the quasielastic cross section to the free pp cross section. At incoming momentum of 5.9 GeV/c, the transparency of carbon decreases by a factor of 2 from θc.m.≃85° to θc.m.≃89°. At the largest angle the transparency of carbon increases from 5.9 to 7.5 GeV/c by more than 50%. The transparency in deuterium does not depend on incoming momentum nor on θc.m.. APS Digital Backfile Archive 1893-2003 Mardor, I. oth Durrant, S. oth Aclander, J. oth Alster, J. oth Barton, D. oth Bunce, G. oth Carroll, A. oth Christensen, N. oth Courant, H. oth Gushue, S. oth Heppelmann, S. oth Kosonovsky, E. oth Mardor, Y. oth Marshak, M. oth Makdisi, Y. oth Minor, E. D. oth Navon, I. oth Nicholson, H. oth Piasetzky, E. oth Roser, T. oth Russell, J. oth Sutton, C. S. oth Tanaka, M. oth White, C. oth Wu, J.-Y. oth Enthalten in Physical review letters College Park, Md. : APS, 1958 81(1998), 23, Seite 5085-5088 Online-Ressource (DE-627)NLEJ248237888 (DE-600)1472655-5 1079-7114 nnns volume:81 year:1998 number:23 pages:5085-5088 extent:4 https://www.tib.eu/de/suchen/id/aps%3A74f7c5e4127d32d5f6ba98536e7aadcea8df9885 Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 81 1998 23 5085-5088 4 |
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(DE-627)NLEJ250715147 (DE-601)aps:74f7c5e4127d32d5f6ba98536e7aadcea8df9885 DE-627 ger DE-627 rakwb Nuclear Transparency in Large Momentum Transfer Quasielastic Scattering 1998 Online-Ressource 4 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We measured simultaneously pp elastic and quasielastic (p,2p) scattering in hydrogen, deuterium, and carbon for momentum transfers of 4.8 to 6.2 (GeV/c)2 at incoming momenta of 5.9 and 7.5 GeV/c and center-of-mass scattering angles in the range θc.m.=83.7°–90°. The nuclear transparency is defined as the ratio of the quasielastic cross section to the free pp cross section. At incoming momentum of 5.9 GeV/c, the transparency of carbon decreases by a factor of 2 from θc.m.≃85° to θc.m.≃89°. At the largest angle the transparency of carbon increases from 5.9 to 7.5 GeV/c by more than 50%. The transparency in deuterium does not depend on incoming momentum nor on θc.m.. APS Digital Backfile Archive 1893-2003 Mardor, I. oth Durrant, S. oth Aclander, J. oth Alster, J. oth Barton, D. oth Bunce, G. oth Carroll, A. oth Christensen, N. oth Courant, H. oth Gushue, S. oth Heppelmann, S. oth Kosonovsky, E. oth Mardor, Y. oth Marshak, M. oth Makdisi, Y. oth Minor, E. D. oth Navon, I. oth Nicholson, H. oth Piasetzky, E. oth Roser, T. oth Russell, J. oth Sutton, C. S. oth Tanaka, M. oth White, C. oth Wu, J.-Y. oth Enthalten in Physical review letters College Park, Md. : APS, 1958 81(1998), 23, Seite 5085-5088 Online-Ressource (DE-627)NLEJ248237888 (DE-600)1472655-5 1079-7114 nnns volume:81 year:1998 number:23 pages:5085-5088 extent:4 https://www.tib.eu/de/suchen/id/aps%3A74f7c5e4127d32d5f6ba98536e7aadcea8df9885 Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 81 1998 23 5085-5088 4 |
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(DE-627)NLEJ250715147 (DE-601)aps:74f7c5e4127d32d5f6ba98536e7aadcea8df9885 DE-627 ger DE-627 rakwb Nuclear Transparency in Large Momentum Transfer Quasielastic Scattering 1998 Online-Ressource 4 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier We measured simultaneously pp elastic and quasielastic (p,2p) scattering in hydrogen, deuterium, and carbon for momentum transfers of 4.8 to 6.2 (GeV/c)2 at incoming momenta of 5.9 and 7.5 GeV/c and center-of-mass scattering angles in the range θc.m.=83.7°–90°. The nuclear transparency is defined as the ratio of the quasielastic cross section to the free pp cross section. At incoming momentum of 5.9 GeV/c, the transparency of carbon decreases by a factor of 2 from θc.m.≃85° to θc.m.≃89°. At the largest angle the transparency of carbon increases from 5.9 to 7.5 GeV/c by more than 50%. The transparency in deuterium does not depend on incoming momentum nor on θc.m.. APS Digital Backfile Archive 1893-2003 Mardor, I. oth Durrant, S. oth Aclander, J. oth Alster, J. oth Barton, D. oth Bunce, G. oth Carroll, A. oth Christensen, N. oth Courant, H. oth Gushue, S. oth Heppelmann, S. oth Kosonovsky, E. oth Mardor, Y. oth Marshak, M. oth Makdisi, Y. oth Minor, E. D. oth Navon, I. oth Nicholson, H. oth Piasetzky, E. oth Roser, T. oth Russell, J. oth Sutton, C. S. oth Tanaka, M. oth White, C. oth Wu, J.-Y. oth Enthalten in Physical review letters College Park, Md. : APS, 1958 81(1998), 23, Seite 5085-5088 Online-Ressource (DE-627)NLEJ248237888 (DE-600)1472655-5 1079-7114 nnns volume:81 year:1998 number:23 pages:5085-5088 extent:4 https://www.tib.eu/de/suchen/id/aps%3A74f7c5e4127d32d5f6ba98536e7aadcea8df9885 Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 81 1998 23 5085-5088 4 |
