Beam Charge Asymmetries for Deeply Virtual Compton Scattering on the Proton at CLAS12
The parameterization of the nucleon structure through Generalized Parton Distributions (GPDs) shed a new light on the nucleon internal dynamics. For its direct interpretation, Deeply Virtual Compton Scattering (DVCS) is the golden channel for GPDs investigation. The DVCS process interferes with the...
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creator | Voutier, E Burkert, V Niccolai, S Paremuzyan, R Afanasev, A J -S Alvarado-Galeano Atoui, M Barion, L Battaglieri, M Bernauer, J Bianconi, A Bondi, M Briscoe, W Camsonne, A Capobianco, R Celentano, A Chatagnon, P Chetry, T Ciullo, G Cole, P Contalbrigo, M Costantini, G Defurne, M Deur, A De Vita, R Diehl, S Dupré, R Elouadrhiri, L Fernando, I Filippi, A est, T Girod, F -X Gosta, G Grames, J Gueye, P Habet, S Hattawy, M Higinbotham, D Hobart, A Hyde, C Joo, K Kim, A Klimenko, V Kubarovsky, V Leali, M Lenisa, P Marchand, D Marsicano, L Mascagna, V Matamoros, D McCaughan, M McKinnon, B Migliorati, S Mitra, H S Movsisyan, A Muñoz-Camacho, C Osipenko, M Ouillon, M Pappalardo, L Pasquini, B Pasyuk, E Pilleux, N Poelker, M Raue, B Ripani, M Santos, R Schmidt, A Singh, R Sokhan, D Spreafico, M Stoler, P Strakovsky, I Taiuti, M Venturelli, L P -K Wang Wei, X Zhao, Z the CLAS Collaboration the Jefferson Lab Positron Working Group |
description | The parameterization of the nucleon structure through Generalized Parton Distributions (GPDs) shed a new light on the nucleon internal dynamics. For its direct interpretation, Deeply Virtual Compton Scattering (DVCS) is the golden channel for GPDs investigation. The DVCS process interferes with the Bethe-Heitler (BH) mechanism to constitute the leading order amplitude of the \(eN \to eN\gamma\) process. The study of the \(ep\gamma\) reaction with polarized positron and electron beams gives a complete set of unique observables to unravel the different contributions to the \(ep \gamma\) cross section. This separates the different reaction amplitudes, providing a direct access to their real and imaginary parts which procures crucial constraints on the model dependences and associated systematic uncertainties on GPDs extraction. The real part of the BH-DVCS interference amplitude is particularly sensitive to the \(D\)-term which parameterizes the Gravitational Form Factors of the nucleon. The separation of the imaginary parts of the interference and DVCS amplitudes provides insights on possible higher-twist effects. We propose to measure the unpolarized and polarized Beam Charge Asymmetries (BCAs) of the \(\vec{e}^{\pm}p \to e^{\pm}p \gamma\) process on an unpolarized hydrogen target with {\tt CLAS12}, using polarized positron and electron beams at 10.6 GeV. The azimuthal and \(t\)-dependences of the unpolarized and polarized BCAs will be measured over a large \((x_B,Q^2)\) phase space using a 100 day run with a luminosity of 0.66\(\times 10^{35}\)cm\(^{-2}\cdot\)s\(^{-1}\). |
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For its direct interpretation, Deeply Virtual Compton Scattering (DVCS) is the golden channel for GPDs investigation. The DVCS process interferes with the Bethe-Heitler (BH) mechanism to constitute the leading order amplitude of the \(eN \to eN\gamma\) process. The study of the \(ep\gamma\) reaction with polarized positron and electron beams gives a complete set of unique observables to unravel the different contributions to the \(ep \gamma\) cross section. This separates the different reaction amplitudes, providing a direct access to their real and imaginary parts which procures crucial constraints on the model dependences and associated systematic uncertainties on GPDs extraction. The real part of the BH-DVCS interference amplitude is particularly sensitive to the \(D\)-term which parameterizes the Gravitational Form Factors of the nucleon. The separation of the imaginary parts of the interference and DVCS amplitudes provides insights on possible higher-twist effects. We propose to measure the unpolarized and polarized Beam Charge Asymmetries (BCAs) of the \(\vec{e}^{\pm}p \to e^{\pm}p \gamma\) process on an unpolarized hydrogen target with {\tt CLAS12}, using polarized positron and electron beams at 10.6 GeV. The azimuthal and \(t\)-dependences of the unpolarized and polarized BCAs will be measured over a large \((x_B,Q^2)\) phase space using a 100 day run with a luminosity of 0.66\(\times 10^{35}\)cm\(^{-2}\cdot\)s\(^{-1}\).