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1. Strong interaction physics at the luminosity frontier with 22 GeV electrons at Jefferson Lab

Author

Accardi, A, Achenbach, P, Adhikari, D, Afanasev, A, Akondi, CS, Akopov, N, Albaladejo, M, Albataineh, H, Albrecht, M, Almeida-Zamora, B, Amaryan, M, Androić, D, Armstrong, W, Armstrong, DS, Arratia, M, Arrington, J, Asaturyan, A, Austregesilo, A, Avakian, H, Averett, T, Gayoso, C Ayerbe, Bacchetta, A, Balantekin, AB, Baltzell, N, Barion, L, Barry, PC, Bashir, A, Battaglieri, M, Bellini, V, Belov, I, Benhar, O, Benkel, B, Benmokhtar, F, Bentz, W, Bertone, V, Bhatt, H, Bianconi, A, Bibrzycki, L, Bijker, R, Binosi, D, Biswas, D, Boër, M, Boeglin, W, Bogacz, SA, Boglione, M, Bondí, M, Boos, EE, Bosted, P, Bozzi, G, Brash, EJ, Briceño, RA, Brindza, PD, Briscoe, WJ, Brodsky, SJ, Brooks, WK, Burkert, VD, Camsonne, A, Cao, T, Cardman, LS, Carman, DS, Carpinelli, M, Cates, GD, Caylor, J, Celentano, A, Celiberto, FG, Cerutti, M, Chang, L, Chatagnon, P, Chen, C, Chen, J-P, Chetry, T, Christopher, A, Christy, E, Chudakov, E, Cisbani, E, Cloët, IC, Cobos-Martinez, JJ, Cohen, EO, Colangelo, P, Cole, PL, Constantinou, M, Contalbrigo, M, Costantini, G, Cosyn, W, Cotton, C, Courtoy, A, Dusa, S Covrig, Crede, V, Cui, Z-F, D’Angelo, A, Döring, M, Dalton, MM, Danilkin, I, Davydov, M, Day, D, De Fazio, F, De Napoli, M, De Vita, R, Dean, DJ, and Defurne, M

Subjects
Nuclear and Plasma Physics, Particle and High Energy Physics, Synchrotrons and Accelerators, Physical Sciences, Atomic, Molecular, Nuclear, Particle and Plasma Physics, Nuclear & Particles Physics, Nuclear and plasma physics, Particle and high energy physics, Synchrotrons and accelerators
Published
2024

2. Measurement of the J/ψ photoproduction cross section over the full near-threshold kinematic region

Author

Adhikari, S, Afzal, F, Akondi, CS, Albrecht, M, Amaryan, M, Arroyave, V, Asaturyan, A, Austregesilo, A, Baldwin, Z, Barbosa, F, Barlow, J, Barriga, E, Barsotti, R, Beattie, TD, Berdnikov, VV, Black, T, Boeglin, W, Briscoe, WJ, Britton, T, Brooks, WK, Byer, D, Chudakov, E, Cole, PL, Cortes, O, Crede, V, Dalton, MM, Darulis, D, Deur, A, Dobbs, S, Dolgolenko, A, Dotel, R, Dugger, M, Dzhygadlo, R, Ebersole, D, Egiyan, H, Erbora, T, Eugenio, P, Fabrizi, A, Fanelli, C, Fang, S, Fegan, S, Fitches, J, Foda, AM, Furletov, S, Gan, L, Gao, H, Gardner, A, Gasparian, A, Gleason, C, Goetzen, K, Goryachev, VS, Grube, B, Guo, J, Guo, L, Hague, TJ, Hakobyan, H, Hernandez, J, Hoffman, ND, Hornidge, D, Hou, G, Huber, GM, Hurck, P, Hurley, A, Imoehl, W, Ireland, DG, Ito, MM, Jaegle, I, Jarvis, NS, Jeske, T, Jones, RT, Kakoyan, V, Kalicy, G, Khachatryan, V, Khatchatryan, M, Kourkoumelis, C, LaDuke, A, Larin, I, Lawrence, D, Lersch, DI, Li, H, Li, WB, Liu, B, Livingston, K, Lolos, GJ, Lorenti, L, Lyubovitskij, V, Mack, D, Mahmood, A, Martel, PP, Marukyan, H, Matveev, V, McCaughan, M, McCracken, M, Meyer, CA, Miskimen, R, Mitchell, RE, Mizutani, K, Neelamana, V, Ng, L, and Nissen, E