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Mardor, I. @@oth@@ Durrant, S. @@oth@@ Aclander, J. @@oth@@ Alster, J. @@oth@@ Barton, D. @@oth@@ Bunce, G. @@oth@@ Carroll, A. @@oth@@ Christensen, N. @@oth@@ Courant, H. @@oth@@ Gushue, S. @@oth@@ Heppelmann, S. @@oth@@ Kosonovsky, E. @@oth@@ Mardor, Y. @@oth@@ Marshak, M. @@oth@@ Makdisi, Y. @@oth@@ Minor, E. D. @@oth@@ Navon, I. @@oth@@ Nicholson, H. @@oth@@ Piasetzky, E. @@oth@@ Roser, T. @@oth@@ Russell, J. @@oth@@ Sutton, C. S. @@oth@@ Tanaka, M. @@oth@@ White, C. @@oth@@ Wu, J.-Y. @@oth@@ |
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Nuclear Transparency in Large Momentum Transfer Quasielastic Scattering |
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Nuclear Transparency in Large Momentum Transfer Quasielastic Scattering |
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Nuclear Transparency in Large Momentum Transfer Quasielastic Scattering |
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nuclear transparency in large momentum transfer quasielastic scattering |
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Nuclear Transparency in Large Momentum Transfer Quasielastic Scattering |
| abstract |
We measured simultaneously pp elastic and quasielastic (p,2p) scattering in hydrogen, deuterium, and carbon for momentum transfers of 4.8 to 6.2 (GeV/c)2 at incoming momenta of 5.9 and 7.5 GeV/c and center-of-mass scattering angles in the range θc.m.=83.7°–90°. The nuclear transparency is defined as the ratio of the quasielastic cross section to the free pp cross section. At incoming momentum of 5.9 GeV/c, the transparency of carbon decreases by a factor of 2 from θc.m.≃85° to θc.m.≃89°. At the largest angle the transparency of carbon increases from 5.9 to 7.5 GeV/c by more than 50%. The transparency in deuterium does not depend on incoming momentum nor on θc.m.. |
| abstractGer |
We measured simultaneously pp elastic and quasielastic (p,2p) scattering in hydrogen, deuterium, and carbon for momentum transfers of 4.8 to 6.2 (GeV/c)2 at incoming momenta of 5.9 and 7.5 GeV/c and center-of-mass scattering angles in the range θc.m.=83.7°–90°. The nuclear transparency is defined as the ratio of the quasielastic cross section to the free pp cross section. At incoming momentum of 5.9 GeV/c, the transparency of carbon decreases by a factor of 2 from θc.m.≃85° to θc.m.≃89°. At the largest angle the transparency of carbon increases from 5.9 to 7.5 GeV/c by more than 50%. The transparency in deuterium does not depend on incoming momentum nor on θc.m.. |
| abstract_unstemmed |
We measured simultaneously pp elastic and quasielastic (p,2p) scattering in hydrogen, deuterium, and carbon for momentum transfers of 4.8 to 6.2 (GeV/c)2 at incoming momenta of 5.9 and 7.5 GeV/c and center-of-mass scattering angles in the range θc.m.=83.7°–90°. The nuclear transparency is defined as the ratio of the quasielastic cross section to the free pp cross section. At incoming momentum of 5.9 GeV/c, the transparency of carbon decreases by a factor of 2 from θc.m.≃85° to θc.m.≃89°. At the largest angle the transparency of carbon increases from 5.9 to 7.5 GeV/c by more than 50%. The transparency in deuterium does not depend on incoming momentum nor on θc.m.. |
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Nuclear Transparency in Large Momentum Transfer Quasielastic Scattering |
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Mardor, I. Durrant, S. Aclander, J. Alster, J. Barton, D. Bunce, G. Carroll, A. Christensen, N. Courant, H. Gushue, S. Heppelmann, S. Kosonovsky, E. Mardor, Y. Marshak, M. Makdisi, Y. Minor, E. D. Navon, I. Nicholson, H. Piasetzky, E. Roser, T. Russell, J. Sutton, C. S. Tanaka, M. White, C. Wu, J.-Y. |
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Mardor, I. Durrant, S. Aclander, J. Alster, J. Barton, D. Bunce, G. Carroll, A. Christensen, N. Courant, H. Gushue, S. Heppelmann, S. Kosonovsky, E. Mardor, Y. Marshak, M. Makdisi, Y. Minor, E. D. Navon, I. Nicholson, H. Piasetzky, E. Roser, T. Russell, J. Sutton, C. S. Tanaka, M. White, C. Wu, J.-Y. |
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