Ratios of helicity amplitudes for exclusive ρ0 electroproduction
Abstract Exclusive ρ0-meson electroproduction is studied in the HERMES experiment, using a 27.6 GeV longitudinally polarized electron/positron beam and unpolarized hydrogen and deuterium targets in the kinematic region 0.5 $ GeV^{2} $<Q2<7.0 $ GeV^{2} $, 3.0 GeV <W<6.3 GeV, and −t′<0....
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Airapetian, A. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2011 |
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| Schlagwörter: |
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| Anmerkung: |
© The Author(s) 2011 |
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| Übergeordnetes Werk: |
Enthalten in: The European physical journal - Berlin : Springer, 1998, 71(2011), 4 vom: Apr. |
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| Übergeordnetes Werk: |
volume:71 ; year:2011 ; number:4 ; month:04 |
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| DOI / URN: |
10.1140/epjc/s10052-011-1609-2 |
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| Katalog-ID: |
SPR008325030 |
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| 035 | |a (SPR)s10052-011-1609-2-e | ||
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| 041 | |a eng | ||
| 100 | 1 | |a Airapetian, A. |e verfasserin |4 aut | |
| 245 | 1 | 0 | |a Ratios of helicity amplitudes for exclusive ρ0 electroproduction |
| 264 | 1 | |c 2011 | |
| 336 | |a Text |b txt |2 rdacontent | ||
| 337 | |a Computermedien |b c |2 rdamedia | ||
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| 500 | |a © The Author(s) 2011 | ||
| 520 | |a Abstract Exclusive ρ0-meson electroproduction is studied in the HERMES experiment, using a 27.6 GeV longitudinally polarized electron/positron beam and unpolarized hydrogen and deuterium targets in the kinematic region 0.5 $ GeV^{2} $<Q2<7.0 $ GeV^{2} $, 3.0 GeV <W<6.3 GeV, and −t′<0.4 $ GeV^{2} $. Real and imaginary parts of the ratios of the natural-parity-exchange helicity amplitudes T11 ($\gamma^{*}_{T} \rightarrow\rho_{T}$), T01 ($\gamma^{*}_{T} \rightarrow \rho_{L}$), T10 ($\gamma^{*}_{L} \rightarrow\rho_{T}$), and T1−1 ($\gamma^{*}_{-T} \rightarrow\rho_{T}$) to T00 ($\gamma^{*}_{L}\rightarrow\rho_{L}$) are extracted from the data. For the unnatural-parity-exchange amplitude U11, the ratio |U11/T00| is obtained. The Q2 and t′ dependences of these ratios are presented and compared with perturbative QCD predictions. | ||
| 650 | 4 | |a Systematic Uncertainty |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Amplitude Ratio |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Total Uncertainty |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Helicity Amplitude |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a ZEUS Collaboration |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Akopov, N. |4 aut | |
| 700 | 1 | |a Akopov, Z. |4 aut | |
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| 700 | 1 | |a Augustyniak, W. |4 aut | |
| 700 | 1 | |a Avakian, R. |4 aut | |
| 700 | 1 | |a Avetissian, A. |4 aut | |
| 700 | 1 | |a Avetisyan, E. |4 aut | |
| 700 | 1 | |a Belostotski, S. |4 aut | |
| 700 | 1 | |a Bianchi, N. |4 aut | |
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| 700 | 1 | |a Borissov, A. |4 aut | |
| 700 | 1 | |a Bowles, J. |4 aut | |
| 700 | 1 | |a Bryzgalov, V. |4 aut | |
| 700 | 1 | |a Burns, J. |4 aut | |
| 700 | 1 | |a Capiluppi, M. |4 aut | |
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| 700 | 1 | |a Cisbani, E. |4 aut | |
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| 700 | 1 | |a Diefenthaler, M. |4 aut | |
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10.1140/epjc/s10052-011-1609-2 doi (DE-627)SPR008325030 (SPR)s10052-011-1609-2-e DE-627 ger DE-627 rakwb eng Airapetian, A. verfasserin aut Ratios of helicity amplitudes for exclusive ρ0 electroproduction 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2011 Abstract Exclusive ρ0-meson electroproduction is studied in the HERMES experiment, using a 27.6 GeV longitudinally polarized electron/positron beam and unpolarized hydrogen and deuterium targets in the kinematic region 0.5 $ GeV^{2} $<Q2<7.0 $ GeV^{2} $, 3.0 GeV <W<6.3 GeV, and −t′<0.4 $ GeV^{2} $. Real and imaginary parts of the ratios of the natural-parity-exchange helicity amplitudes T11 ($\gamma^{*}_{T} \rightarrow\rho_{T}$), T01 ($\gamma^{*}_{T} \rightarrow \rho_{L}$), T10 ($\gamma^{*}_{L} \rightarrow\rho_{T}$), and T1−1 ($\gamma^{*}_{-T} \rightarrow\rho_{T}$) to T00 ($\gamma^{*}_{L}\rightarrow\rho_{L}$) are extracted from the data. For the unnatural-parity-exchange amplitude U11, the ratio |U11/T00| is obtained. The Q2 and t′ dependences of these ratios are presented and compared with perturbative QCD predictions. Systematic Uncertainty (dpeaa)DE-He213 Amplitude Ratio (dpeaa)DE-He213 Total Uncertainty (dpeaa)DE-He213 Helicity Amplitude (dpeaa)DE-He213 ZEUS Collaboration (dpeaa)DE-He213 Akopov, N. aut Akopov, Z. aut Aschenauer, E. C. aut Augustyniak, W. aut Avakian, R. aut Avetissian, A. aut Avetisyan, E. aut Belostotski, S. aut Bianchi, N. aut Blok, H. P. aut Borissov, A. aut Bowles, J. aut Bryzgalov, V. aut Burns, J. aut Capiluppi, M. aut Capitani, G. P. aut Cisbani, E. aut Ciullo, G. aut Contalbrigo, M. aut Dalpiaz, P. F. aut Deconinck, W. aut De Leo, R. aut De Nardo, L. aut De Sanctis, E. aut Diefenthaler, M. aut Di Nezza, P. aut Düren, M. aut Ehrenfried, M. aut Elbakian, G. aut Ellinghaus, F. aut Fabbri, R. aut Fantoni, A. aut Felawka, L. aut Frullani, S. aut Gabbert, D. aut Gapienko, G. aut Gapienko, V. aut Garibaldi, F. aut Gavrilov, G. aut Gharibyan, V. aut Giordano, F. aut Gliske, S. aut Golembiovskaya, M. aut Hadjidakis, C. aut Hartig, M. aut Hasch, D. aut Hill, G. aut Hillenbrand, A. aut Hoek, M. aut Holler, Y. aut Hristova, I. aut Imazu, Y. aut Ivanilov, A. aut Jackson, H. E. aut Jo, H. S. aut Joosten, S. aut Kaiser, R. aut Karyan, G. aut Keri, T. aut Kinney, E. aut Kisselev, A. aut Kobayashi, N. aut Korotkov, V. aut Kozlov, V. aut Kravchenko, P. aut Krivokhijine, V. G. aut Lagamba, L. aut Lamb, R. aut Lapikás, L. aut Lehmann, I. aut Lenisa, P. aut Linden-Levy, L. A. aut López Ruiz, A. aut Lorenzon, W. aut Lu, X.-G. aut Lu, X.-R. aut Ma, B.-Q. aut Mahon, D. aut Makins, N. C. R. aut Manaenkov, S. I. aut Manfré, L. aut Mao, Y. aut Marianski, B. aut Martinez de la Ossa, A. aut Marukyan, H. aut Miller, C. A. aut Miyachi, Y. aut Movsisyan, A. aut Muccifora, V. aut Murray, M. aut Mussgiller, A. aut Nappi, E. aut Naryshkin, Y. aut Nass, A. aut Negodaev, M. aut Nowak, W.-D. aut Pappalardo, L. L. aut Perez-Benito, R. aut Pickert, N. aut Reimer, P. E. aut Reolon, A. R. aut Riedl, C. aut Rith, K. aut Rosner, G. aut Rostomyan, A. aut Rubin, J. aut Ryckbosch, D. aut Salomatin, Y. aut Sanftl, F. aut Schäfer, A. aut Schnell, G. aut Schüler, K. P. aut Seitz, B. aut Shibata, T.-A. aut Shutov, V. aut Stancari, M. aut Statera, M. aut Steffens, E. aut Steijger, J. J. M. aut Stinzing, F. aut Taroian, S. aut Terkulov, A. aut Trzcinski, A. aut Tytgat, M. aut Vandenbroucke, A. aut Van Haarlem, Y. aut Van Hulse, C. aut Veretennikov, D. aut Vikhrov, V. aut Vilardi, I. aut Wang, S. aut Yaschenko, S. aut Yen, S. aut Yu, W. aut Zihlmann, B. aut Zupranski, P. aut Enthalten in The European physical journal Berlin : Springer, 1998 71(2011), 4 vom: Apr. (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:71 year:2011 number:4 month:04 https://dx.doi.org/10.1140/epjc/s10052-011-1609-2 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_63 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_206 GBV_ILN_267 GBV_ILN_293 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2068 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_4012 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4305 GBV_ILN_4307 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4338 AR 71 2011 4 04 |
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10.1140/epjc/s10052-011-1609-2 doi (DE-627)SPR008325030 (SPR)s10052-011-1609-2-e DE-627 ger DE-627 rakwb eng Airapetian, A. verfasserin aut Ratios of helicity amplitudes for exclusive ρ0 electroproduction 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2011 Abstract Exclusive ρ0-meson electroproduction is studied in the HERMES experiment, using a 27.6 GeV longitudinally polarized electron/positron beam and unpolarized hydrogen and deuterium targets in the kinematic region 0.5 $ GeV^{2} $<Q2<7.0 $ GeV^{2} $, 3.0 GeV <W<6.3 GeV, and −t′<0.4 $ GeV^{2} $. Real and imaginary parts of the ratios of the natural-parity-exchange helicity amplitudes T11 ($\gamma^{*}_{T} \rightarrow\rho_{T}$), T01 ($\gamma^{*}_{T} \rightarrow \rho_{L}$), T10 ($\gamma^{*}_{L} \rightarrow\rho_{T}$), and T1−1 ($\gamma^{*}_{-T} \rightarrow\rho_{T}$) to T00 ($\gamma^{*}_{L}\rightarrow\rho_{L}$) are extracted from the data. For the unnatural-parity-exchange amplitude U11, the ratio |U11/T00| is