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Hakobyan, Hayk
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Hakobyan, Hayk
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Campus / Sede
Campus Casa Central Valparaíso
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Now showing 1 - 10 of 23
- PublicationExclusive photoproduction of π0 up to large values of Mandelstam variables s, t, and u with CLAS(2018-07-25)
;Kunkel, M. C. ;Amaryan, M. J. ;Strakovsky, I. I. ;Ritman, J. ;Goldstein, G. R. ;Adhikari, K. P. ;Adhikari, S. ;Avakian, H. ;Ball, J. ;Balossino, I. ;Barion, L. ;Battaglieri, M. ;Batourine, V. ;Bedlinskiy, I. ;Biselli, A. S. ;Boiarinov, S. ;Briscoe, W. J.; ;Bültmann, S. ;Burkert, V. D. ;Cao, F. ;Carman, D. S. ;Celentano, A. ;Charles, G. ;Chetry, T. ;Ciullo, G. ;Clark, L. ;Cole, P. L. ;Contalbrigo, M. ;Cortes, O. ;Crede, V. ;D'Angelo, A. ;Dashyan, N. ;De Vita, R. ;De Sanctis, E. ;Degtyarenko, P. V. ;Defurne, M. ;Deur, A. ;Djalali, C. ;Dugger, M. ;Dupre, R. ;Egiyan, H.; ;El Fassi, L. ;Elouadrhiri, L. ;Eugenio, P. ;Fedotov, G. ;Fersch, R. ;Filippi, A. ;Fradi, A. ;Gavalian, G. ;Ghandilyan, Y. ;Ghosh, S. ;Gilfoyle, G. P. ;Giovanetti, K. L. ;Girod, F. X. ;Glazier, D. I. ;Gohn, W. ;Golovatch, E. ;Gothe, R. W. ;Griffioen, K. A. ;Guo, L. ;Guidal, M. ;Hafidi, K.; ;Harrison, N. ;Hattawy, M. ;Hicks, K. ;Holtrop, M. ;Hyde, C. E. ;Ireland, D. G. ;Ishkhanov, B. S. ;Isupov, E. L. ;Jenkins, D. ;Joo, K. ;Kabir, M. L. ;Keller, D. ;Khachatryan, G. ;Khachatryan, M. ;Khandaker, M. ;Kim, A. ;Kim, W. ;Klein, A. ;Klein, F. ;Kubarovsky, V. ;Kuhn, S. E. ;Laget, J. M. ;Lanza, L. ;Lenisa, P. ;Lersch, D. ;Livingston, K. ;Macgregor, I. J.D. ;Markov, N. ;Mbianda Njencheu, G. ;McKinnon, B.; ;Mokeev, V. ;Montgomery, R. A. ;Movsisyan, A.Munoz Camacho, C.Exclusive photoproduction cross sections have been measured for the process γp → pπ0[e+e−(γ )] with the Dalitz decay final state using tagged photon energies in the range of Eγ = 1.275–5.425 GeV. The complete angular distribution of the final state π0, for the entire photon energy range up to large values of t and u, has been measured for the first time. The data obtained show that the cross section dσ/dt, at mid to large angles, decreases with energy as s−6.89±0.26. This is in agreement with the perturbative QCD quark counting rule prediction of s−7. Paradoxically, the size of angular distribution of measured cross sections is greatly underestimated by the QCD-based generalized parton distribution mechanism at highest available invariant energy s = 11 GeV2 . At the same time, the Regge-exchange-based models for π0 photoproduction are more consistent with experimental data. - PublicationMeasurement of the beam asymmetry Σ for π0 and η photoproduction on the proton at Eγ=9 GeV(2017-04-24)