Subjects
Nuclear and Plasma Physics, Particle and High Energy Physics, Physical Sciences, Nuclear and plasma physics
Abstract

We report the total and differential cross sections for J/ψ photoproduction with the large acceptance GlueX spectrometer for photon beam energies from the threshold at 8.2 GeV up to 11.44 GeV and over the full kinematic range of momentum transfer squared, t. Such coverage facilitates the extrapolation of the differential cross sections to the forward (t=0) point beyond the physical region. The forward cross section is used by many theoretical models and plays an important role in understanding J/ψ photoproduction and its relation to the J/ψ-proton interaction. These measurements of J/ψ photoproduction near threshold are also crucial inputs to theoretical models that are used to study important aspects of the gluon structure of the proton, such as the gluon generalized parton distribution of the proton, the mass radius of the proton, and the trace anomaly contribution to the proton mass. We observe possible structures in the total cross section energy dependence and find evidence for contributions beyond gluon exchange in the differential cross section close to threshold, both of which are consistent with contributions from open-charm intermediate states.

Published
2023

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Author

Adhikari, S, Adhikari, S, Afzal, F, Akondi, CS, Albrecht, M, Amaryan, M, Arroyave, V, Asaturyan, A, Austregesilo, A, Baldwin, Z, Barbosa, F, Barlow, J, Barriga, E, Barsotti, R, Beattie, TD, Berdnikov, VV, Black, T, Boeglin, W, Briscoe, WJ, Britton, T, Brooks, WK, Byer, D, Chudakov, E, Cole, PL, Cortes, O, Crede, V, Dalton, MM, Darulis, D, Deur, A, Dobbs, S, Dolgolenko, A, Dotel, R, Dugger, M, Dzhygadlo, R, Ebersole, D, Egiyan, H, Erbora, T, Eugenio, P, Fabrizi, A, Fanelli, C, Fang, S, Fegan, S, Fitches, J, Foda, AM, Furletov, S, Gan, L, Gao, H, Gardner, A, Gasparian, A, Gleason, C, Goetzen, K, Goryachev, VS, Grube, B, Guo, J, Guo, L, Hague, TJ, Hakobyan, H, Hernandez, J, Hoffman, ND, Hornidge, D, Hou, G, Huber, GM, Hurck, P, Hurley, A, Imoehl, W, Ireland, DG, Ito, MM, Jaegle, I, Jarvis, NS, Jeske, T, Jones, RT, Kakoyan, V, Kalicy, G, Khachatryan, V, Khatchatryan, M, Kourkoumelis, C, LaDuke, A, Larin, I, Lawrence, D, Lersch, DI, Li, H, Li, WB, Liu, B, Livingston, K, Lolos, GJ, Lorenti, L, Lyubovitskij, V, Mack, D, Mahmood, A, Martel, PP, Marukyan, H, Matveev, V, McCaughan, M, McCracken, M, Meyer, CA, Miskimen, R, Mitchell, RE, Mizutani, K, Neelamana, V, Ng, L, Nissen, E, Adhikari, S, Adhikari, S, Afzal, F, Akondi, CS, Albrecht, M, Amaryan, M, Arroyave, V, Asaturyan, A, Austregesilo, A, Baldwin, Z, Barbosa, F, Barlow, J, Barriga, E, Barsotti, R, Beattie, TD, Berdnikov, VV, Black, T, Boeglin, W, Briscoe, WJ, Britton, T, Brooks, WK, Byer, D, Chudakov, E, Cole, PL, Cortes, O, Crede, V, Dalton, MM, Darulis, D, Deur, A, Dobbs, S, Dolgolenko, A, Dotel, R, Dugger, M, Dzhygadlo, R, Ebersole, D, Egiyan, H, Erbora, T, Eugenio, P, Fabrizi, A, Fanelli, C, Fang, S, Fegan, S, Fitches, J, Foda, AM, Furletov, S, Gan, L, Gao, H, Gardner, A, Gasparian, A, Gleason, C, Goetzen, K, Goryachev, VS, Grube, B, Guo, J, Guo, L, Hague, TJ, Hakobyan, H, Hernandez, J, Hoffman, ND, Hornidge, D, Hou, G, Huber, GM, Hurck, P, Hurley, A, Imoehl, W, Ireland, DG, Ito, MM, Jaegle, I, Jarvis, NS, Jeske, T, Jones, RT, Kakoyan, V, Kalicy, G, Khachatryan, V, Khatchatryan, M, Kourkoumelis, C, LaDuke, A, Larin, I, Lawrence, D, Lersch, DI, Li, H, Li, WB, Liu, B, Livingston, K, Lolos, GJ, Lorenti, L, Lyubovitskij, V, Mack, D, Mahmood, A, Martel, PP, Marukyan, H, Matveev, V, McCaughan, M, McCracken, M, Meyer, CA, Miskimen, R, Mitchell, RE, Mizutani, K, Neelamana, V, Ng, L, and Nissen, E

