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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Hauptverfasser: 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
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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. 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><subject>Amplitudes</subject><subject>Asymmetry</subject><subject>Constraint modelling</subject><subject>Elastic scattering</subject><subject>Electron beams</subject><subject>Form factors</subject><subject>Interference</subject><subject>Luminosity</subject><subject>Nucleons</subject><subject>Parameterization</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><recordid>eNqNik8LgjAcQEcQJOV3-EFnYc7MebRVdOgQWF1lxM9_OGfbPPjtM-gDdHo83lsQj0VRGPAdYyviW9tSStk-YXEceeRxQKlA1NJUCJmdlEJnGrRQagNHxKGb4NkYN8oOhFaD0z3kL-kcmqavYDZXI9yM_gbpQFyzPGQbsixlZ9H_cU2259NdXILB6PeI1hWtHk0_p4JxniZpSCmP_rs-MnI_lA</recordid><startdate>20231113</startdate><enddate>20231113</enddate><creator>Voutier, E</creator><creator>Burkert, V</creator><creator>Niccolai, S</creator><creator>Paremuzyan, R</creator><creator>Afanasev, A</creator><creator>J -S Alvarado-Galeano</creator><creator>Atoui, M</creator><creator>Barion, L</creator><creator>Battaglieri, M</creator><creator>Bernauer, J</creator><creator>Bianconi, A</creator><creator>Bondi, M</creator><creator>Briscoe, W</creator><creator>Camsonne, A</creator><creator>Capobianco, R</creator><creator>Celentano, A</creator><creator>Chatagnon, P</creator><creator>Chetry, T</creator><creator>Ciullo, G</creator><creator>Cole, P</creator><creator>Contalbrigo, M</creator><creator>Costantini, G</creator><creator>Defurne, M</creator><creator>Deur, A</creator><creator>De Vita, R</creator><creator>Diehl, S</creator><creator>Dupré, R</creator><creator>Elouadrhiri, L</creator><creator>Fernando, I</creator><creator>Filippi, A</creator><creator>est, T</creator><creator>Girod, F -X</creator><creator>Gosta, G</creator><creator>Grames, J</creator><creator>Gueye, P</creator><creator>Habet, S</creator><creator>Hattawy, M</creator><creator>Higinbotham, D</creator><creator>Hobart, A</creator><creator>Hyde, C</creator><creator>Joo, K</creator><creator>Kim, A</creator><creator>Klimenko, V</creator><creator>Kubarovsky, V</creator><creator>Leali, M</creator><creator>Lenisa, P</creator><creator>Marchand, D</creator><creator>Marsicano, L</creator><creator>Mascagna, V</creator><creator>Matamoros, D</creator><creator>McCaughan, M</creator><creator>McKinnon, B</creator><creator>Migliorati, S</creator><creator>Mitra, H S</creator><creator>Movsisyan, A</creator><creator>Muñoz-Camacho, C</creator><creator>Osipenko, M</creator><creator>Ouillon, M</creator><creator>Pappalardo, L</creator><creator>Pasquini, B</creator><creator>Pasyuk, E</creator><creator>Pilleux, N</creator><creator>Poelker, M</creator><creator>Raue, B</creator><creator>Ripani, M</creator><creator>Santos, R</creator><creator>Schmidt, A</creator><creator>Singh, R</creator><creator>Sokhan, D</creator><creator>Spreafico, M</creator><creator>Stoler, P</creator><creator>Strakovsky, I</creator><creator>Taiuti, M</creator><creator>Venturelli, L</creator><creator>P -K Wang</creator><creator>Wei, X</creator><creator>Zhao, 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 ; 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</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-proquest_journals_28897910083</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>Amplitudes</topic><topic>Asymmetry</topic><topic>Constraint modelling</topic><topic>Elastic scattering</topic><topic>Electron beams</topic><topic>Form factors</topic><topic>Interference</topic><topic>Luminosity</topic><topic>Nucleons</topic><topic>Parameterization</topic><toplevel>online_resources</toplevel><creatorcontrib>Voutier, E</creatorcontrib><creatorcontrib>Burkert, V</creatorcontrib><creatorcontrib>Niccolai, S</creatorcontrib><creatorcontrib>Paremuzyan, R</creatorcontrib><creatorcontrib>Afanasev, A</creatorcontrib><creatorcontrib>J -S Alvarado-Galeano</creatorcontrib><creatorcontrib>Atoui, M</creatorcontrib><creatorcontrib>Barion, L</creatorcontrib><creatorcontrib>Battaglieri, M</creatorcontrib><creatorcontrib>Bernauer, J</creatorcontrib><creatorcontrib>Bianconi, A</creatorcontrib><creatorcontrib>Bondi, M</creatorcontrib><creatorcontrib>Briscoe, W</creatorcontrib><creatorcontrib>Camsonne, A</creatorcontrib><creatorcontrib>Capobianco, R</creatorcontrib><creatorcontrib>Celentano, A</creatorcontrib><creatorcontrib>Chatagnon, P</creatorcontrib><creatorcontrib>Chetry, T</creatorcontrib><creatorcontrib>Ciullo, G</creatorcontrib><creatorcontrib>Cole, P</creatorcontrib><creatorcontrib>Contalbrigo, M</creatorcontrib><creatorcontrib>Costantini, G</creatorcontrib><creatorcontrib>Defurne, M</creatorcontrib><creatorcontrib>Deur, A</creatorcontrib><creatorcontrib>De Vita, R</creatorcontrib><creatorcontrib>Diehl, S</creatorcontrib><creatorcontrib>Dupré, R</creatorcontrib><creatorcontrib>Elouadrhiri, L</creatorcontrib><creatorcontrib>Fernando, I</creatorcontrib><creatorcontrib>Filippi, A</creatorcontrib><creatorcontrib>est, T</creatorcontrib><creatorcontrib>Girod, F -X</creatorcontrib><creatorcontrib>Gosta, G</creatorcontrib><creatorcontrib>Grames, J</creatorcontrib><creatorcontrib>Gueye, P</creatorcontrib><creatorcontrib>Habet, S</creatorcontrib><creatorcontrib>Hattawy, M</creatorcontrib><creatorcontrib>Higinbotham, D</creatorcontrib><creatorcontrib>Hobart, A</creatorcontrib><creatorcontrib>Hyde, C</creatorcontrib><creatorcontrib>Joo, K</creatorcontrib><creatorcontrib>Kim, A</creatorcontrib><creatorcontrib>Klimenko, V</creatorcontrib><creatorcontrib>Kubarovsky, V</creatorcontrib><creatorcontrib>Leali, M</creatorcontrib><creatorcontrib>Lenisa, P</creatorcontrib><creatorcontrib>Marchand, D</creatorcontrib><creatorcontrib>Marsicano, L</creatorcontrib><creatorcontrib>Mascagna, V</creatorcontrib><creatorcontrib>Matamoros, D</creatorcontrib><creatorcontrib>McCaughan, M</creatorcontrib><creatorcontrib>McKinnon, B</creatorcontrib><creatorcontrib>Migliorati, S</creatorcontrib><creatorcontrib>Mitra, H S</creatorcontrib><creatorcontrib>Movsisyan, A</creatorcontrib><creatorcontrib>Muñoz-Camacho, 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 &amp; 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>
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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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