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Bosted, P. E.,Biselli, A. S.,Careccia, S.,Dodge, G.,Fersch, R.,Guler, N.,Kuhn, S. E.,Pierce, J.,Prok, Y.,Zheng, X.,Adhikari, K. P.,Adikaram, D.,Akbar, Z.,Amaryan, M. J.,Anefalos Pereira, S.,Asryan, G. American Physical Society 2016 Physical Review C Vol.94 No.5
<P>Beam-target double-spin asymmetries and target single-spin asymmetries in exclusive pi(+) and quasiexclusive pi(-) electroproduction were obtained from scattering of 1.6- to 5.7-GeV longitudinally polarized electrons from longitudinally polarized protons (for pi(+)) and deuterons (for pi(-)) using the CEBAF Large Acceptance Spectrometer (CLAS) at Jefferson Lab. The kinematic range covered is 1.1 < W < 2.6 GeV and 0.05 < Q(2) < 5 GeV2, with good angular coverage in the forward hemisphere. The asymmetry results were divided into approximately 40 000 kinematic bins for pi(+) from free protons and 15 000 bins for pi(-) production from bound nucleons in the deuteron. The present results are found to be in reasonable agreement with fits to previous world data for W < 1.7 GeV and Q(2) < 0.5 GeV2, with discrepancies increasing at higher values of Q(2), especially for W > 1.5 GeV. Very large target-spin asymmetries are observed for W > 1.6 GeV. When combined with cross-section measurements, the present results can provide powerful constraints on nucleon resonance amplitudes at moderate and large values of Q(2), for resonances with masses as high as 2.3 GeV.</P>
Beam-spin asymmetries from semi-inclusive pion electroproduction
Gohn, W.,Avakian, H.,Joo, K.,Ungaro, M.,Adhikari, K. P.,Aghasyan, M.,Amaryan, M. J.,Anderson, M. D.,Anefalos Pereira, S.,Ball, J.,Baltzell, N. A.,Battaglieri, M.,Biselli, A. S.,Bono, J.,Briscoe, W. J. American Physical Society 2014 PHYSICAL REVIEW D - Vol.89 No.7
Photoproduction ofπ+π−meson pairs on the proton
Battaglieri, M.,De Vita, R.,Szczepaniak, A. P.,Adhikari, K. P.,Amaryan, M. J.,Anghinolfi, M.,Baghdasaryan, H.,Bedlinskiy, I.,Bellis, M.,Bibrzycki, L.,Biselli, A. S.,Bookwalter, C.,Branford, D.,Briscoe American Physical Society 2009 PHYSICAL REVIEW D - Vol.80 No.7
Photoproduction of the<sub>f1</sub>(1285)meson
Dickson, R.,Schumacher, R. A.,Adhikari, K. P.,Akbar, Z.,Amaryan, M. J.,Anefalos Pereira, S.,Badui, R. A.,Ball, J.,Battaglieri, M.,Batourine, V.,Bedlinskiy, I.,Biselli, A.,Boiarinov, S.,Briscoe, W. J. American Physical Society 2016 Physical Review C Vol.93 No.6
<P>The f(1)(1285) meson withmass 1281.0 +/- 0.8MeV/c(2) and width 18.4 +/- 1.4MeV (full width at half maximum) was measured for the first time in photoproduction from a proton target using CLAS at Jefferson Lab. Differential cross sections were obtained via the eta pi(+)pi(-), K+(K) over bar (0) pi(-), and (K-K0)pi(+) decay channels from threshold up to a center-of-mass energy of 2.8 GeV. The mass, width, and an amplitude analysis of the eta pi(+)pi(-) final-state Dalitz distribution are consistent with the axial-vector J(P) = 1(+) f(1)(1285) identity, rather than the pseudoscalar 0(-) eta(1295). The production mechanism is more consistent with s-channel decay of a high-mass N* state and not with t-channel meson exchange. Decays to eta pi pi go dominantly via the intermediate a(0)(+/-) (980)pi(-/+) states, with the branching ratio Gamma [a(0)pi (no (K) over barK)]/Gamma[eta pi pi (all)] = 0.74 +/- 0.09. The branching ratios Gamma (K (K) over bar pi)/Gamma(eta pi pi) = 0.216 +/- 0.033 and Gamma (gamma rho(0))/Gamma(eta pi pi) = 0.047 +/- 0.018 were also obtained. The first is in agreement with previous data for the f(1)(1285), while the latter is lower than the world average.</P>
Bosted, P. E.,Amaryan, M. J.,Anefalos Pereira, S.,Avakian, H.,Badui, R. A.,Ball, J.,Baltzell, N. A.,Battaglieri, M.,Batourine, V.,Bedlinskiy, I.,Biselli, A. S.,Briscoe, W. J.,Bü,ltmann, S.,Burkert American Physical Society 2017 Physical Review C Vol.95 No.3
<P>Beam-target double-spin asymmetries and target single-spin asymmetries were measured for the exclusive pi(+) electroproduction reaction. gamma(*) p -> n pi(+). The results were obtained from scattering of 6-GeV longitudinally polarized electrons off longitudinally polarized protons using the CEBAF Large Acceptance Spectrometer at Jefferson Laboratory. The kinematic range covered is 1.1 < W < 3 GeV and 1 < Q(2) < 6 GeV2. Results were obtained for about 6000 bins in W, Q(2), cos(theta(*)), and phi(*). Except at forward angles, very large target-spin asymmetries are observed over the entire W region. Reasonable agreement is found with phenomenological fits to previous data for W < 1.6 GeV, but very large differences are seen at higher values of W. A generalized parton distributions (GPD)-based model is in poor agreement with the data. When combined with cross-sectional measurements, the present results provide powerful constraints on nucleon resonance amplitudes at moderate and large values of Q(2), for resonances with masses as high as 2.4 GeV.</P>
Kim, A.,Avakian, H.,Burkert, V.,Joo, K.,Kim, W.,Adhikari, K.P.,Akbar, Z.,Anefalos Pereira, S.,Badui, R.A.,Battaglieri, M.,Batourine, V.,Bedlinskiy, I.,Biselli, A.S.,Boiarinov, S.,Bosted, P.,Briscoe, W North-Holland Pub. Co 2017 Physics letters. Section B Vol.768 No.-
<P><B>Abstract</B></P> <P>The target and double spin asymmetries of the exclusive pseudoscalar channel e → p → → e p <SUP> π 0 </SUP> were measured for the first time in the deep-inelastic regime using a longitudinally polarized 5.9 GeV electron beam and a longitudinally polarized proton target at Jefferson Lab with the CEBAF Large Acceptance Spectrometer (CLAS). The data were collected over a large kinematic phase space and divided into 110 four-dimensional bins of <SUP> Q 2 </SUP> , <SUB> x B </SUB> , −<I>t</I> and <I>ϕ</I>. Large values of asymmetry moments clearly indicate a substantial contribution to the polarized structure functions from transverse virtual photon amplitudes. The interpretation of experimental data in terms of generalized parton distributions (GPDs) provides the first insight on the chiral-odd GPDs <SUB> H ˜ T </SUB> and <SUB> E T </SUB> , and complement previous measurements of unpolarized structure functions sensitive to the GPDs <SUB> H T </SUB> and <SUB> E ¯ T </SUB> . These data provide a crucial input for parametrizations of essentially unknown chiral-odd GPDs and will strongly influence existing theoretical calculations based on the handbag formalism.</P>