Upper limits for the photoproduction cross section for the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mi>Φ</mml:mi><mml:mrow><mml:mo>−</mml:mo><mml:mo>−</mml:mo></mml:mrow></mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:mn>1860</mml:mn><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:math>pentaquark state off the deuteron

Egiyan, H.; Langheinrich, J.; Gothe, R. W.; Graham, L.; Holtrop, M.; Lu, H. Y.; Mattione, P.; Mutchler, G. S.; Park, K.; Smith, E. S.; Zhao, Z. W.; Adhikari, K. P.; Aghasyan, M.; Anghinolfi, M.; Baghdasaryan, H.; Ball, J.; Baltzell, N. A.; Battaglieri, M.; Bedlinskiy, I.; Bennett, R.; Biselli, A.; Bookwalter, C.; Branford, D.; Briscoe, W. J.; Brooks, W. K.; Burkert, V. D.; Carman, D. S.; Celentano, A.; Chandavar, S.; Contalbrigo, M.; D’Angelo, A.; Daniel, A.; Dashyan, N.; Vita, R. De; Sanctis, E. De; Deur, A.; Dey, B.; Dickson, R.; Djalali, C.; Doughty, D.; Dupré, R.; Alaoui, A. El; Fassi, L. El; Eugenio, P.; Fedotov, G.; Fegan, S.; Fradi, A.; Gabrielyan, M.; Gevorgyan, N.; Gilfoyle, G. P.; Giovanetti, K. L.; Girod, F. X.; Goetz, J. T.; Gohn, W.; Golovatch, E.; Griffioen, K. A.; Guidal, M.; Guler, N.; Guo, L.; Gyurjyan, V.; Hafidi, K.; Hakobyan, H.; Hanretty, C.; Heddle, D.; Hicks, K.; Ilieva, Y.; Ireland, D. G.; Ишханов, Б. С.; Jo, H. S.; Joo, K. S.; Khetarpal, P.; Kim, A.; Kim, W.; Klein, A.; Klein, F. J.; Kubarovsky, V.; Kuleshov, S.; Livingston, K.; MacGregor, I. J. D.; Mao, Y.; Mayer, Martin; McKinnon, B.; Mokeev, V.; Munévar, E.; Nadel-Turoński, P.; Ni, A.; Niculescu, G.; Ostrovidov, A. I.; Paolone, M.; Pappalardo, L. L.; Paremuzyan, R.; Park, S.; Pasyuk, E.; Pereira, S. Anefalos; Phelps, E.; Pogorelko, O.; Pozdniakov, S.; Price, J. W.; Procureur, S.; Protopopescu, D.; Raue, B. A.; Ricco, G.; Rimal, D.; Ripani, M.; Ritchie, Barry; Rosner, G.; Rossi, P.; Sabatié, F.; Saini, M. S.; Salgado, C.; Schott, D.; Schumacher, R. A.; Seder, E.; Seraydaryan, H.; Sharabian, Y. G.; Smith, G. D.; Sober, D. I.; Stepanyan, S.; Strauch, S.; Taiuti, M.; Tang, W.; Taylor, C.; Tedeschi, D. J.; Ungaro, M.; Voutier, E.; Watts, D. P.; Weinstein, L. B.; Weygand, D. P.; Wood, M. H.; Zachariou, N.; Zana, L.; Zhao, B.

doi:10.1103/physrevc.85.015205

Cited by 4 publications

(2 citation statements)

References 45 publications

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“…The electron beam is deflected in the magnetic field of the tagging system after it passed through a radiator with a nominal thickness of 5x10 4 radiation length. The standard electron beam current was chosen to be 30 nA, and it was limited by the drift chamber performance [1]. The trigger required a hit in the tagger in the energy range from 4.5 to 5.5 GeV.…”

Section: Discussionmentioning

confidence: 99%

Study of the two pion final state photoproduction on deuterium

Graham¹,

Park²,

Gothe³

et al. 2010

AIP Conference Proceedings

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Understanding the structure of baryons in terms of the fundamental interaction of the constituent quarks and gluons is one of the challenges in strong interaction physics. This interaction is governed by Quantum Chromodynamics (QCD). However, solutions of this theory in the non-perturbative domain of the interaction are extremely difficult to achieve. In inelastic electron scattering, very little is known about exclusive hadron production purely contributed to a lack of knowledge. The γN interaction is recognized for being a powerful method for investigating hadrons and the mysteries that still exist within the strong interaction. From reactions with the nucleon, the strong interaction can be tested through the amplitudes of the N and ∆ resonances. More specifically, if an electromagnetic interaction is well known then the intermediate resonance states may be evaluated through pion photoproduction. To gain more detailed insight into this interaction, we look to probe the baryon structure of ∆ and the meson structure of the pion through photon scattering off a deuteron producing two pions in the final state. The photoproduction processes on the deuteron will be used to investigate known baryon resonances in the proton-pion channel. The two pion final state will be investigated for unraveling new information in to the rho decay at threshold. We want to explore both final states interactions to search for "missing" states that are predicted by quark models but have not yet been found experimentally. Using the CEBAF Large Acceptance Spectrometer (CLAS), the hadronic products are detected in coincidence with the scattered photon. This makes it possible to measure the differential cross section and the decay angular distribution for the production of two and three pion final states. The measured cross sections will contribute significantly and push the knowledge of the strong interaction to the next level. We propose to use the CEBAF Large Acceptance Spectrometer (CLAS) to study the two pion channel from the EG3 data set, for ∆ ++ (1232) production. We look to investigate the exclusive reaction of γd→pπ + π-(n), extracting the relevant cross sections to comparable data sets. This reaction is produced using a high intensity photon beam incident on a deuterium target. These measurements provide unique and coherent results from tagged photons over a broad range of energy, and represent the only pion production data above 5 GeV at this present time.

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Section: Discussionmentioning

confidence: 99%

Study of the two pion final state photoproduction on deuterium

Graham¹,

Park²,

Gothe³

et al. 2010

AIP Conference Proceedings

View full text Add to dashboard Cite

show abstract

“…Leptons, for which as for quarks there are six different mass eigenstates, can be observed as quasi-free particles in nature, while quarks almost exclusively appear as constituents of bound states (hadrons); due to confinement any observable state in the SM must not carry any net colour charge, such that baryons (consisting of three quarks or three anti-quarks) and mesons (one quark and one anti-quark) are the only bound states of quarks that have been observed so far. The SM does also allow bound states with more constituents -pentaquarks, for instancebut the experimental evidence for such states is controversial [28,29,30,31,32,33]. There are no known bound states with top-quarks because their average lifetime is much smaller than the hadronisation time.…”

Section: Particle Contentmentioning

confidence: 99%