;Al Ghoul, H. ;Anassontzis, E. G. ;Austregesilo, A. ;Barbosa, F. ;Barnes, A. ;Beattie, T. D. ;Bennett, D. W. ;Berdnikov, V. V. ;Black, T. ;Boeglin, W. ;Briscoe, W. J.; ;Cannon, B. E. ;Chernyshov, O. ;Chudakov, E. ;Crede, V. ;Dalton, M. M. ;Deur, A. ;Dobbs, S. ;Dolgolenko, A. ;Dugger, M. ;Dzhygadlo, R. ;Egiyan, H. ;Eugenio, P. ;Fanelli, C. ;Foda, A. M. ;Frye, J. ;Furletov, S. ;Gan, L. ;Gasparian, A. ;Gerasimov, A. ;Gevorgyan, N. ;Goetzen, K. ;Goryachev, V. S. ;Guo, L.; ;Hardin, J. ;Henderson, A. ;Huber, G. M. ;Ireland, D. G. ;Ito, M. M. ;Jarvis, N. S. ;Jones, R. T. ;Kakoyan, V. ;Kamel, M. ;Klein, F. J. ;Kliemt, R. ;Kourkoumeli, C.; ;Kuznetsov, I. ;Lara, M. ;Larin, I. ;Lawrence, D. ;Levine, W. I. ;Livingston, K. ;Lolos, G. J. ;Lyubovitskij, V. ;Mack, D. ;Mattione, P. T. ;Matveev, V. ;McCaughan, M. ;McCracken, M. ;McGinley, W. ;McIntyre, J. ;Mendez, R. ;Meyer, C. A. ;Miskimen, R. ;Mitchell, R. E. ;Mokaya, F. ;Moriya, K. ;Nerling, F. ;Nigmatkulov, G. ;Ochoa, N. ;Ostrovidov, A. I. ;Papandreou, Z. ;Patsyuk, M. ;Pedroni, R. ;Pennington, M. R. ;Pentchev, L. ;Peters, K. J. ;Pooser, E. ;Pratt, B. ;Qiang, Y. ;Reinhold, J. ;Ritchie, B. G. ;Robison, L. ;Romanov, D. ;Salgado, C. ;Schumacher, R. A. ;Schwarz, C. ;Schwiening, J. ;Semenov, A. Yu ;Semenova, I. A. ;Seth, K. K. ;Shepherd, M. R. ;Smith, E. S. ;Sober, D. I. ;Somov, A. ;Somov, S.Soto, O.We report measurements of the photon beam asymmetry for the reactions γ p → pπ0 and γ p → pη from the GLUEX experiment using a 9 GeV linearly polarized, tagged photon beam incident on a liquid hydrogen target in Jefferson Lab’s Hall D. The asymmetries, measured as a function of the proton momentum transfer, possess greater precision than previous π0 measurements and are the first η measurements in this energy regime. The results are compared with theoretical predictions based on t-channel, quasiparticle exchange and constrain the axial-vector component of the neutral meson production mechanism in these models. - PublicationMeasurement of the beam asymmetry Σ and the target asymmetry T in the photoproduction of ω mesons off the proton using CLAS at Jefferson Laboratory(2018-05-04)
;Roy, P. ;Akbar, Z. ;Park, S. ;Crede, V. ;Anisovich, A. V. ;Denisenko, I. ;Klempt, E. ;Nikonov, V. A. ;Sarantsev, A. V. ;Adhikari, K. P. ;Adhikari, S. ;Anefalos Pereira, S. ;Ball, J. ;Balossino, I. ;Bashkanov, M. ;Battaglieri, M. ;Batourine, V. ;Bedlinskiy, I. ;Biselli, A. S. ;Boiarinov, S. ;Briscoe, W. J. ;Brock, J.; ;Burkert, V. D. ;Carlin, C. ;Carman, D. S. ;Celentano, A. ;Charles, G. ;Chetry, T. ;Ciullo, G. ;Clary, B. A. ;Cole, P. L. ;Contalbrigo, M. ;D'Angelo, A. ;Dashyan, N. ;De Vita, R. ;Deur, A. ;Djalali, C. ;Dugger, M. ;Dupre, R.; ;El Fassi, L. ;Elouadrhiri, L. ;Eugenio, P. ;Fedotov, G. ;Fegan, S. ;Filippi, A. ;Fradi, A. ;Gavalian, G. ;Gevorgyan, N. ;Gilfoyle, G. P. ;Giovanetti, K. L. ;Girod, F. X. ;Gleason, C. ;Gohn, W. ;Golovatch, E. ;Gothe, R. W. ;Griffioen, K. A. ;Guidal, M. ;Guo, L. ;Hafidi, K.; ;Hanretty, C. ;Hattawy, M. ;Hicks, K. ;Holtrop, M. ;Ilieva, Y. ;Ireland, D. G. ;Ishkhanov, B. S. ;Isupov, E. L. ;Jenkins, D. ;Joo, K. ;Joosten, S. ;Keith, C. D. ;Keller, D. ;Khachatryan, G. ;Khandaker, M. ;Kim, A. ;Kim, W. ;Klein, A. ;Klein, F. J. ;Kubarovsky, V.; ;Lanza, L. ;Lenisa, P. ;Livingston, K. ;Lu, H. Y. ;Macgregor, I. J.D. ;Markov, N. ;Mayer, M. ;McCracken, M. E. ;McKinnon, B. ;Meekins, D. G. ;Meyer, C. A. ;Meziani, Z. E.; ;Mokeev, V. ;Montgomery, R. A. ;Movsisyan, A.Munoz