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Virtual Compton scattering on the proton has been investigated at three yet unexplored values of the four-momentum transfer $Q^2$: 0.10, 0.20 and 0.45 GeV$^2$, at the Mainz Microtron. Fits performed using either the low-energy theorem or dispersion r...
Virtual Compton scattering on the proton has been investigated at three yet unexplored values of the four-momentum transfer $Q^2$: 0.10, 0.20 and 0.45 GeV$^2$, at the Mainz Microtron. Fits performed using either the low-energy theorem or dispersion r...
Alcorn, J.;Anderson, B.D.;Aniol, K.A.;Annand, J.R.M.;Auerbach, L.;Arrington, J.;Averett, T.;Baker, F.T.;Baylac, M.;Beise, E.J.;Berthot, J.;Bertin, P.Y.;Bertozzi, W.;Bimbot, L.;Black, T.;Boeglin, W.U.;Boykin, D.V.;Brash, E.J.;Breton, V.;Breuer, H.;Brindza, P.;Brown, D.;Burtin, E.;Calarco, J.R.;Cardman, L.S.;Carr, R.;Cates, G.D.;Cavata, C.;Chai, Z.;Chang, C.C.;Chant, N.S.;Chen, J.P.;Choi, S.;Chudakov, E.;Churchwell, S.;Coman, M.;Cisbani, E.;Colilli, S.;Colombel, N.;Crateri, R.;Dale, D.S.;Degrande, N.;de Jager, C.W.;De Leo, R.;Deur, A.;Dezern, G.;Diederich, B.;Dieterich, S.;di Salvo, R.;Djawotho, P.;Domingo, J.;Ducret, J.E.;Dutta, D.;Egiyan, K.;Epstein, M.B.;Escoffier, S.;Esp, S.;Ewell, L.A.;Finn, J.M.;Fissum, K.G.;Folts, E.;Fonvieille, H.;Frois, B.;Frullani, S.;Gao, H.;Gao, J.;Garibaldi, F.;Gasparian, A.;Gavalya, A.;Gayou, O.;Gilad, S.;Gilman, R.;Giuliani, F.;Glamazdin, A.;Glashausser, C.;Gomez, J.;Gorbenko, V.;Gorringe, T.;Gricia, M.;Griffioen, K.;Hamilton, David;Hansen, J.O.;Hersman, F.W.;Higinbotham, D.W.;Holmes, R.;Holmgren, H.;Holtrop, M.;d'Hose, N.;Hovhannisyan, E.;Howell, C.;Huber, G.M.;Hughes, E.;Hyde-Wright, C.E.;Ibrahim, H.;Incerti, S.;Iodice, M.;Iommi, R.;Ireland, D.;Jaminion, S.;Jardillier, J.;Jensen, S.;Jiang, X.;Jones, C.E.;Jones, M.K.;Joo, K.;Jutier, C.;Kahl, W.;Kato, S.;Katramatou, A.T.;Kelly, J.J.;Kerhoas, S.;Ketikyan, A.;Khandaker, M.;Khayat, M.;Kino, K.;Kominis, I.;Korsch, W.;Kox, S.;Kramer, K.;Kumar, K.S.;Kumbartzki, G.;Kuss, M.;Lagamba, L.;Laveissiere, G.;Leone, A.;Lerose, J.J.;Marie, F.;Levchuk, L.;Leuschner, M.;Lhuillier, D.;Liang, M.;Livingston, K.;Lindgren, R.A.;Liyanage, N.;Lolos, G.J.;Lourie, R.W.;Lucentini, M.;Madey, R.;Maeda, K.;Malov, S.;Manley, D.M.;Margaziotis, D.J.;Markowitz, P.;Marroncle, J.;Martine, J.;Mayilyan, S.;McCarthy, J.S.;McCormick, K.;McIntyre, J.;McKeown, R.D.;Meekins, D.;van der Meer, R.L.J.;Meziani, Z.E.;Michaels, R.;Milbrath, B.;Miller, J.A.;Miller, W.;Mitchell, J.;Mougey, J.;Nanda, S.;Nathan, A.;Neyret, D.;Offermann, E.A.J.M.;Papandreou, Z.;Perdrisat, C.F.;Perrino, R.;Petratos, G.G.;Petrosyan, A.;Pierangeli, L.;Platchkov, S.;Pomatsalyuk, R.;Pripstein, D.;Prout, D.L.;Punjabi, V.A.;Pussieux, T.;Quemener, G.;Ransomez, R.D.;Ravel, O.;Reitz, B.;Roblin, Y.;Roche, R.;Roedelbronn, M.;Rondon-Aramayo, O.A.;Roos, P.G.;Rosner, G.;Rowntree, D.;Rutledge, G.A.;Rutt, P.M.;Rvachev, M.;Sabatavenere, F.;Saha, A.;Saito, T.;Santavenere, F.;Sarty, A.J.;Schneider, W.J.;Segal, J.P.;Serdarevic-Offermann, A.;Shahinyan, A.;Slifer, K.;Smith, T.P.;Soldi, A.;Sorokin, P.;Souder, P.;Spiegel, S.L.;Stevens, M.A.;Strauch, S.;Suleiman, R.;Templon, J.A.;Terasawa, T.;Todor, L.;Tsubota, H.;Ueno, H.;Ulmer, P.E.;Urciuoli, G.M.;Van Hoorebeke, L.;Van de Vyver, R.;van Verst, S.;Vernin, P.;Vlahovic, B.;Voskanyan, H.;Voutier, E.;Walter, R.;Watson, J.W.;Watts, D.P.;Weinstein, L.B.;Wijesooriya, K.;Wojtsekhowski, B.;Xiang, H.;Xiong, F.;Xu, W.;Zainea, D.G.;Zeps, V.;Zhao, J.;Zheng, X.;Zhou, Z.L.;Zhu, L.;Zolnierczuk, P.A.
The instrumentation in Hall A at the Thomas Jefferson National Accelerator Facility was designed to study electro-and photo- induced reactions at very high luminosity and good momentum and angular resolution for at least one of the reaction products....
The ratio of the electric and magnetic form factors of the proton G(Ep)/G(Mp), which is an image of its charge and magnetization distributions, was measured at the Thomas Jefferson National Accelerator Facility (JLab) using the recoil polarization te...
The beam-recoil double polarization Ph x0 and Ph z0 and the recoil polarization Py0 were measured for the first time for the pe~ ; e0p~ reaction at a four-momentum transfer of Q2 0:1 GeV2=c2 and a center of mass production angle of 120 at the Mainz M...
Virtual Compton scattering on the proton has been investigated at three yet unexplored values of the four-momentum transfer $Q^2$: 0.10, 0.20 and 0.45 GeV$^2$, at the Mainz Microtron. Fits performed using either the low-energy theorem or dispersion r...
International audience