Browsing by Author "Stoler, P."
Now showing 1 - 4 of 4
- Results Per Page
- Sort Options
- Some of the metrics are blocked by yourconsent settings
Publication Cross Sections for the Exclusive Photon Electroproduction on the Proton and Generalized Parton Distributions(2015-11-17) ;Jo, H. S. ;Girod, F. X. ;Avakian, H. ;Burkert, V. D. ;Garçon, M. ;Guidal, M. ;Kubarovsky, V. ;Niccolai, S. ;Stoler, P. ;Adhikari, K. P. ;Adikaram, D. ;Amaryan, M. J. ;Anderson, M. D. ;Anefalos Pereira, S. ;Ball, J. ;Baltzell, N. A. ;Battaglieri, M. ;Batourine, V. ;Bedlinskiy, I. ;Biselli, A. S. ;Boiarinov, S. ;Briscoe, W. J.; ;Carman, D. S. ;Celentano, A. ;Chandavar, S. ;Charles, G. ;Colaneri, L. ;Cole, P. L. ;Compton, N. ;Contalbrigo, M. ;Crede, V. ;D'Angelo, A. ;Dashyan, N. ;De Vita, R. ;De Sanctis, E. ;Deur, A. ;Djalali, C. ;Dupre, R.; ;Fassi, L. El ;Elouadrhiri, L. ;Fedotov, G. ;Fegan, S. ;Filippi, A. ;Fleming, J. A. ;Garillon, B. ;Gevorgyan, N. ;Ghandilyan, Y. ;Gilfoyle, G. P. ;Giovanetti, K. L. ;Goetz, J. T. ;Golovatch, E. ;Gothe, R. W. ;Griffioen, K. A. ;Guegan, B. ;Guler, N. ;Guo, L. ;Hafidi, K.; ;Harrison, N. ;Hattawy, M. ;Hicks, K. ;Hirlinger Saylor, N. ;Ho, D. ;Holtrop, M. ;Hughes, S. M. ;Ilieva, Y. ;Ireland, D. G. ;Ishkhanov, B. S. ;Jenkins, D. ;Joo, K. ;Joosten, S. ;Keller, D. ;Khachatryan, G. ;Khandaker, M. ;Kim, A. ;Kim, W. ;Klein, A. ;Klein, F. J. ;Kuhn, S. E.; ;Lenisa, P. ;Livingston, K. ;Lu, H. Y. ;Macgregor, I. J.D. ;McKinnon, B. ;Meziani, Z. E. ;Mirazita, M. ;Mokeev, V. ;Montgomery, R. A. ;Moutarde, H. ;Movsisyan, A. ;Munevar, E. ;Munoz Camacho, C. ;Nadel-Turonski, P. ;Net, L. A. ;Niculescu, G. ;Osipenko, M.Ostrovidov, A. I.Unpolarized and beam-polarized fourfold cross sections ðd4σ=dQ2dxBdtdϕÞ for the ep → e0 p0 γ reaction were measured using the CLAS detector and the 5.75-GeV polarized electron beam of the Jefferson Lab accelerator, for 110 (Q2; xB; t) bins over the widest phase space ever explored in the valencequark region. Several models of generalized parton distributions (GPDs) describe the data well at most of our kinematics. This increases our confidence that we understand the GPD H, expected to be the dominant contributor to these observables. Through a leading-twist extraction of Compton form factors, these results support the model predictions of a larger nucleon size at lower quark-momentum fraction xB.Scopus© Citations 87 - Some of the metrics are blocked by yourconsent settings
Publication Measurement of exclusive π0 electroproduction structure functions and their relationship to transverse generalized parton distributions(2012-09-10) ;Bedlinskiy, I. ;Kubarovsky, V. ;Niccolai, S. ;Stoler, P. ;Adhikari, K. P. ;Aghasyan, M. ;Amaryan, M. J. ;Anghinolfi, M. ;Avakian, H. ;Baghdasaryan, H. ;Ball, J. ;Baltzell, N. A. ;Battaglieri, M. ;Bennett, R. P. ;Biselli, A. S. ;Bookwalter, C. ;Boiarinov, S. ;Briscoe, W. J.; ;Burkert, V. D. ;Carman, D. S. ;Celentano, A. ;Chandavar, S. ;Charles, G. ;Contalbrigo, M. ;Crede, V. ;D'Angelo, A. ;Daniel, A. ;Dashyan, N. ;De Vita, R. ;De Sanctis, E. ;Deur, A. ;Djalali, C. ;Doughty, D. ;Dupre, R. ;Egiyan, H. ;El Alaoui, A. ;El