Camacho, C.The photoproduction of ω mesons off the proton has been studied in the reaction γp → p ω using the CEBAF Large Acceptance Spectrometer (CLAS) and the frozen-spin target in Hall B at the Thomas Jefferson National Accelerator Facility. For the first time, the target asymmetry T has been measured in photoproduction from the decay ω → π+π−π0, using a transversely polarized target with energies ranging from just above the reaction threshold up to 2.8 GeV. Significant nonzero values are observed for these asymmetries, reaching about 30–40% in the third-resonance region. New measurements for the photon-beam asymmetry are also presented, which agree well with previous CLAS results and extend the world database up to 2.1 GeV. These data and additional ω photoproduction observables from CLAS were included in a partial-wave analysis within the Bonn-Gatchina framework. Significant contributions from s-channel resonance production were found in addition to t-channel exchange processes.Scopus© Citations 10 - PublicationLongitudinal target-spin asymmetries for deeply virtual compton scattering(2015-01-22)
;Seder, E. ;Biselli, A. ;Pisano, S. ;Niccolai, S. ;Smith, G. D. ;Joo, K. ;Adhikari, K. ;Amaryan, M. J. ;Anderson, M. D. ;Anefalos Pereira, S. ;Avakian, H. ;Battaglieri, M. ;Bedlinskiy, I. ;Bono, J. ;Boiarinov, S. ;Bosted, P. ;Briscoe, W. ;Brock, J.; ;Bültmann, S. ;Burkert, V. D. ;Carman, D. S. ;Carlin, C. ;Celentano, A. ;Chandavar, S. ;Charles, G. ;Colaneri, L. ;Cole, P. L. ;Contalbrigo, M. ;Crabb, D. ;Crede, V. ;D'Angelo, A. ;Dashyan, N. ;De Vita, R. ;De Sanctis, E. ;Deur, A. ;Djalali, C. ;Doughty, D. ;Dupre, R. ;El Fassi, L. ;Elouadrhiri, L. ;Eugenio, P. ;Fedotov, G. ;Fegan, S. ;Filippi, A. ;Fleming, J. A. ;Fradi, A. ;Garillon, B. ;Garçon, M. ;Gevorgyan, N. ;Ghandilyan, Y. ;Giovanetti, K. L. ;Girod, F. X. ;Goetz, J. T. ;Gohn, W. ;Gothe, R. W. ;Griffioen, K. A. ;Guegan, B. ;Guidal, M. ;Guo, L. ;Hafidi, K.; ;Hanretty, C. ;Harrison, N. ;Hattawy, M. ;Hirlinger Saylor, N. ;Holtrop, M. ;Hughes, S. M. ;Ilieva, Y. ;Ireland, D. G. ;Ishkhanov, B. S. ;Isupov, E. L. ;Jo, H. S. ;Joosten, S. ;Keith, C. D. ;Keller, D. ;Khachatryan, G. ;Khandaker, M. ;Kim, A. ;Kim, W. ;Klein, A. ;Klein, F. J. ;Koirala, S. ;Kubarovsky, V. ;Kuhn, S. E. ;Lenisa, P. ;Livingston, K. ;Lu, H. Y. ;Macgregor, I. J.D. ;Markov, N. ;Mayer, M. ;McKinnon, B. ;Meekins, D. G.; ;Mirazita, M. ;Mokeev, V. ;Montgomery, R. ;Moody, C. I. ;Moutarde, H.Movsisyan, A.A measurement of the electroproduction of photons off protons in the deeply inelastic regime was performed at Jefferson Lab using a nearly 6 GeV electron beam, a longitudinally polarized