obtained. The Q2 and t′ dependences of these ratios are presented and compared with perturbative QCD predictions. Systematic Uncertainty (dpeaa)DE-He213 Amplitude Ratio (dpeaa)DE-He213 Total Uncertainty (dpeaa)DE-He213 Helicity Amplitude (dpeaa)DE-He213 ZEUS Collaboration (dpeaa)DE-He213 Akopov, N. aut Akopov, Z. aut Aschenauer, E. C. aut Augustyniak, W. aut Avakian, R. aut Avetissian, A. aut Avetisyan, E. aut Belostotski, S. aut Bianchi, N. aut Blok, H. P. aut Borissov, A. aut Bowles, J. aut Bryzgalov, V. aut Burns, J. aut Capiluppi, M. aut Capitani, G. P. aut Cisbani, E. aut Ciullo, G. aut Contalbrigo, M. aut Dalpiaz, P. F. aut Deconinck, W. aut De Leo, R. aut De Nardo, L. aut De Sanctis, E. aut Diefenthaler, M. aut Di Nezza, P. aut Düren, M. aut Ehrenfried, M. aut Elbakian, G. aut Ellinghaus, F. aut Fabbri, R. aut Fantoni, A. aut Felawka, L. aut Frullani, S. aut Gabbert, D. aut Gapienko, G. aut Gapienko, V. aut Garibaldi, F. aut Gavrilov, G. aut Gharibyan, V. aut Giordano, F. aut Gliske, S. aut Golembiovskaya, M. aut Hadjidakis, C. aut Hartig, M. aut Hasch, D. aut Hill, G. aut Hillenbrand, A. aut Hoek, M. aut Holler, Y. aut Hristova, I. aut Imazu, Y. aut Ivanilov, A. aut Jackson, H. E. aut Jo, H. S. aut Joosten, S. aut Kaiser, R. aut Karyan, G. aut Keri, T. aut Kinney, E. aut Kisselev, A. aut Kobayashi, N. aut Korotkov, V. aut Kozlov, V. aut Kravchenko, P. aut Krivokhijine, V. G. aut Lagamba, L. aut Lamb, R. aut Lapikás, L. aut Lehmann, I. aut Lenisa, P. aut Linden-Levy, L. A. aut López Ruiz, A. aut Lorenzon, W. aut Lu, X.-G. aut Lu, X.-R. aut Ma, B.-Q. aut Mahon, D. aut Makins, N. C. R. aut Manaenkov, S. I. aut Manfré, L. aut Mao, Y. aut Marianski, B. aut Martinez de la Ossa, A. aut Marukyan, H. aut Miller, C. A. aut Miyachi, Y. aut Movsisyan, A. aut Muccifora, V. aut Murray, M. aut Mussgiller, A. aut Nappi, E. aut Naryshkin, Y. aut Nass, A. aut Negodaev, M. aut Nowak, W.-D. aut Pappalardo, L. L. aut Perez-Benito, R. aut Pickert, N. aut Reimer, P. E. aut Reolon, A. R. aut Riedl, C. aut Rith, K. aut Rosner, G. aut Rostomyan, A. aut Rubin, J. aut Ryckbosch, D. aut Salomatin, Y. aut Sanftl, F. aut Schäfer, A. aut Schnell, G. aut Schüler, K. P. aut Seitz, B. aut Shibata, T.-A. aut Shutov, V. aut Stancari, M. aut Statera, M. aut Steffens, E. aut Steijger, J. J. M. aut Stinzing, F. aut Taroian, S. aut Terkulov, A. aut Trzcinski, A. aut Tytgat, M. aut Vandenbroucke, A. aut Van Haarlem, Y. aut Van Hulse, C. aut Veretennikov, D. aut Vikhrov, V. aut Vilardi, I. aut Wang, S. aut Yaschenko, S. aut Yen, S. aut Yu, W. aut Zihlmann, B. aut Zupranski, P. aut Enthalten in The European physical journal Berlin : Springer, 1998 71(2011), 4 vom: Apr. (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:71 year:2011 number:4 month:04 https://dx.doi.org/10.1140/epjc/s10052-011-1609-2 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_63 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_206 GBV_ILN_267 GBV_ILN_293 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2068 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_4012 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4305 GBV_ILN_4307 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4338 AR 71 2011 4 04 |
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10.1140/epjc/s10052-011-1609-2 doi (DE-627)SPR008325030 (SPR)s10052-011-1609-2-e DE-627 ger DE-627 rakwb eng Airapetian, A. verfasserin aut Ratios of helicity amplitudes for exclusive ρ0 electroproduction 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2011 Abstract Exclusive ρ0-meson electroproduction is studied in the HERMES experiment, using a 27.6 GeV longitudinally polarized electron/positron beam and unpolarized hydrogen and deuterium targets in the kinematic region 0.5 $ GeV^{2} $<Q2<7.0 $ GeV^{2} $, 3.0 GeV <W<6.3 GeV, and −t′<0.4 $ GeV^{2} $. Real and imaginary parts of the ratios of the natural-parity-exchange helicity amplitudes T11 ($\gamma^{*}_{T} \rightarrow\rho_{T}$), T01 ($\gamma^{*}_{T} \rightarrow \rho_{L}$), T10 ($\gamma^{*}_{L} \rightarrow\rho_{T}$), and T1−1 ($\gamma^{*}_{-T} \rightarrow\rho_{T}$) to T00 ($\gamma^{*}_{L}\rightarrow\rho_{L}$) are extracted from the data. For the unnatural-parity-exchange amplitude U11, the ratio |U11/T00| is obtained. The Q2 and t′ dependences of these ratios are presented and compared with perturbative QCD predictions. Systematic Uncertainty (dpeaa)DE-He213 Amplitude Ratio (dpeaa)DE-He213 Total Uncertainty (dpeaa)DE-He213 