Fassi, L. ;Elouadrhiri, L. ;Eugenio, P. ;Fedotov, G. ;Fegan, S. ;Fleming, J. A. ;Forest, T. A. ;Fradi, A. ;Garçon, M. ;Gevorgyan, N. ;Giovanetti, K. L. ;Girod, F. X. ;Gohn, W. ;Gothe, R. W. ;Graham, L. ;Griffioen, K. A. ;Guegan, B. ;Guidal, M. ;Guo, L. ;Hafidi, K.; ;Hanretty, C. ;Heddle, D. ;Hicks, K. ;Holtrop, M. ;Ilieva, Y. ;Ireland, D. G. ;Ishkhanov, B. S. ;Isupov, E. L. ;Jo, H. S. ;Joo, K. ;Keller, D. ;Khandaker, M. ;Khetarpal, P. ;Kim, A. ;Kim, W. ;Klein, F. J. ;Koirala, S. ;Kubarovsky, A. ;Kuhn, S. E.; ;Kvaltine, N. D. ;Livingston, K. ;Lu, H. Y. ;MacGregor, I. J.D. ;Mao, Y. ;Markov, N. ;Martinez, D. ;Mayer, M. ;McKinnon, B. ;Meyer, C. A. ;Mineeva, T. ;Mirazita, M. ;Mokeev, V. ;Moutarde, H. ;Munevar, E. ;Munoz Camacho, C. ;Nadel-Turonski, P. ;Niculescu, G. ;Niculescu, I. ;Osipenko, M. ;Ostrovidov, A. I.Pappalardo, L. L.Exclusive π⁰ electroproduction at a beam energy of 5.75 GeV has been measured with the Jefferson Lab CLAS spectrometer. Differential cross sections were measured at more than 1800 kinematic values in Q², xB, t, and φ, in the Q² range from 1.0 to 4.6 GeV², t up to 2 GeV², and xB from 0.1 to 0.58. Structure functions σT+L, σTT, and σLT were extracted as functions of t for each of 17 combinations of Q² and xB. The data were compared directly with two handbag-based calculations including both longitudinal and transversity generalized parton distributions (GPDs). Inclusion of only longitudinal GPDs very strongly underestimates σT+L and fails to account for σTT and σLT, while inclusion of transversity GPDs brings the calculations into substantially better agreement with the data. There is very strong sensitivity to the relative contributions of nucleon helicity-flip and helicity nonflip processes. The results confirm that exclusive π⁰ electroproduction offers direct experimental access to the transversity GPDs.Scopus© Citations 65 - Some of the metrics are blocked by yourconsent settings
Publication Measurement of unpolarized and polarized cross sections for deeply virtual Compton scattering on the proton at Jefferson Laboratory with CLAS(2018-10-09) ;Hirlinger Saylor, N. ;Guegan, B. ;Burkert, V. D. ;Elouadrhiri, L. ;Garçon, M. ;Girod, F. X. ;Guidal, M. ;Jo, H. S. ;Kubarovsky, V. ;Niccolai, S. ;Stoler, P. ;Adhikari, K. P. ;Adhikari, S. ;Akbar, Z. ;Amaryan, M. J. ;Pereira, S. Anefalos ;Ball, J. ;Balossino, I. ;Baltzell, N. A. ;Barion, L. ;Battaglieri, M. ;Batourine, V. ;Bedlinskiy, I. ;Biselli, A. S. ;Boiarinov, S. ;Briscoe, W. J.; ;Bültmann, S. ;Cao, F. ;Carman, D. S. ;Celentano, A. ;Charles, G. ;Chetry, T. ;Ciullo, G. ;Clary, Brandon A. ;Cole, P. L. ;Contalbrigo, M. ;Cortes, O. ;D'Angelo, A. ;Dashyan, N. ;De Vita, R. ;Defurne, M. ;Deur, A. ;Diehl, S. ;Djalali, C. ;Dupre, R. ;Egiyan, H.; ;Fassi, L. El ;Eugenio, P. ;Fedotov, G. ;Fersch, R. ;Filippi, A. ;Forest, T. A. ;Fradi, A. ;Gavalian, G. ;Gevorgyan, N. ;Ghandilyan, Y. ;Gilfoyle, G. P. ;Giovanetti, K. L. ;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. ;Ilieva, Y. ;Ireland, D. G. ;Ishkhanov, B. S. ;Isupov, E. L. ;Jenkins, D. ;Johnston, S. ;Joo, K. ;Joosten, S. ;Kabir, M. L. ;Keller, D. ;Khachatryan, G. ;Khachatryan, M. ;Khandaker, M. ;Kim, A. ;Kim, W. ;Klein, A. ;Klein, F. J. ;Kuhn, S. E.; ;Lanza, L. ;Lenisa, P. ;Livingston, K. ;Lu, H. Y. ;Macgregor, I. J.D. ;Markov, N.This