Exclusive electroproduction of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>φ</mml:mi></mml:math>mesons at 4.2 GeV

Lukashin, K.; Smith, E. S.; Adams, G. S.; Anciant, E.; Anghinolfi, M.; Asavapibhop, B.; Audit, G.; Auger, T.; Avakian, H.; Ball, J.; Barrow, S.; Battaglieri, M.; Beard, K.; Bektasoglu, M.; Bertozzi, W.; Bianchi, N.; Biselli, A.; Boiarinov, S.; Bonner, B. E.; Bouchigny, S.; Branford, D.; Briscoe, W. J.; Brooks, W. K.; Burkert, Volker; Calarco, J. R.; Carman, D. S.; Carnahan, B.; Ciciani, L.; Clark, Robert Beck; Cole, P. L.; Coleman, Alan; Cords, D.; Corvisiero, P.; Crabb, D.; Crannell, H.; Cummings, J. P.; Degtiarenko, Pavel; Dennis, L.; Sanctis, E. De; DeVita, R.; Dhuga, K. S.; Djalali, C.; Dodge, G. E.; Domingo, J.; Doughty, D.; Dragovitsch, P.; Dytman, S.; Eckhause, M.; Egiyan, H.; Egiyan, K. S.; Elouadrhiri, L.; Empl, A.; Fatemi, R.; Feuerbach, R. J.; Ficenec, J.; Fissum, Kevin; Forest, T. A.; Freyberger, A.; Funsten, H. O.; Gaff, S. J.; Gai, M.; Gavalian, G.; Gilad, S.; Gilfoyle, G. P.; Giovanetti, K. L.; Girard, Pascal; Griffioen, K. A.; Guidal, M.; Guillo, M.; Gyurjyan, V.; Hardie, J.; Heddle, D.; Hersman, F. W.; Hicks, K.; Hicks, R. S.; Holtrop, M.; Hu, J. F.; Hyde‐Wright, C. E.; Ito, M. M.; Jenkins, D.; Joo, K.; Kelley, J. H.; Khandaker, M.; Kim, K.; Kim, K. Y.; Kim, W.; Klein, A.; Klein, Frank; Klusman, M.; Kossov, M.; Kramer, L. H.; Kuhn, S. E.; Laget, J. M.; Lawrence, D.; Longhi, A.; Manak, J. J.; Marchand, Claude; McAleer, S.; McCarthy, J.; McNabb, J. W.; Mecking, B. A.; Mestayer, M. D.; Meyer, C. A.; Mikhailov, K.; Minehart, R.; Mirazita, M.; Miskimen, R.; Muccifora, V.; Muêller, J.; Mutchler, G. S.; Napolitano, J.; Nelson, S. O.; Niculescu, G.; Niculescu, I.; Niczyporuk, B. B.; Niyazov, R. A.; Opper, A. K.; O’Rielly, G. V.; O’Brien, J. T.; Park, K.; Paschke, K.; Pasyuk, E.; Peterson, G. A.; Philips, S. A.; Pivnyuk, N.; Počanić, D.; Pogorelko, O.; Polli, E.; Pozdniakov, S.; Preedom, B. M.; Price, J. W.; Qin, L. M.; Raue, B. A.; Reolon, A. R.; Riccardi, G.; Ricco, G.; Ripani, M.; Ritchie, B. G.; Ronchetti, F.; Rossi, P.; Rowntree, D.; Rubin, P. D.; Sabatié, F.; Sabourov, K.; Salgado, C.; Sapunenko, V.; Schumacher, R. A.; Serov, V. S.; Sharabian, Y. G.; Shaw, J.; Simionatto, S.; Skabelin, A. V.; Smith, L. C.; Sober, D. I.; Stavinsky, A.; Stepanyan, S.; Stoler, P.; Strakovsky, I. I.; Taiuti, M.; Taylor, S.; Tedeschi, D. J.; Thompson, R.; Vineyard, M. F.; Vlassov, A. V.; Wang, K.; Weller, H.R.; Weinstein, Lawrence; Welsh, R. E.; Weygand, D. P.; Whisnant, S.; Wolin, E.; Yanik, L.; Yegneswaran, A.; Yun, Jaeseok; Zhao, J.; Zhang, B.; Zhou, Zhengfang

doi:10.1103/physrevc.63.065205

Cited by 20 publications

(5 citation statements)

References 34 publications

Supporting

Mentioning

Contrasting

Order By: Relevance

“…For light vector mesons, Q 2 ranges from Q 2 =0 GeV 2 up to 100 GeV 2 in the high W domain, where there are data from the H1 [33,34,35], ZEUS [36,37,38,39,40,41,42] and HERMES [43] (HERA) and E665 (Fermilab) [44] experiments. At low W , experiments at CORNELL [45] and with the CLAS detector at Jefferson Lab [46,47,48,49,50] have measured the ρ 0 , ω and φ electroproduction channels up to Q 2 =5 GeV 2 . For the heavy mesons, there are electroproduction data only for the J/Ψ from HERA [51,54]; otherwise, there are photoproduction data coming from the H1 [52], ZEUS [53], LHCb [55,56,57,58] and ALICE [59] experiments and a few fixed target data at low energies.…”