</description><identifier>EISSN: 2331-8422</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Amplitudes ; Asymmetry ; Constraint modelling ; Elastic scattering ; Electron beams ; Form factors ; Interference ; Luminosity ; Nucleons ; Parameterization</subject><ispartof>arXiv.org, 2023-11</ispartof><rights>2023. This work is published under http://arxiv.org/licenses/nonexclusive-distrib/1.0/ (the “License”). 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For its direct interpretation, Deeply Virtual Compton Scattering (DVCS) is the golden channel for GPDs investigation. The DVCS process interferes with the Bethe-Heitler (BH) mechanism to constitute the leading order amplitude of the \(eN \to eN\gamma\) process. The study of the \(ep\gamma\) reaction with polarized positron and electron beams gives a complete set of unique observables to unravel the different contributions to the \(ep \gamma\) cross section. This separates the different reaction amplitudes, providing a direct access to their real and imaginary parts which procures crucial constraints on the model dependences and associated systematic uncertainties on GPDs extraction. The real part of the BH-DVCS interference amplitude is particularly sensitive to the \(D\)-term which parameterizes the Gravitational Form Factors of the nucleon. The separation of the imaginary parts of the interference and DVCS amplitudes provides insights on possible higher-twist effects. We propose to measure the unpolarized and polarized Beam Charge Asymmetries (BCAs) of the \(\vec{e}^{\pm}p \to e^{\pm}p \gamma\) process on an unpolarized hydrogen target with {\tt CLAS12}, using polarized positron and electron beams at 10.6 GeV. 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Z</creator><creator>the CLAS Collaboration</creator><creator>the Jefferson Lab Positron Working Group</creator><general>Cornell University Library, arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope></search><sort><creationdate>20231113</creationdate><title>Beam Charge Asymmetries for Deeply Virtual Compton Scattering on the Proton at CLAS12</title><author>Voutier, E ; Burkert, V ; Niccolai, S ; Paremuzyan, R ; Afanasev, A ; J -S Alvarado-Galeano ; Atoui, M ; Barion, L ; Battaglieri, M ; Bernauer, J ; Bianconi, A ; Bondi, M ; Briscoe, W ; Camsonne, A ; Capobianco, R ; Celentano, A ; Chatagnon, P ; Chetry, T ; Ciullo, G ; Cole, P ; Contalbrigo, M ; 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C</creatorcontrib><creatorcontrib>Osipenko, M</creatorcontrib><creatorcontrib>Ouillon, M</creatorcontrib><creatorcontrib>Pappalardo, L</creatorcontrib><creatorcontrib>Pasquini, B</creatorcontrib><creatorcontrib>Pasyuk, E</creatorcontrib><creatorcontrib>Pilleux, N</creatorcontrib><creatorcontrib>Poelker, M</creatorcontrib><creatorcontrib>Raue, B</creatorcontrib><creatorcontrib>Ripani, M</creatorcontrib><creatorcontrib>Santos, R</creatorcontrib><creatorcontrib>Schmidt, A</creatorcontrib><creatorcontrib>Singh, R</creatorcontrib><creatorcontrib>Sokhan, D</creatorcontrib><creatorcontrib>Spreafico, M</creatorcontrib><creatorcontrib>Stoler, P</creatorcontrib><creatorcontrib>Strakovsky, I</creatorcontrib><creatorcontrib>Taiuti, M</creatorcontrib><creatorcontrib>Venturelli, L</creatorcontrib><creatorcontrib>P -K Wang</creatorcontrib><creatorcontrib>Wei, X</creatorcontrib><creatorcontrib>Zhao, Z</creatorcontrib><creatorcontrib>the CLAS Collaboration</creatorcontrib><creatorcontrib>the Jefferson Lab Positron Working Group</creatorcontrib><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>ProQuest Engineering Collection</collection><collection>Engineering Database</collection><collection>Access via ProQuest (Open Access)</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><collection>Engineering