proton target, and the CEBAF Large Acceptance Spectrometer. Target-spin asymmetries for ep → e0 p0 γ events, which arise from the interference of the deeply virtual Compton scattering and the Bethe-Heitler processes, were extracted over the widest kinematics in Q2, xB, t, and ϕ, for 166 four-dimensional bins. In the framework of generalized parton distributions, at leading twist the t dependence of these asymmetries provides insight into the spatial distribution of the axial charge of the proton, which appears to be concentrated in its center. These results also bring important and necessary constraints for the existing parametrizations of chiral-even generalized parton distributions.Scopus© Citations 48 - PublicationBeam–target helicity asymmetry E in K+Σ− photoproduction on the neutron(2020-09-10)
;Zachariou, N. ;Watts, D. P. ;Fleming, J. ;Sarantsev, A. V. ;Nikonov, V. A. ;D'Angelo, A. ;Bashkanov, M. ;Hanretty, C. ;Kageya, T. ;Klein, F. J. ;Lowry, M. ;Lu, H. ;Sandorfi, A. ;Wei, X. ;Zonta, I. ;Adhikari, K. P. ;Adhikari, S. ;Amaryan, M. J. ;Angelini, G. ;Asryan, G. ;Atac, H. ;Barion, L. ;Bass, C. ;Battaglieri, M. ;Bedlinskiy, I. ;Benmokhtar, F. ;Bianconi, A. ;Biselli, A. S. ;Bossù, F. ;Boiarinov, S. ;Briscoe, W. J.; ;Bulumulla, D. ;Burkert, V. ;Carman, D. S. ;Carvajal, J. C. ;Celentano, A. ;Charles, G. ;Chatagnon, P. ;Chetry, T. ;Ciullo, G. ;Cole, P. L. ;Contalbrigo, M. ;Dashyan, N. ;De Vita, R. ;Deur, A. ;Diehl, S. ;Djalali, C. ;Dupre, R. ;Egiyan, H. ;Ehrhart, M.; ;Eugenio, P. ;Fegan, S. ;Fersch, R. ;Filippi, A. ;Gavalian, G. ;Gevorgyan, N. ;Ghandilyan, Y. ;Gilfoyle, G. P. ;Girod, F. X. ;Gohn, W. ;Golovatch, E. ;Gothe, R. W. ;Griffioen, K. A. ;Guidal, M. ;Hafidi, K.; ;Hattawy, M. ;Heddle, D. ;Hicks, K. ;Ho, D. ;Holtrop, M. ;Ilieva, Y. ;Ireland, D. G. ;Ishkhanov, B. S. ;Isupov, E. L. ;Jenkins, D. ;Jo, H. S. ;Joo, K. ;Joosten, S. J. ;Keller, D. ;Khachatryan, M. ;Khanal, A. ;Khandaker, M. ;Kim, C. W. ;Kim, W. ;Kubarovsky, V. ;Lanza, L. ;Leali, M. ;Lenisa, P. ;Livingston, K. ;MacGregor, I. J.D. ;Marchand, D. ;Markov, N. ;Marsicano, L. ;Mascagna, V. ;Mayer, M.; Soto, O.We report a measurement of a beam–target double-polarisation observable (E) for the γn(p) → K +−(p) reaction. The data were obtained impinging the circularly-polarised energy-tagged photon beam of Hall B at Jefferson Lab on a longitudinally-polarised frozen-spin hydrogen deuteride (HD) nuclear target. The E observable for an effective neutron target was determined for centre-of-mass energies 1.70 ≤ W ≤ 2.30 GeV, with reaction products detected over a wide angular acceptance by the CLAS spectrometer. These new double-polarisation data give unique constraints on the strange decays of excited neutron states. Inclusion of the new data within the Bonn-Gatchina theoretical model results in significant changes for the extracted photocouplings of a number of established nucleon resonances. Possible improvements in the PWA description of the experimental data with additional “missing” resonance states, including the N(2120)3/2− resonance, are also quantified.Scopus© Citations 8 - PublicationNear-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 2 - PublicationReconstruction of 400 GeV/c proton interactions with the SHiP-charm project(2024-06-01)