Published
2023

4. Upper Limit on the Photoproduction Cross Section of the Spin-Exotic π_{1}(1600).

Author

Afzal F, Akondi CS, Albrecht M, Amaryan M, Arrigo S, Arroyave V, Asaturyan A, Austregesilo A, Baldwin Z, Barbosa F, Barlow J, Barriga E, Barsotti R, Barton D, Baturin V, Berdnikov VV, Black T, Boeglin W, Boer M, Briscoe WJ, Britton T, Cao S, Chudakov E, Chung G, Cole PL, Cortes O, Crede V, Dalton MM, Darulis D, Deur A, Dobbs S, Dolgolenko A, Dugger M, Dzhygadlo R, Ebersole D, Edo M, Egiyan H, Erbora T, Eugenio P, Fabrizi A, Fanelli C, Fang S, Fitches J, Foda AM, Furletov S, Gan L, Gao H, Gardner A, Gasparian A, Glazier D, Gleason C, Goryachev VS, Grube B, Guo J, Guo L, Hernandez J, Hernandez K, Hoffman ND, Hornidge D, Hou G, Hurck P, Hurley A, Imoehl W, Ireland DG, Ito MM, Jaegle I, Jarvis NS, Jeske T, Jing M, Jones RT, Kakoyan V, Kalicy G, Khachatryan V, Kourkoumelis C, LaDuke A, Larin I, Lawrence D, Lersch DI, Li H, Liu B, Livingston K, Lolos GJ, Lorenti L, Lyubovitskij V, Ma R, Mack D, Mahmood A, Marukyan H, Matveev V, McCaughan M, McCracken M, Meyer CA, Miskimen R, Mitchell RE, Mizutani K, Neelamana V, Ng L, Nissen E, Orešić S, Ostrovidov AI, Papandreou Z, Paudel C, Pedroni R, Pentchev L, Peters KJ, Prather E, Rakshit S, Reinhold J, Remington A, Ritchie BG, Ritman J, Rodriguez G, Romanov D, Saldana K, Salgado C, Schadmand S, Schertz AM, Scheuer K, Schick A, Schmidt A, Schumacher RA, Schwiening J, Septian N, Sharp P, Shen X, Shepherd MR, Sikes J, Smith A, Smith ES, Sober DI, Somov A, Somov S, Stevens JR, Strakovsky II, Sumner B, Suresh K, Tarasov VV, Taylor S, Teymurazyan A, Thiel A, Viducic T, Whitlatch T, Wickramaarachchi N, Wunderlich Y, Yu B, Zarling J, Zhang Z, Zhou X, and Zihlmann B

Abstract

The spin-exotic hybrid meson π_{1}(1600) is predicted to have a large decay rate to the ωππ final state. Using 76.6  pb^{-1} of data collected with the GlueX detector, we measure the cross sections for the reactions γp→ωπ^{+}π^{-}p, γp→ωπ^{0}π^{0}p, and γp→ωπ^{-}π^{0}Δ^{++} in the range E_{γ}=8-10  GeV. Using isospin conservation, we set the first upper limits on the photoproduction cross sections of the π_{1}^{0}(1600) and π_{1}^{-}(1600). We combine these limits with lattice calculations of decay widths and find that photoproduction of η^{'}π is the most sensitive two-body system to search for the π_{1}(1600).

Published
2024
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5. First Measurement Using Elliptically Polarized Photons of the Double-Polarization Observable E for γp→pπ^{0} and γp→nπ^{+}.

