Browsing by Author "Badui, R. A."
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Publication Measurement of two-photon exchange effect by comparing elastic e±p cross sections(2017-06-01) ;Rimal, D. ;Adikaram, D. ;Raue, B. A. ;Weinstein, L. B. ;Arrington, J. ;Brooks, W. K. ;Ungaro, M. ;Adhikari, K. P. ;Afanasev, A. V. ;Akbar, Z. ;Pereira, S. Anefalos ;Badui, R. A. ;Ball, J. ;Baltzell, N. A. ;Battaglieri, M. ;Batourine, V. ;Bedlinskiy, I. ;Biselli, A. S. ;Boiarinov, S. ;Briscoe, W. J. ;Bültmann, S. ;Burkert, V. D. ;Carman, D. S. ;Celentano, A. ;Chetry, T. ;Ciullo, G. ;Clark, L. ;Colaneri, L. ;Cole, P. L. ;Compton, N. ;Contalbrigo, M. ;Cortes, O. ;Crede, V. ;D'Angelo, A. ;Dashyan, N. ;De Vita, R. ;Deur, A. ;Djalali, C. ;Dupre, R. ;Egiyan, H.; ;Fassi, L. El ;Eugenio, P. ;Fanchini, E. ;Fedotov, G. ;Fersch, R. ;Filippi, A. ;Fleming, J. A. ;Forest, T. A. ;Fradi, A. ;Gevorgyan, N. ;Ghandilyan, Y. ;Gilfoyle, G. P. ;Giovanetti, K. L. ;Girod, F. X. ;Gleason, C. ;Gohn, W. ;Golovatch, E. ;Gothe, R. W. ;Griffioen, K. A. ;Guo, L. ;Hafidi, K. ;Hanretty, C. ;Harrison, N. ;Hattawy, M. ;Heddle, D. ;Hicks, K. ;Holtrop, M. ;Hughes, S. M. ;Ilieva, Y. ;Ireland, D. G. ;Ishkhanov, B. S. ;Isupov, E. L. ;Jenkins, D. ;Jiang, H. ;Joosten, S. ;Keller, D. ;Khachatryan, G. ;Khandaker, M. ;Kim, W. ;Klein, A. ;Klein, F. J. ;Kubarovsky, V. ;Kuhn, S. E.; ;Lanza, L. ;Lenisa, P. ;Livingston, K. ;Lu, H. Y. ;Macgregor, I. J.D. ;Markov, N. ;McKinnon, B. ;Mestayer, M. D. ;Mirazita, M. ;Mokeev, V. ;Movsisyan, A. ;Munevar, E. ;Camacho, C. Munoz ;Nadel-Turonski, P.Ni, A.The electromagnetic form factors of the proton measured by unpolarized and polarized electron scattering experiments show a significant disagreement that grows with the squared four-momentum transfer (Q²). Calculations have shown that the two measurements can be largely reconciled by accounting for the contributions of two-photon exchange (TPE). TPE effects are not typically included in the standard set of radiative corrections since theoretical calculations of the TPE effects are highly model dependent, and, until recently, no direct evidence of significant TPE effects has been observed. We measured the ratio of positron-proton to electron-proton elastic-scattering cross sections in order to determine the TPE contribution to elastic electron-proton scattering and thereby resolve the proton electric form factor discrepancy. We produced a mixed simultaneous electron-positron beam in Jefferson Lab’s Hall B by passing the 5.6-GeV primary electron beam through a radiator to produce a bremsstrahlung photon beam and then passing the photon beam through a converter to produce electron-positron pairs. The mixed electron-positron (lepton) beam with useful energies from approximately 0.85 to 3.5 GeV then struck a 30-cm-long liquid hydrogen (LH₂) target located within the CEBAF Large Acceptance Spectrometer (CLAS). By detecting both the scattered leptons and the recoiling protons, we identified and reconstructed elastic scattering events and determined the incident lepton energy. A detailed description of the experiment is presented. We present previously unpublished results for the quantity R₂γ, the TPE correction to the elastic-scattering cross section, at Q² ≈ 0.85 and 1.45 GeV² over a