Collection</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Voutier, E</au><au>Burkert, V</au><au>Niccolai, S</au><au>Paremuzyan, R</au><au>Afanasev, A</au><au>J -S Alvarado-Galeano</au><au>Atoui, M</au><au>Barion, L</au><au>Battaglieri, M</au><au>Bernauer, J</au><au>Bianconi, A</au><au>Bondi, M</au><au>Briscoe, W</au><au>Camsonne, A</au><au>Capobianco, R</au><au>Celentano, A</au><au>Chatagnon, P</au><au>Chetry, T</au><au>Ciullo, G</au><au>Cole, P</au><au>Contalbrigo, M</au><au>Costantini, G</au><au>Defurne, M</au><au>Deur, A</au><au>De Vita, R</au><au>Diehl, S</au><au>Dupré, R</au><au>Elouadrhiri, L</au><au>Fernando, I</au><au>Filippi, A</au><au>est, T</au><au>Girod, F -X</au><au>Gosta, G</au><au>Grames, J</au><au>Gueye, P</au><au>Habet, S</au><au>Hattawy, M</au><au>Higinbotham, D</au><au>Hobart, A</au><au>Hyde, C</au><au>Joo, K</au><au>Kim, A</au><au>Klimenko, V</au><au>Kubarovsky, V</au><au>Leali, M</au><au>Lenisa, P</au><au>Marchand, D</au><au>Marsicano, L</au><au>Mascagna, V</au><au>Matamoros, D</au><au>McCaughan, M</au><au>McKinnon, B</au><au>Migliorati, S</au><au>Mitra, H S</au><au>Movsisyan, A</au><au>Muñoz-Camacho, C</au><au>Osipenko, M</au><au>Ouillon, M</au><au>Pappalardo, L</au><au>Pasquini, B</au><au>Pasyuk, E</au><au>Pilleux, N</au><au>Poelker, M</au><au>Raue, B</au><au>Ripani, M</au><au>Santos, R</au><au>Schmidt, A</au><au>Singh, R</au><au>Sokhan, D</au><au>Spreafico, M</au><au>Stoler, P</au><au>Strakovsky, I</au><au>Taiuti, M</au><au>Venturelli, L</au><au>P -K Wang</au><au>Wei, X</au><au>Zhao, Z</au><au>the CLAS Collaboration</au><au>the Jefferson Lab Positron Working Group</au><format>book</format><genre>document</genre><ristype>GEN</ristype><atitle>Beam Charge Asymmetries for Deeply Virtual Compton Scattering on the Proton at CLAS12</atitle><jtitle>arXiv.org</jtitle><date>2023-11-13</date><risdate>2023</risdate><eissn>2331-8422</eissn><abstract>The parameterization of the nucleon structure through Generalized Parton Distributions (GPDs) shed a new light on the nucleon internal dynamics. For its direct interpretation, Deeply Virtual Compton Scattering (DVCS) is the golden channel for GPDs investigation. The DVCS process interferes with the Bethe-Heitler (BH) mechanism to constitute the leading order amplitude of the \(eN \to eN\gamma\) process. The study of the \(ep\gamma\) reaction with polarized positron and electron beams gives a complete set of unique observables to unravel the different contributions to the \(ep \gamma\) cross section. This separates the different reaction amplitudes, providing a direct access to their real and imaginary parts which procures crucial constraints on the model dependences and associated systematic uncertainties on GPDs extraction. The real part of the BH-DVCS interference amplitude is particularly sensitive to the \(D\)-term which parameterizes the Gravitational Form Factors of the nucleon. The separation of the imaginary parts of the interference and DVCS amplitudes provides insights on possible higher-twist effects. We propose to measure the unpolarized and polarized Beam Charge Asymmetries (BCAs) of the \(\vec{e}^{\pm}p \to e^{\pm}p \gamma\) process on an unpolarized hydrogen target with {\tt CLAS12}, using polarized positron and electron beams at 10.6 GeV. The azimuthal and \(t\)-dependences of the unpolarized and polarized BCAs will be measured over a large \((x_B,Q^2)\) phase space using a 100 day run with a luminosity of 0.66\(\times 10^{35}\)cm\(^{-2}\cdot\)s\(^{-1}\).</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><oa>free_for_read</oa></addata></record> |
fulltext | fulltext |
identifier | EISSN: 2331-8422 |
ispartof | arXiv.org, 2023-11 |
issn | 2331-8422 |
language | eng |
recordid | cdi_proquest_journals_2889791008 |
source | Free E- Journals |
subjects | Amplitudes Asymmetry Constraint modelling Elastic scattering Electron beams Form factors Interference Luminosity Nucleons Parameterization |
title | Beam Charge Asymmetries for Deeply Virtual Compton Scattering on the Proton at CLAS12 |
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