Differential cross section for γd → ωd using CLAS at Jefferson Lab

Chetry, T.; Hicks, K.; Compton, N.; Sargsian, Misak; Adhikari, S.; Ball, J.; Balossino, I.; Barion, L.; Battaglieri, M.; Batourine, V.; Bedlinskiy, I.; Biselli, A.; Boiarinov, S.; Briscoe, W. J.; Brooks, W. K.; Burkert, V. D.; Carman, D. S.; Celentano, A.; Charles, G.; Ciullo, G.; Clark, L.; Clary, B. A.; Cole, P. L.; Contalbrigo, M.; Credé, V.; D’Angelo, A.; Dashyan, N.; Vita, R. De; Sanctis, E. De; Deur, A.; Djalali, C.; Dupré, R.; Alaoui, A. El; Fassi, L. El; Eugenio, P.; Fedotov, G.; Fersch, R.; Filippi, A.; Gavalian, G.; Ghandilyan, Y.; Giovanetti, K. L.; Girod, F. X.; Golovatch, E.; Gothe, R.; Griffioen, K. A.; Guo, L.; Hafidi, K.; Harrison, N.; Hattawy, M.; Holtrop, M.; Ilieva, Y.; Ireland, D. G.; Ишханов, Б. С.; Isupov, E. L.; Jenkins, D.; Johnston, S.; Kabir, Latiful; Keller, D.; Khachatryan, G.; Khachatryan, M.; Khandaker, M.; Kim, A.; Kim, W.; Klein, F. J.; Kubarovsky, V.; Lanza, L.; Lenisa, P.; Livingston, K.; MacGregor, I. J. D.; Markov, N.; McKinnon, B.; Mokeev, V.; Movsisyan, A.; Camacho, C. Muñoz; Nadel-Turoński, P.; Niccolai, S.; Niculescu, G.; Osipenko, M.; Ostrovidov, A. I.; Paolone, M.; Paremuzyan, R.; Park, K.; Pasyuk, E.; Phelps, W.; Pogorelko, O.; Price, J. W.; Prok, Y.; Ripani, M.; Riser, D.; Ritchie, B. G.; Rizzo, A.; Rosner, G.; Salgado, C.; Schumacher, R. A.; Skorodumina, Iu.; Smith, G. D.; Sober, D. I.; Sokhan, D.; Sparveris, N.; Stepanyan, S.; Strakovsky, I. I.; Strauch, S.; Taiuti, M.; Tan, J. A.; Ungaro, M.; Voskanyan, H.; Voutier, E.; Weinstein, L. B.; Wood, M. H.; Zachariou, N.; Zhang, J.; Zhao, Z. W.

doi:10.1016/j.physletb.2018.06.003

Cited by 3 publications

(2 citation statements)

References 15 publications

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“…The energy dependent values of s f t N have been evaluated using the experimentally determined values of ( ) [20,42] and α fN = − 0.3 [34] in equation (13).…”

Section: Resultsmentioning

confidence: 99%

“…Beyond the resonance region, the coherent vector mesons production in the nuclear reaction has been used to investigate various features of these mesons in the nucleus. The coherent photoproductions of the ω and f mesons from the deuteron at high momentum transfer region could not be explained by the single scattering of the meson but they are realized by the double scattering of the meson [13,14]. The interference of the ρ 0 and ω mesons (coherently photoproduced from the nucleus) in the semi-hadronic decay channel demonstrates the enhancement in the cross section away from the peak region [15].…”

Section: Introductionmentioning

confidence: 95%

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Forward coherent ω and ϕ mesons production in the photonuclear reaction on nuclei

Das¹

2021

Phys. Scr.

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The differential cross sections of the forward coherent ω and φ mesons photoproduction from nuclei have been calculated using the Glauber model for the nuclear reaction. The measured cross section of the elementary reaction, i.e., γN → ω(φ)N reaction, are used as input in the Glauber model. The experimentally determined free-space scattering parameters of the quoted mesons have been used to evaluate the meson nucleus interactions. The sensitivity of the cross section to the Fermimotion of the nucleon and the nucleon-nucleon short-range correlation in the nucleus are studied. The calculated results are compared with the measured cross sections.

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“…The energy dependent values of s f t N have been evaluated using the experimentally determined values of ( ) [20,42] and α fN = − 0.3 [34] in equation (13).…”

Section: Resultsmentioning

confidence: 99%