Helicity Amplitude (dpeaa)DE-He213 ZEUS Collaboration (dpeaa)DE-He213 Akopov, N. aut Akopov, Z. aut Aschenauer, E. C. aut Augustyniak, W. aut Avakian, R. aut Avetissian, A. aut Avetisyan, E. aut Belostotski, S. aut Bianchi, N. aut Blok, H. P. aut Borissov, A. aut Bowles, J. aut Bryzgalov, V. aut Burns, J. aut Capiluppi, M. aut Capitani, G. P. aut Cisbani, E. aut Ciullo, G. aut Contalbrigo, M. aut Dalpiaz, P. F. aut Deconinck, W. aut De Leo, R. aut De Nardo, L. aut De Sanctis, E. aut Diefenthaler, M. aut Di Nezza, P. aut Düren, M. aut Ehrenfried, M. aut Elbakian, G. aut Ellinghaus, F. aut Fabbri, R. aut Fantoni, A. aut Felawka, L. aut Frullani, S. aut Gabbert, D. aut Gapienko, G. aut Gapienko, V. aut Garibaldi, F. aut Gavrilov, G. aut Gharibyan, V. aut Giordano, F. aut Gliske, S. aut Golembiovskaya, M. aut Hadjidakis, C. aut Hartig, M. aut Hasch, D. aut Hill, G. aut Hillenbrand, A. aut Hoek, M. aut Holler, Y. aut Hristova, I. aut Imazu, Y. aut Ivanilov, A. aut Jackson, H. E. aut Jo, H. S. aut Joosten, S. aut Kaiser, R. aut Karyan, G. aut Keri, T. aut Kinney, E. aut Kisselev, A. aut Kobayashi, N. aut Korotkov, V. aut Kozlov, V. aut Kravchenko, P. aut Krivokhijine, V. G. aut Lagamba, L. aut Lamb, R. aut Lapikás, L. aut Lehmann, I. aut Lenisa, P. aut Linden-Levy, L. A. aut López Ruiz, A. aut Lorenzon, W. aut Lu, X.-G. aut Lu, X.-R. aut Ma, B.-Q. aut Mahon, D. aut Makins, N. C. R. aut Manaenkov, S. I. aut Manfré, L. aut Mao, Y. aut Marianski, B. aut Martinez de la Ossa, A. aut Marukyan, H. aut Miller, C. A. aut Miyachi, Y. aut Movsisyan, A. aut Muccifora, V. aut Murray, M. aut Mussgiller, A. aut Nappi, E. aut Naryshkin, Y. aut Nass, A. aut Negodaev, M. aut Nowak, W.-D. aut Pappalardo, L. L. aut Perez-Benito, R. aut Pickert, N. aut Reimer, P. E. aut Reolon, A. R. aut Riedl, C. aut Rith, K. aut Rosner, G. aut Rostomyan, A. aut Rubin, J. aut Ryckbosch, D. aut Salomatin, Y. aut Sanftl, F. aut Schäfer, A. aut Schnell, G. aut Schüler, K. P. aut Seitz, B. aut Shibata, T.-A. aut Shutov, V. aut Stancari, M. aut Statera, M. aut Steffens, E. aut Steijger, J. J. M. aut Stinzing, F. aut Taroian, S. aut Terkulov, A. aut Trzcinski, A. aut Tytgat, M. aut Vandenbroucke, A. aut Van Haarlem, Y. aut Van Hulse, C. aut Veretennikov, D. aut Vikhrov, V. aut Vilardi, I. aut Wang, S. aut Yaschenko, S. aut Yen, S. aut Yu, W. aut Zihlmann, B. aut Zupranski, P. aut Enthalten in The European physical journal Berlin : Springer, 1998 71(2011), 4 vom: Apr. (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:71 year:2011 number:4 month:04 https://dx.doi.org/10.1140/epjc/s10052-011-1609-2 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_63 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_206 GBV_ILN_267 GBV_ILN_293 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2068 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_4012 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4305 GBV_ILN_4307 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4338 AR 71 2011 4 04 |
| allfieldsGer |
10.1140/epjc/s10052-011-1609-2 doi (DE-627)SPR008325030 (SPR)s10052-011-1609-2-e DE-627 ger DE-627 rakwb eng Airapetian, A. verfasserin aut Ratios of helicity amplitudes for exclusive ρ0 electroproduction 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2011 Abstract Exclusive ρ0-meson electroproduction is studied in the HERMES experiment, using a 27.6 GeV longitudinally polarized electron/positron beam and unpolarized hydrogen and deuterium targets in the kinematic region 0.5 $ GeV^{2} $<Q2<7.0 $ GeV^{2} $, 3.0 GeV <W<6.3 GeV, and −t′<0.4 $ GeV^{2} $. Real and imaginary parts of the ratios of the natural-parity-exchange helicity amplitudes T11 ($\gamma^{*}_{T} \rightarrow\rho_{T}$), T01 ($\gamma^{*}_{T} \rightarrow \rho_{L}$), T10 ($\gamma^{*}_{L} \rightarrow\rho_{T}$), and T1−1 ($\gamma^{*}_{-T} \rightarrow\rho_{T}$) to T00 ($\gamma^{*}_{L}\rightarrow\rho_{L}$) are extracted from the data. For the unnatural-parity-exchange amplitude U11, the ratio |U11/T00| is obtained. The Q2 and t′ dependences of these ratios are presented and compared with perturbative QCD predictions. Systematic Uncertainty (dpeaa)DE-He213 Amplitude Ratio (dpeaa)DE-He213 Total Uncertainty (dpeaa)DE-He213 Helicity Amplitude (dpeaa)DE-He213 ZEUS Collaboration (dpeaa)DE-He213 Akopov, N. aut Akopov, Z. aut Aschenauer, E. C. aut Augustyniak, W. aut Avakian, R. aut Avetissian, A. aut Avetisyan, E. aut Belostotski, S. aut Bianchi, N. aut Blok, H. P. aut