;Ahdida, C. ;Akmete, A. ;Bieschke, S. ;Borburgh, J. ;Chumakov, A. ;Cornelis, K. ;D’Ambrosio, N. ;D’Appollonio, G. ;de Asmundis, R. ;De Carvalho Saraiva, J. ;Di Giulio, L.; ;Dijkstra, H. ;Dougherty, L. A. ;Drohan, V. ;Durhan, O. ;Ehlert, M. ;Elikkaya, E. ;Graverini, E. ;Grenard, J. L.; ; Lyubovitskij, V.AbstractThe SHiP-charm project was proposed to measure the associated charm production induced by 400 GeV/c protons in a thick target, including the contribution from cascade production. An optimisation run was performed in July 2018 at CERN SPS using a hybrid setup. The high resolution of nuclear emulsions acting as vertex detector was complemented by electronic detectors for kinematic measurements and muon identification. Here we present first results on the analysis of nuclear emulsions exposed in the 2018 run, which prove the capability of reconstructing proton interaction vertices in a harsh environment, where the signal is largely dominated by secondary particles produced in hadronic and electromagnetic showers within the lead target. - PublicationCross 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 85 - PublicationImproved Λp Elastic Scattering Cross Sections between 0.9 and 2.0 GeV/c as a Main Ingredient of the Neutron Star Equation of State(2021-12-31)
;Rowley, J. ;Compton, N. ;Djalali, C. ;Hicks, K. ;Price, J. ;Zachariou, N. ;Adhikari, K. P. ;Armstrong, W. R. ;Atac, H. ;Baashen, L. ;Barion, L. ;Bashkanov, M. ;Battaglieri, M. ;Bedlinskiy, I. ;Benmokhtar, F. ;Bianconi, A. ;Biondo, L. ;Biselli, A. S. ;Bondi, M. ;Bossù, F. ;Boiarinov, S. ;Briscoe, W. J.; ;Bulumulla, D. ;Burkert, V. D. ;Carman, D. S. ;Carvajal, J. C. ;Celentano, A. ;Chatagnon, P. ;Chesnokov, V. ;Chetry, T. ;Ciullo, G. ;Clark, L. ;Cole, P. L. ;Contalbrigo, M. ;Costantini, G. ;Crede, V. ;D'Angelo, A. ;Dashyan, N. ;De Vita, R. ;Defurne, M. ;Deur, A. ;Diehl, S. ;Dupré, R. ;Egiyan, H. ;Ehrhart, M.; ;El Fassi, L. ;Eugenio, P. ;Fedotov, G. ;Fegan, S. ;Fersch, R. ;Filippi, A. ;Fradi, A. ;Gavalian, G. ;Girod, F. X. ;Glazier, D. I. ;Golubenko, A. ;Gothe, R. W. ;Griffioen, K. ;Guo, L. ;Hafidi, K.; ;Hattawy, M. ;Hayward, T. B. ;Heddle, D. ;Hobart, A. ;Holtrop, M. ;Ilieva, Y. ;Ireland, D. G. ;Isupov, E. L. ;Jenkins, D. ;Jo, H. S. ;Joo, K. ;Keller, D. ;Khanal, A. ;Khandaker, M. ;Kim, A. ;Korover, I. ;Kripko, A. ;Kubarovsky, V. ;Kuhn, S. E. ;Lanza, L. ;Leali, M. ;Lenisa, P. ;Livingston, K. ;Macgregor, I. J.D. ;Marchand, D. ;Markov, N. ;Marsicano, L. ;Mascagna, V. ;McCracken, M. E. ;McKinnon, B. ;McLauchlin, C. ;Meziani, Z. E. ;Migliorati, S.; ;Mirazita, M. ;Mokeev, V.Munevar, E.Strange matter is believed to exist in the cores of neutron stars