Author

Afzal F, Spieker K, Hurck P, Abt S, Achenbach P, Adlarson P, Ahmed Z, Akondi CS, Annand JRM, Arends HJ, Bashkanov M, Beck R, Biroth M, Borisov N, Braghieri A, Briscoe WJ, Cividini F, Collicott C, Costanza S, Denig A, Dieterle M, Downie EJ, Drexler P, Fegan S, Gardner S, Ghosal D, Glazier DI, Gorodnov I, Gradl W, Gurevich D, Heijkenskjöld L, Hornidge D, Huber GM, Kashevarov VL, Kay SJD, Korolija M, Krusche B, Lazarev A, Livingston K, Lutterer S, MacGregor IJD, Macrae RG, Manley DM, Martel PP, Miskimen R, Mocanu M, Mornacchi E, Mullen C, Neganov A, Neiser A, Oberle M, Ostrick M, Otte PB, Paudyal D, Pedroni P, Powell A, Reicherz G, Rostomyan T, Sfienti C, Sokhoyan V, Steffen O, Strakovsky II, Strub T, Supek I, Thiel A, Thiel M, Thomas A, Usov YA, Wagner S, Walford NK, Watts DP, Werthmüller D, Wettig J, Witthauer L, Wolfes M, and Zachariou N

Abstract

We report the measurement of the helicity asymmetry E for the pπ^{0} and nπ^{+} final states using, for the first time, an elliptically polarized photon beam in combination with a longitudinally polarized target at the Crystal Ball experiment at MAMI. The results agree very well with data that were taken with a circularly polarized photon beam, showing that it is possible to simultaneously measure polarization observables that require linearly (e.g., G) and circularly polarized photons (e.g., E) and a longitudinally polarized target. The new data cover a photon energy range 270-1400 MeV for the pπ^{0} final state (230-842 MeV for the nπ^{+} final state) and the full range of pion polar angles, θ, providing the most precise measurement of the observable E. A moment analysis gives a clear observation of the pη cusp in the pπ^{0} final state.

Published
2024
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6. Single π 0 production off neutrons bound in deuteron with linearly polarized photons.

Author

Mullen C, Gardner S, Glazier DI, Kay SJD, Livingston K, Strakovsky II, Workman RL, Abt S, Achenbach P, Afzal F, Ahmed Z, Akondi CS, Annand JRM, Bashkanov M, Beck R, Biroth M, Borisov NS, Braghieri A, Briscoe WJ, Cividini F, Collicott C, Costanza S, Denig A, Dieterle M, Downie EJ, Drexler P, Fegan S, Ferretti-Bondy MI, Ghosal D, Gorodnov I, Gradl W, Günther M, Gurevic G, Heijkenskjöld L, Hornidge D, Huber GM, Jermann N, Kaeser A, Korolija M, Kashevarov VL, Krusche B, Kulikov VV, Lazarev A, Lutterer S, MacGregor IJD, Manley DM, Martel PP, Martemianov MA, Meier C, Miskimen R, Mocanu M, Mornacchi E, Neganov A, Oberle M, Ostrick M, Otte P, Paudyal D, Pedroni P, Powell A, Prakhov SN, Reicherz G, Ron G, Rostomyan T, Sfienti C, Sokhoyan V, Spieker K, Steffen O, Strub T, Supek I, Thiel A, Thiel M, Thomas A, Unverzagt M, Usov YA, Wagner S, Walford NK, Watts DP, Werthmüller D, Wettig J, Witthauer L, Wolfes M, and Zachariou N

Abstract

The quasifree γ → d → π 0 n ( p ) photon beam asymmetry, Σ , has been measured at photon energies, E γ , from 390 to 610 MeV, corresponding to center of mass energy from 1.271 to 1.424 GeV, for the first time. The data were collected in the A2 hall of the MAMI electron beam facility with the Crystal Ball and TAPS calorimeters covering pion center-of-mass angles from 49 ∘ to 148 ∘ . In this kinematic region, polarization observables are sensitive to contributions from the Δ ( 1232 ) and N (1440) resonances. The extracted values of Σ have been compared to predictions based on partial-wave analyses (PWAs) of the existing pion photoproduction database. Our comparison includes the SAID, MAID and Bonn-Gatchina analyses; while a revised SAID fit, including the new Σ measurements, has also been performed. In addition, isospin symmetry is examined as a way to predict π 0 n photoproduction observables, based on fits to published data in the channels π 0 p , π + n and π - p ., (© The Author(s) 2021.)