Borissov, A. aut Bowles, J. aut Bryzgalov, V. aut Burns, J. aut Capiluppi, M. aut Capitani, G. P. aut Cisbani, E. aut Ciullo, G. aut Contalbrigo, M. aut Dalpiaz, P. F. aut Deconinck, W. aut De Leo, R. aut De Nardo, L. aut De Sanctis, E. aut Diefenthaler, M. aut Di Nezza, P. aut Düren, M. aut Ehrenfried, M. aut Elbakian, G. aut Ellinghaus, F. aut Fabbri, R. aut Fantoni, A. aut Felawka, L. aut Frullani, S. aut Gabbert, D. aut Gapienko, G. aut Gapienko, V. aut Garibaldi, F. aut Gavrilov, G. aut Gharibyan, V. aut Giordano, F. aut Gliske, S. aut Golembiovskaya, M. aut Hadjidakis, C. aut Hartig, M. aut Hasch, D. aut Hill, G. aut Hillenbrand, A. aut Hoek, M. aut Holler, Y. aut Hristova, I. aut Imazu, Y. aut Ivanilov, A. aut Jackson, H. E. aut Jo, H. S. aut Joosten, S. aut Kaiser, R. aut Karyan, G. aut Keri, T. aut Kinney, E. aut Kisselev, A. aut Kobayashi, N. aut Korotkov, V. aut Kozlov, V. aut Kravchenko, P. aut Krivokhijine, V. G. aut Lagamba, L. aut Lamb, R. aut Lapikás, L. aut Lehmann, I. aut Lenisa, P. aut Linden-Levy, L. A. aut López Ruiz, A. aut Lorenzon, W. aut Lu, X.-G. aut Lu, X.-R. aut Ma, B.-Q. aut Mahon, D. aut Makins, N. C. R. aut Manaenkov, S. I. aut Manfré, L. aut Mao, Y. aut Marianski, B. aut Martinez de la Ossa, A. aut Marukyan, H. aut Miller, C. A. aut Miyachi, Y. aut Movsisyan, A. aut Muccifora, V. aut Murray, M. aut Mussgiller, A. aut Nappi, E. aut Naryshkin, Y. aut Nass, A. aut Negodaev, M. aut Nowak, W.-D. aut Pappalardo, L. L. aut Perez-Benito, R. aut Pickert, N. aut Reimer, P. E. aut Reolon, A. R. aut Riedl, C. aut Rith, K. aut Rosner, G. aut Rostomyan, A. aut Rubin, J. aut Ryckbosch, D. aut Salomatin, Y. aut Sanftl, F. aut Schäfer, A. aut Schnell, G. aut Schüler, K. P. aut Seitz, B. aut Shibata, T.-A. aut Shutov, V. aut Stancari, M. aut Statera, M. aut Steffens, E. aut Steijger, J. J. M. aut Stinzing, F. aut Taroian, S. aut Terkulov, A. aut Trzcinski, A. aut Tytgat, M. aut Vandenbroucke, A. aut Van Haarlem, Y. aut Van Hulse, C. aut Veretennikov, D. aut Vikhrov, V. aut Vilardi, I. aut Wang, S. aut Yaschenko, S. aut Yen, S. aut Yu, W. aut Zihlmann, B. aut Zupranski, P. aut Enthalten in The European physical journal Berlin : Springer, 1998 71(2011), 4 vom: Apr. (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:71 year:2011 number:4 month:04 https://dx.doi.org/10.1140/epjc/s10052-011-1609-2 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_63 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_206 GBV_ILN_267 GBV_ILN_293 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2068 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_4012 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4305 GBV_ILN_4307 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4338 AR 71 2011 4 04 |
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10.1140/epjc/s10052-011-1609-2 doi (DE-627)SPR008325030 (SPR)s10052-011-1609-2-e DE-627 ger DE-627 rakwb eng Airapetian, A. verfasserin aut Ratios of helicity amplitudes for exclusive ρ0 electroproduction 2011 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s) 2011 Abstract Exclusive ρ0-meson electroproduction is studied in the HERMES experiment, using a 27.6 GeV longitudinally polarized electron/positron beam and unpolarized hydrogen and deuterium targets in the kinematic region 0.5 $ GeV^{2} $<Q2<7.0 $ GeV^{2} $, 3.0 GeV <W<6.3 GeV, and −t′<0.4 $ GeV^{2} $. Real and imaginary parts of the ratios of the natural-parity-exchange helicity amplitudes T11 ($\gamma^{*}_{T} \rightarrow\rho_{T}$), T01 ($\gamma^{*}_{T} \rightarrow \rho_{L}$), T10 ($\gamma^{*}_{L} \rightarrow\rho_{T}$), and T1−1 ($\gamma^{*}_{-T} \rightarrow\rho_{T}$) to T00 ($\gamma^{*}_{L}\rightarrow\rho_{L}$) are extracted from the data. For the unnatural-parity-exchange amplitude U11, the ratio |U11/T00| is obtained. The Q2 and t′ dependences of these ratios are presented and compared with perturbative QCD predictions. Systematic Uncertainty (dpeaa)DE-He213 Amplitude Ratio (dpeaa)DE-He213 Total Uncertainty (dpeaa)DE-He213 Helicity Amplitude (dpeaa)DE-He213 ZEUS Collaboration (dpeaa)DE-He213 Akopov, N. aut Akopov, Z. aut Aschenauer, E. C. aut Augustyniak, W. aut Avakian, R. aut Avetissian, A. aut Avetisyan, E. aut Belostotski, S. aut Bianchi, N. aut Blok, H. P. aut Borissov, A. aut Bowles, J. aut Bryzgalov, V. aut Burns, J. aut Capiluppi, M. aut Capitani, G. P. aut Cisbani, E. aut Ciullo, G. aut Contalbrigo, M. aut Dalpiaz, P. F. aut Deconinck, W. aut De Leo, R. aut De