Section: The Parametrization Of the Gpdsmentioning

confidence: 99%

Deeply virtual meson production on the nucleon

et al. 2016

Self Cite

View full text Add to dashboard Cite

show abstract

Section: The Parametrization Of the Gpdsmentioning

confidence: 99%

Deeply virtual meson production on the nucleon

et al. 2016

Self Cite

View full text Add to dashboard Cite

show abstract

“…The CLAS collaboration has published results for ρ 0 production at x B = 0.31 and at x B = 0.38, with Q 2 values between 1.5 and 2.3 GeV 2 [14], and for φ production at x B = 0.29 and Q 2 = 1.7 GeV 2 [50]. We consider that this kinematics, where the hadronic invariant mass W is below 2.3 GeV, is too close to threshold for comparison with a leading-twist calculation.…”

Section: Comparison With Data and Discussion Of Power Correctionsmentioning

confidence: 99%

Exclusive channels in semi-inclusive production of pions and kaons

et al. 2005

View full text Add to dashboard Cite

We investigate the role of exclusive channels in semi-inclusive electroproduction of pions and kaons. Using the QCD factorization theorem for hard exclusive processes we evaluate the cross sections for exclusive pseudoscalar and vector meson production in terms of generalized parton distributions and meson distribution amplitudes. We investigate the uncertainties arising from the modeling of the nonperturbative input quantities. Combining these results with available experimental data, we compare the cross sections for exclusive channels to that obtained from quark fragmentation in semi-inclusive deep inelastic scattering. We find that ρ 0 production is the only exclusive channel with significant contributions to semiinclusive pion production at large z and moderate Q 2 . The corresponding contribution to kaon production from the decay of exclusively produced φ and K * is rather small.

show abstract

“…For more information on the world data. See references: CLAS [45,46], Cornell [47,48], HERMES [49], NMC [50], ZEUS [51], and H1 [52]. [25].…”

Section: Experimental Statusmentioning

confidence: 99%

“…The parametrization in W and Q 2 used for cross-section calculation for φ production off a proton target plotted against world data. For more information on the world data, see references: CLAS [45,46], Cornell [47,48], HERMES [49], NMC [50], ZEUS [51], and H1 [52]. Reproduced from [25] Chapter 3…”

Section: Experimental Statusmentioning

confidence: 99%

Partonic Structure of Light Nuclei

Armstrong¹,

Arrington²,

Cloët³

et al. 2017

Preprint

View full text Add to dashboard Cite

In this run group, we propose a comprehensive physics program to investigate the fundamental structure of the 4 He nucleus. An important focus of this program is on the coherent exclusive Deep Virtual Compton Scattering (DVCS) and Deep Virtual Meson Production (DVMP) with emphasis on φ meson production. These are particularly powerful tools enabling model-independent nuclear 3D tomography through the access of partons' position in the transverse plane. These exclusive measurements will give the chance to compare directly the quark and gluon radii of the helium nucleus. Another important measurement proposed in this program is the study of the partonic structure of bound nucleons. To this end, we propose next generation nuclear measurements in which low energy recoil nuclei are detected. The tagging of recoil nuclei in deep inelastic reactions is a powerful technique, which will provide unique information about the nature of medium modifications through the measurement of the EMC ratio and its dependence on the nucleon off-shellness. Finally, we propose to measure incoherent spectator-tagged DVCS on light nuclei (d, 4 He) where the observables are sensitive to the Generalized Parton Distributions (GPDs) of a quasi-free neutron for the case of the deuteron, and bound proton and neutron for the case of 4 He. The objective is to study and separate nuclear effects and their manifestation in GPDs. The fully exclusive kinematics provide a novel approach for studying final state interactions in the measurements of the beam spin asymmetries and the off-forward EMC ratio.At the heart of this program is the Low Energy Recoil Tracker (ALERT) combined with the CLAS12 detector. The ALERT detector is composed of a stereo drift chamber for track reconstruction and an array of scintillators for particle identification. Coupling these two types of fast detectors will allow ALERT to be included in the trigger for efficient † Contact Person: Kawtar Hafidi

show abstract

Exclusive electroproduction ofφmesons at 4.2 GeV

Cited by 20 publications

References 34 publications

Deeply virtual meson production on the nucleon

Deeply virtual meson production on the nucleon

Exclusive channels in semi-inclusive production of pions and kaons

Partonic Structure of Light Nuclei

Contact Info

Product

Resources

About