paper reports the measurement of polarized and unpolarized cross sections for the ep → e'p'γ reaction, which is composed of deeply virtual Compton scattering (DVCS) and Bethe-Heitler (BH) processes, at an electron beam energy of 5.88 GeV at the Thomas Jefferson National Accelerator Facility using the Large Acceptance Spectrometer CLAS. The unpolarized cross sections and polarized cross section differences have been measured over broad kinematics, 0.10 < x_B < 0.58, 1.0 < Q² < 4.8 GeV², and 0.09 < -t < 2.00 GeV². The results are found to be consistent with previous CLAS data, and these new data are discussed in the framework of the generalized parton distribution approach. Calculations with two widely used phenomenological models are approximately compatible with the experimental results over a large portion of the kinematic range of the data.Scopus© Citations 15 - Some of the metrics are blocked by yourconsent settings
Publication Near-threshold neutral pion electroproduction at high momentum transfers and generalized form factors(2013-04-15) ;Khetarpal, P. ;Stoler, P. ;Aznauryan, I. G. ;Kubarovsky, V. ;Adhikari, K. P. ;Adikaram, D. ;Aghasyan, M. ;Amaryan, M. J. ;Anderson, M. D. ;Anefalos Pereira, S. ;Anghinolfi, M. ;Avakian, H. ;Baghdasaryan, H. ;Ball, J. ;Baltzell, N. A. ;Battaglieri, M. ;Batourine, V. ;Bedlinskiy, I. ;Biselli, A. S. ;Bono, J. ;Boiarinov, S. ;Briscoe, W. J.; ;Carman, D. S. ;Celentano, A. ;Charles, G. ;Cole, P. L. ;Contalbrigo, M. ;Crede, V. ;D'Angelo, A. ;Dashyan, N. ;De Vita, R. ;De Sanctis, E. ;Deur, A. ;Djalali, C. ;Doughty, D. ;Dugger, M. ;Dupre, R. ;Egiyan, H. ;El Alaoui, A. ;El Fassi, L. ;Eugenio, P. ;Fedotov, G. ;Fegan, S. ;Fersch, R. ;Fleming, J. A. ;Fradi, A. ;Gabrielyan, M. Y. ;Garçon, M. ;Gevorgyan, N. ;Gilfoyle, G. P. ;Giovanetti, K. L. ;Girod, F. X. ;Goetz, J. T. ;Gohn, W. ;Golovatch, E. ;Gothe, R. W. ;Griffioen, K. A. ;Guegan, B. ;Guidal, M. ;Guo, L. ;Hafidi, K.; ;Hanretty, C. ;Harrison, N. ;Hicks, K. ;Ho, D. ;Holtrop, M. ;Hyde, C. E. ;Ilieva, Y. ;Ireland, D. G. ;Ishkhanov, B. S. ;Isupov, E. L. ;Jo, H. S. ;Joo, K. ;Keller, D. ;Khandaker, M. ;Kim, A. ;Kim, W. ;Klein, F. J. ;Koirala, S. ;Kubarovsky, A.; ;Kvaltine, N. D. ;Lewis, S. ;Livingston, K. ;Lu, H. Y. ;Macgregor, I. J.D. ;Mao, Y. ;Martinez, D. ;Mayer, M. ;McKinnon, B. ;Meyer, C. A. ;Mineeva, T. ;Mirazita, M. ;Mokeev, V. ;Montgomery, R. A. ;Moutarde, H.Munevar, E.We report the measurement of near-threshold neutral pion electroproduction cross sections and the extraction of the associated structure functions on the proton in the kinematic range Q2 from 2 to 4.5 GeV2 and W from 1.08 to 1.16 GeV. These measurements allow us to access the dominant pion-nucleon s-wave multipoles E0+ and S0+ in the near-threshold region. In the light-cone sum-rule framework (LCSR), these multipoles are related to the generalized form factors Gπ0p 1 (Q2) and Gπ0p 2 (Q2). The data are compared to these generalized form factors and the results for Gπ0p 1 (Q2) are found to be in good agreement with the LCSR predictions, but the level of agreement with Gπ0p 2 (Q2) is poor.Scopus© Citations 3