Nardo, L. aut De Sanctis, E. aut Diefenthaler, M. aut Di Nezza, P. aut Düren, M. aut Ehrenfried, M. aut Elbakian, G. aut Ellinghaus, F. aut Fabbri, R. aut Fantoni, A. aut Felawka, L. aut Frullani, S. aut Gabbert, D. aut Gapienko, G. aut Gapienko, V. aut Garibaldi, F. aut Gavrilov, G. aut Gharibyan, V. aut Giordano, F. aut Gliske, S. aut Golembiovskaya, M. aut Hadjidakis, C. aut Hartig, M. aut Hasch, D. aut Hill, G. aut Hillenbrand, A. aut Hoek, M. aut Holler, Y. aut Hristova, I. aut Imazu, Y. aut Ivanilov, A. aut Jackson, H. E. aut Jo, H. S. aut Joosten, S. aut Kaiser, R. aut Karyan, G. aut Keri, T. aut Kinney, E. aut Kisselev, A. aut Kobayashi, N. aut Korotkov, V. aut Kozlov, V. aut Kravchenko, P. aut Krivokhijine, V. G. aut Lagamba, L. aut Lamb, R. aut Lapikás, L. aut Lehmann, I. aut Lenisa, P. aut Linden-Levy, L. A. aut López Ruiz, A. aut Lorenzon, W. aut Lu, X.-G. aut Lu, X.-R. aut Ma, B.-Q. aut Mahon, D. aut Makins, N. C. R. aut Manaenkov, S. I. aut Manfré, L. aut Mao, Y. aut Marianski, B. aut Martinez de la Ossa, A. aut Marukyan, H. aut Miller, C. A. aut Miyachi, Y. aut Movsisyan, A. aut Muccifora, V. aut Murray, M. aut Mussgiller, A. aut Nappi, E. aut Naryshkin, Y. aut Nass, A. aut Negodaev, M. aut Nowak, W.-D. aut Pappalardo, L. L. aut Perez-Benito, R. aut Pickert, N. aut Reimer, P. E. aut Reolon, A. R. aut Riedl, C. aut Rith, K. aut Rosner, G. aut Rostomyan, A. aut Rubin, J. aut Ryckbosch, D. aut Salomatin, Y. aut Sanftl, F. aut Schäfer, A. aut Schnell, G. aut Schüler, K. P. aut Seitz, B. aut Shibata, T.-A. aut Shutov, V. aut Stancari, M. aut Statera, M. aut Steffens, E. aut Steijger, J. J. M. aut Stinzing, F. aut Taroian, S. aut Terkulov, A. aut Trzcinski, A. aut Tytgat, M. aut Vandenbroucke, A. aut Van Haarlem, Y. aut Van Hulse, C. aut Veretennikov, D. aut Vikhrov, V. aut Vilardi, I. aut Wang, S. aut Yaschenko, S. aut Yen, S. aut Yu, W. aut Zihlmann, B. aut Zupranski, P. aut Enthalten in The European physical journal Berlin : Springer, 1998 71(2011), 4 vom: Apr. (DE-627)253722934 (DE-600)1459069-4 1434-6052 nnns volume:71 year:2011 number:4 month:04 https://dx.doi.org/10.1140/epjc/s10052-011-1609-2 kostenfrei Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_63 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_206 GBV_ILN_267 GBV_ILN_293 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2068 GBV_ILN_2106 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_4012 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4305 GBV_ILN_4307 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4338 AR 71 2011 4 04 |
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Airapetian, A. @@aut@@ Akopov, N. @@aut@@ Akopov, Z. @@aut@@ Aschenauer, E. C. @@aut@@ Augustyniak, W. @@aut@@ Avakian, R. @@aut@@ Avetissian, A. @@aut@@ Avetisyan, E. @@aut@@ Belostotski, S. @@aut@@ Bianchi, N. @@aut@@ Blok, H. P. @@aut@@ Borissov, A. @@aut@@ Bowles, J. @@aut@@ Bryzgalov, V. @@aut@@ Burns, J. @@aut@@ Capiluppi, M. @@aut@@ Capitani, G. P. @@aut@@ Cisbani, E. @@aut@@ Ciullo, G. @@aut@@ Contalbrigo, M. @@aut@@ Dalpiaz, P. F. @@aut@@ Deconinck, W. @@aut@@ De Leo, R. @@aut@@ De Nardo, L. @@aut@@ De Sanctis, E. @@aut@@ Diefenthaler, M. @@aut@@ Di Nezza, P. @@aut@@ Düren, M. @@aut@@ Ehrenfried, M. @@aut@@ Elbakian, G. @@aut@@ Ellinghaus, F. @@aut@@ Fabbri, R. @@aut@@ Fantoni, A. @@aut@@ Felawka, L. @@aut@@ Frullani, S. @@aut@@ Gabbert, D. @@aut@@ Gapienko, G. @@aut@@ Gapienko, V. @@aut@@ Garibaldi, F. @@aut@@ Gavrilov, G. @@aut@@ Gharibyan, V. @@aut@@ Giordano, F. @@aut@@ Gliske, S. @@aut@@ Golembiovskaya, M. @@aut@@ Hadjidakis, C. @@aut@@ Hartig, M. @@aut@@ Hasch, D. @@aut@@ Hill, G. @@aut@@ Hillenbrand, A. @@aut@@ Hoek, M. @@aut@@ Holler, Y. @@aut@@ Hristova, I. @@aut@@ Imazu, Y. @@aut@@ Ivanilov, A. @@aut@@ Jackson, H. E. @@aut@@ Jo, H. S. @@aut@@ Joosten, S. @@aut@@ Kaiser, R. @@aut@@ Karyan, G. @@aut@@ Keri, T. @@aut@@ Kinney, E. @@aut@@ Kisselev, A. @@aut@@ Kobayashi, N. @@aut@@ Korotkov, V. @@aut@@ Kozlov, V. @@aut@@ Kravchenko, P. @@aut@@ Krivokhijine, V. G. @@aut@@ Lagamba, L. @@aut@@ Lamb, R. @@aut@@ Lapikás, L. @@aut@@ Lehmann, I. @@aut@@ Lenisa, P. @@aut@@ Linden-Levy, L. A. @@aut@@ López Ruiz, A. @@aut@@ Lorenzon, W. @@aut@@ Lu, X.-G. @@aut@@ Lu, X.-R. @@aut@@ Ma, B.-Q. @@aut@@ Mahon, D. @@aut@@ Makins, N. C. R. @@aut@@ Manaenkov, S. I. @@aut@@ Manfré, L. @@aut@@ Mao, Y. @@aut@@ Marianski, B. @@aut@@ Martinez de la Ossa, A. @@aut@@ Marukyan, H. @@aut@@ Miller, C. A. @@aut@@ Miyachi, Y. @@aut@@ Movsisyan, A. @@aut@@ Muccifora, V. @@aut@@ Murray, M. @@aut@@ Mussgiller, A. @@aut@@ Nappi, E. @@aut@@ Naryshkin, Y. @@aut@@ Nass, A. @@aut@@ Negodaev, M. @@aut@@ Nowak, W.