large range of virtual photon polarization ε. Our results, along with recently published results from VEPP-3, demonstrate a nonzero contribution from TPE effects and are in excellent agreement with the calculations that include TPE effects and largely reconcile the form-factor discrepancy up to Q² ≈ 2 GeV². These data are consistent with an increase in R₂γ with decreasing ε at Q² ≈ 0.85 and 1.45 GeV². There are indications of a slight increase in R₂γ with Q².Scopus© Citations 51 - Some of the metrics are blocked by yourconsent settings
Publication Target and beam-target spin asymmetries in exclusive pion electroproduction for Q2>1 GeV2. II. ep→eπ0p TARGET and BEAM-TARGET SPIN .... II. ... P. E. BOSTED et al.(2017-03-20) ;Bosted, P. E. ;Kim, A. ;Adhikari, K. P. ;Adikaram, D. ;Akbar, Z. ;Amaryan, M. J. ;Anefalos Pereira, S. ;Avakian, H. ;Badui, R. A. ;Ball, J. ;Balossino, I. ;Battaglieri, M. ;Bedlinskiy, I. ;Biselli, A. S. ;Boiarinov, S. ;Briscoe, W. J.; ;Bültmann, S. ;Burkert, V. D. ;Cao, T. ;Carman, D. S. ;Celentano, A. ;Chandavar, S. ;Charles, G. ;Chetry, T. ;Ciullo, G. ;Clark, L. ;Colaneri, L. ;Cole, P. L. ;Contalbrigo, M. ;Cortes, O. ;Crede, V. ;D'Angelo, A. ;Dashyan, N. ;De Vita, R. ;De Sanctis, E. ;Deur, A. ;Djalali, C. ;Dupre, R. ;Egiyan, H.; ;El Fassi, L. ;Elouadrhiri, L. ;Eugenio, P. ;Fanchini, E. ;Fedotov, G. ;Fegan, S. ;Fersch, R. ;Filippi, A. ;Fleming, J. A. ;Forest, T. A. ;Fradi, A. ;Ghandilyan, Y. ;Gilfoyle, G. P. ;Girod, F. X. ;Glazier, D. I. ;Gohn, W. ;Golovatch, E. ;Gothe, R. W. ;Griffioen, K. A. ;Guidal, M. ;Guler, N.; ;Guo, L. ;Hafidi, K. ;Hanretty, C. ;Harrison, N. ;Hattawy, M. ;Heddle, D. ;Hicks, K. ;Hollis, G. ;Holtrop, M. ;Hughes, S. M. ;Ireland, D. G. ;Isupov, E. L. ;Jenkins, D. ;Jiang, H. ;Jo, H. S. ;Joo, K. ;Keller, D. ;Khachatryan, G. ;Khandaker, M. ;Kim, W. ;Klei, A. ;Klein, F. J. ;Koirala, S. ;Kubarovsky, V. ;Kuhn, S. E. ;Lanza, L. ;Lenisa, P. ;Livingston, K. ;Lu, H. Y. ;Macgregor, I. J.D. ;Markov, N. ;Mayer, M. ;McCracken, M. E. ;McKinnon, B.; ;Mirazita, M.Mokeev, V. I.Beam-target double-spin asymmetries and target single-spin asymmetries were measured for the exclusive π⁰ electroproduction reaction γp → pπ⁰, expanding an analysis of the γp → nπ⁺ reaction from the same experiment. The results were obtained from scattering of 6-GeV longitudinally polarized electrons off longitudinally polarized protons using the CEBAF Large Acceptance Spectrometer at Jefferson Laboratory. The kinematic ranges covered are 1.1 < W < 3 GeV and 1 < Q² < 6 GeV². Results were obtained for about 5700 bins in W, Q², cos(θ*), and φ*. The beam-target asymmetries were found to generally be greater than zero, with relatively modest φ* dependence. The target asymmetries exhibit very strong φ* dependence, with a change in sign occurring between results at low W and high W, in contrast to π⁺ electroproduction. Reasonable agreement is found with phenomenological fits to previous data for W < 1.6 GeV, but significant differences are seen at higher W. When combined with cross-sectional measurements, as well as π⁺ observables, the present results will provide powerful constraints on nucleon resonance amplitudes at moderate and large values of Q², for resonances with masses as high as 2.4 GeV.Scopus© Citations 12