based on simple kinematics. If this is true, then hyperon-nucleon interactions will play a significant part in the neutron star equation of state. Yet, compared to other elastic scattering processes, there is very little data on Λ-N scattering. This experiment utilized the CEBAF Large Acceptance Spectrometer (CLAS) detector to study the Λp → Λp elastic scattering cross section in the incident Λ momentum range 0.9–2.0 GeV=c. These are the first data on this reaction since the 1970s. The new cross sections have significantly better accuracy and precision than the existing world data, and the techniques developed here can also be used in future experiments.Scopus© Citations 26 - PublicationDouble KS0 photoproduction off the proton at CLAS(2018-02-26)
;Chandavar, S. ;Goetz, J. T. ;Hicks, K. ;Keller, D. ;Kunkel, M. C. ;Paolone, M. ;Weygand, D. P. ;Adhikari, K. P. ;Adhikari, S. ;Akbar, Z. ;Ball, J. ;Balossino, I. ;Barion, L. ;Bashkanov, M. ;Battaglieri, M. ;Bedlinskiy, I. ;Biselli, A. S. ;Briscoe, W. J.; ;Burkert, V. D. ;Cao, F. ;Carman, D. S. ;Celentano, A. ;Charles, G. ;Chetry, T. ;Ciullo, G. ;Clark, L. ;Cole, P. L. ;Contalbrigo, M. ;Crede, V. ;D'Angelo, A. ;Dashyan, N. ;De Vita, R. ;De Sanctis, E. ;Defurne, M. ;Deur, A. ;Djalali, C. ;Dupre, R. ;Egiyan, H.; ;El Fassi, L. ;Eugenio, P. ;Fedotov, G. ;Filippi, A. ;Fradi, A. ;Gavalian, G. ;Ghandilyan, Y. ;Gilfoyle, G. P. ;Girod, F. X. ;Glazier, D. I. ;Gohn, W. ;Golovatch, E. ;Gothe, R. W. ;Griffioen, K. A. ;Guidal, M. ;Guo, L. ;Hafidi, K.; ;Hanretty, C. ;Harrison, N. ;Hattawy, M. ;Heddle, D. ;Holtrop, M. ;Ilieva, Y. ;Ireland, D. G. ;Isupov, E. L. ;Jenkins, D. ;Johnston, S. ;Joo, K. ;Joosten, S. ;Kabir, M. L. ;Khachatryan, G. ;Khachatryan, M. ;Khandaker, M. ;Kim, W. ;Klein, A. ;Klein, F. J. ;Kubarovsky, V. ;Lanza, L. ;Lenisa, P. ;Livingston, K. ;MacGregor, I. J.D. ;Markov, N. ;McCracken, M. E. ;McKinnon, B. ;Meyer, C. A.; ;Mokeev, V. ;Movsisyan, A. ;Munoz Camacho, C. ;Nadel-Turonski, P. ;Niccolai, S. ;Niculescu, G. ;Osipenko, M. ;Ostrovidov, A. I. ;Paremuzyan, R. ;Park, K. ;Pasyuk, E. ;Phelps, W.Pogorelko, O.The f0(1500) meson resonance is one of several contenders to have significant mixing with the lightest glueball. This resonance is well established from several previous experiments. Here we present the first photoproduction data for the f0(1500) via decay into the K0 SK0 S channel using the CLAS detector. The reaction γp → fJp → K0 SK0 Sp, where J = 0,2, was measured with photon energies from 2.7–5.1 GeV. A clear peak is seen at 1500 MeV in the background subtracted invariant mass spectra of the two kaons. This is enhanced if the measured fourmomentum transfer to the proton target is restricted to be less than 1.0 GeV2 . By comparing data with simulations, it can be concluded that the peak at 1500 MeV is produced primarily at low t, which is consistent with a t-channel production mechanism.Scopus© Citations 8
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