-D. @@aut@@ Pappalardo, L. L. @@aut@@ Perez-Benito, R. @@aut@@ Pickert, N. @@aut@@ Reimer, P. E. @@aut@@ Reolon, A. R. @@aut@@ Riedl, C. @@aut@@ Rith, K. @@aut@@ Rosner, G. @@aut@@ Rostomyan, A. @@aut@@ Rubin, J. @@aut@@ Ryckbosch, D. @@aut@@ Salomatin, Y. @@aut@@ Sanftl, F. @@aut@@ Schäfer, A. @@aut@@ Schnell, G. @@aut@@ Schüler, K. P. @@aut@@ Seitz, B. @@aut@@ Shibata, T.-A. @@aut@@ Shutov, V. @@aut@@ Stancari, M. @@aut@@ Statera, M. @@aut@@ Steffens, E. @@aut@@ Steijger, J. J. M. @@aut@@ Stinzing, F. @@aut@@ Taroian, S. @@aut@@ Terkulov, A. @@aut@@ Trzcinski, A. @@aut@@ Tytgat, M. @@aut@@ Vandenbroucke, A. @@aut@@ Van Haarlem, Y. @@aut@@ Van Hulse, C. @@aut@@ Veretennikov, D. @@aut@@ Vikhrov, V. @@aut@@ Vilardi, I. @@aut@@ Wang, S. @@aut@@ Yaschenko, S. @@aut@@ Yen, S. @@aut@@ Yu, W. @@aut@@ Zihlmann, B. @@aut@@ Zupranski, P. @@aut@@ |
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englisch |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">SPR008325030</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20240120064807.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">201005s2011 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1140/epjc/s10052-011-1609-2</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR008325030</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s10052-011-1609-2-e</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Airapetian, A.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Ratios of helicity amplitudes for exclusive ρ0 electroproduction</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2011</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© The Author(s) 2011</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract Exclusive ρ0-meson electroproduction is studied in the HERMES experiment, using a 27.6 GeV longitudinally polarized electron/positron beam and unpolarized hydrogen and deuterium targets in the kinematic region 0.5 $ GeV^{2} $<Q2<7.0 $ GeV^{2} $, 3.0 GeV <W<6.3 GeV, and −t′<0.4 $ GeV^{2} $. Real and imaginary parts of the ratios of the natural-parity-exchange helicity amplitudes T11 ($\gamma^{*}_{T} \rightarrow\rho_{T}$), T01 ($\gamma^{*}_{T} \rightarrow \rho_{L}$), T10 ($\gamma^{*}_{L} \rightarrow\rho_{T}$), and T1−1 ($\gamma^{*}_{-T} \rightarrow\rho_{T}$) to T00 ($\gamma^{*}_{L}\rightarrow\rho_{L}$) are extracted from the data. For the unnatural-parity-exchange amplitude U11, the ratio |U11/T00| is obtained. The Q2 and t′ dependences of these ratios are presented and compared with perturbative QCD predictions.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Systematic Uncertainty</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Amplitude Ratio</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Total Uncertainty</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Helicity Amplitude</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">ZEUS Collaboration</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Akopov, N.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Akopov, Z.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Aschenauer, E. 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Ratios of helicity amplitudes for exclusive ρ0 electroproduction Systematic Uncertainty (dpeaa)DE-He213 Amplitude Ratio (dpeaa)DE-He213 Total Uncertainty (dpeaa)DE-He213 Helicity Amplitude (dpeaa)DE-He213 ZEUS Collaboration (dpeaa)DE-He213 |
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Airapetian, A. Akopov, N. Akopov, Z. Aschenauer, E. C. Augustyniak, W. Avakian, R. Avetissian, A. Avetisyan, E. Belostotski, S. Bianchi, N. Blok, H. P. Borissov, A. Bowles, J. Bryzgalov, V. Burns, J. Capiluppi, M. Capitani, G. P. Cisbani, E. Ciullo, G. Contalbrigo, M. Dalpiaz, P. F. Deconinck, W. De Leo, R. De Nardo, L. De Sanctis, E. Diefenthaler, M. Di Nezza, P. Düren, M. Ehrenfried, M. Elbakian, G. Ellinghaus, F. Fabbri, R. Fantoni, A. Felawka, L. Frullani, S. Gabbert, D. Gapienko, G. Gapienko, V. Garibaldi, F. Gavrilov, G. Gharibyan, V. Giordano, F. Gliske, S. Golembiovskaya, M. Hadjidakis, C. Hartig, M. Hasch, D. Hill, G. Hillenbrand, A. Hoek, M. Holler, Y. Hristova, I. Imazu, Y. Ivanilov, A. Jackson, H. E. Jo, H. S. Joosten, S. Kaiser, R. Karyan, G. Keri, T. Kinney, E. Kisselev, A. Kobayashi, N. Korotkov, V. Kozlov, V. Kravchenko, P. Krivokhijine, V. G. Lagamba, L. Lamb, R. Lapikás, L. Lehmann, I. Lenisa, P. Linden-Levy, L. A. López Ruiz, A. Lorenzon, W. Lu, X.-G. Lu, X.-R. Ma, B.-Q. Mahon, D. Makins, N. C. R. Manaenkov, S. I. Manfré, L. Mao, Y. Marianski, B. Martinez de la Ossa, A. Marukyan, H. Miller, C. A. Miyachi, Y. Movsisyan, A. Muccifora, V. Murray, M. Mussgiller, A. Nappi, E. Naryshkin, Y. Nass, A. Negodaev, M. Nowak, W.-D. Pappalardo, L. L. Perez-Benito, R. Pickert, N. Reimer, P. E. Reolon, A. R. Riedl, C. Rith, K. Rosner, G. Rostomyan, A. Rubin, J. Ryckbosch, D. Salomatin, Y. Sanftl, F. Schäfer, A. Schnell, G. Schüler, K. P. Seitz, B. Shibata, T.-A. Shutov, V. Stancari, M. Statera, M. Steffens, E. Steijger, J. J. M. Stinzing, F. Taroian, S. Terkulov, A. Trzcinski, A. Tytgat, M. Vandenbroucke, A. Van Haarlem, Y. Van Hulse, C. Veretennikov, D. Vikhrov, V. Vilardi, I. Wang, S. Yaschenko, S. Yen, S. Yu, W. Zihlmann, B. Zupranski, P. |
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Airapetian, A. |
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10.1140/epjc/s10052-011-1609-2 |
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ratios of helicity amplitudes for exclusive ρ0 electroproduction |
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Ratios of helicity amplitudes for exclusive ρ0 electroproduction |
| abstract |
Abstract Exclusive ρ0-meson electroproduction is studied in the HERMES experiment, using a 27.6 GeV longitudinally polarized electron/positron beam and unpolarized hydrogen and deuterium targets in the kinematic region 0.5 $ GeV^{2} $<Q2<7.0 $ GeV^{2} $, 3.0 GeV <W<6.3 GeV, and −t′<0.4 $ GeV^{2} $. Real and imaginary parts of the ratios of the natural-parity-exchange helicity amplitudes T11 ($\gamma^{*}_{T} \rightarrow\rho_{T}$), T01 ($\gamma^{*}_{T} \rightarrow \rho_{L}$), T10 ($\gamma^{*}_{L} \rightarrow\rho_{T}$), and T1−1 ($\gamma^{*}_{-T} \rightarrow\rho_{T}$) to T00 ($\gamma^{*}_{L}\rightarrow\rho_{L}$) are extracted from the data. For the unnatural-parity-exchange amplitude U11, the ratio |U11/T00| is obtained. The Q2 and t′ dependences of these ratios are presented and compared with perturbative QCD predictions. © The Author(s) 2011 |
| abstractGer |
Abstract Exclusive ρ0-meson electroproduction is studied in the HERMES experiment, using a 27.6 GeV longitudinally polarized electron/positron beam and unpolarized hydrogen and deuterium targets in the kinematic region 0.5 $ GeV^{2} $<Q2<7.0 $ GeV^{2} $, 3.0 GeV <W<6.3 GeV, and −t′<0.4 $ GeV^{2} $. Real and imaginary parts of the ratios of the natural-parity-exchange helicity amplitudes T11 ($\gamma^{*}_{T} \rightarrow\rho_{T}$), T01 ($\gamma^{*}_{T} \rightarrow \rho_{L}$), T10 ($\gamma^{*}_{L} \rightarrow\rho_{T}$), and T1−1 ($\gamma^{*}_{-T} \rightarrow\rho_{T}$) to T00 ($\gamma^{*}_{L}\rightarrow\rho_{L}$) are extracted from the data. For the unnatural-parity-exchange amplitude U11, the ratio |U11/T00| is obtained. The Q2 and t′ dependences of these ratios are presented and compared with perturbative QCD predictions. © The Author(s) 2011 |
| abstract_unstemmed |
Abstract Exclusive ρ0-meson electroproduction is studied in the HERMES experiment, using a 27.6 GeV longitudinally polarized electron/positron beam and unpolarized hydrogen and deuterium targets in the kinematic region 0.5 $ GeV^{2} $<Q2<7.0 $ GeV^{2} $, 3.0 GeV <W<6.3 GeV, and −t′<0.4 $ GeV^{2} $. Real and imaginary parts of the ratios of the natural-parity-exchange helicity amplitudes T11 ($\gamma^{*}_{T} \rightarrow\rho_{T}$), T01 ($\gamma^{*}_{T} \rightarrow \rho_{L}$), T10 ($\gamma^{*}_{L} \rightarrow\rho_{T}$), and T1−1 ($\gamma^{*}_{-T} \rightarrow\rho_{T}$) to T00 ($\gamma^{*}_{L}\rightarrow\rho_{L}$) are extracted from the data. For the unnatural-parity-exchange amplitude U11, the ratio |U11/T00| is obtained. The Q2 and t′ dependences of these ratios are presented and compared with perturbative QCD predictions. © The Author(s) 2011 |
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Real and imaginary parts of the ratios of the natural-parity-exchange helicity amplitudes T11 ($\gamma^{*}_{T} \rightarrow\rho_{T}$), T01 ($\gamma^{*}_{T} \rightarrow \rho_{L}$), T10 ($\gamma^{*}_{L} \rightarrow\rho_{T}$), and T1−1 ($\gamma^{*}_{-T} \rightarrow\rho_{T}$) to T00 ($\gamma^{*}_{L}\rightarrow\rho_{L}$) are extracted from the data. For the unnatural-parity-exchange amplitude U11, the ratio |U11/T00| is obtained. 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