Published
2021
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7. Signatures of the d^{*}(2380) Hexaquark in d(γ,pn[over →]).

Author

Bashkanov M, Watts DP, Kay SJD, Abt S, Achenbach P, Adlarson P, Afzal F, Ahmed Z, Akondi CS, Annand JRM, Arends HJ, Beck R, Biroth M, Borisov N, Braghieri A, Briscoe WJ, Cividini F, Collicott C, Costanza S, Denig A, Downie EJ, Drexler P, Fegan S, Fix A, Gardner S, Ghosal D, Glazier DI, Gorodnov I, Gradl W, Günther M, Gurevich D, Heijkenskjöld L, Hornidge D, Huber GM, Käser A, Kashevarov VL, Korolija M, Krusche B, Lazarev A, Livingston K, Lutterer S, MacGregor IJD, Manley DM, Martel PP, Miskimen R, Mornacchi E, Mullen C, Neganov A, Neiser A, Ostrick M, Otte PB, Paudyal D, Pedroni P, Powell A, Prakhov SN, Ron G, Sarty A, Sfienti C, Sokhoyan V, Spieker K, Steffen O, Strakovsky II, Strub T, Supek I, Thiel A, Thiel M, Thomas A, Usov YA, Wagner S, Walford NK, Werthmüller D, Wettig J, Wolfes M, Zachariou N, and Zana LA

Abstract

We report a measurement of the spin polarization of the recoiling neutron in deuterium photodisintegration, utilizing a new large acceptance polarimeter within the Crystal Ball at MAMI. The measured photon energy range of 300-700 MeV provides the first measurement of recoil neutron polarization at photon energies where the quark substructure of the deuteron plays a role, thereby providing important new constraints on photodisintegration mechanisms. A very high neutron polarization in a narrow structure centered around E_{γ}∼570  MeV is observed, which is inconsistent with current theoretical predictions employing nucleon resonance degrees of freedom. A Legendre polynomial decomposition suggests this behavior could be related to the excitation of the d^{*}(2380) hexaquark.

Published
2020
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8. Study of η and η' Photoproduction at MAMI.

Author

Kashevarov VL, Ott P, Prakhov S, Adlarson P, Afzal F, Ahmed Z, Akondi CS, Annand JRM, Arends HJ, Beck R, Braghieri A, Briscoe WJ, Cividini F, Codling R, Collicott C, Costanza S, Denig A, Downie EJ, Dieterle M, Ferretti Bondy MI, Fil'kov LV, Fix A, Gardner S, Garni S, Glazier DI, Glowa D, Gradl W, Gurevich G, Hamilton DJ, Hornidge D, Howdle D, Huber GM, Käser A, Kay S, Keshelashvili I, Kondratiev R, Korolija M, Krusche B, Linturi J, Lisin V, Livingston K, MacGregor IJD, MacRae R, Mancell J, Manley DM, Martel PP, McGeorge JC, McNicol E, Middleton DG, Miskimen R, Mornacchi E, Mullen C, Mushkarenkov A, Neiser A, Oberle M, Ostrick M, Otte PB, Oussena B, Paudyal D, Pedroni P, Polyanski VV, Rajabi A, Reicherz G, Robinson J, Rosner G, Rostomyan T, Sarty A, Schott DM, Schumann S, Sfienti C, Sokhoyan V, Spieker K, Steffen O, Strandberg B, Strakovsky II, Strub T, Supek I, Taragin MF, Thiel A, Thiel M, Tiator L, Thomas A, Unverzagt M, Wagner S, Watts DP, Werthmüller D, Wettig J, Witthauer L, Wolfes M, Workman RL, and Zana L

Abstract

The reactions γp→ηp and γp→η^{'}p are measured from their thresholds up to the center-of-mass energy W=1.96  GeV with the tagged-photon facilities at the Mainz Microtron, MAMI. Differential cross sections are obtained with unprecedented statistical accuracy, providing fine energy binning and full production-angle coverage. A strong cusp is observed in the total cross section for η photoproduction at the energies in the vicinity of the η^{'} threshold, W=1896  MeV (E_{γ}=1447  MeV). Within the framework of a revised ηMAID isobar model, the cusp, in connection with a steep rise of the η^{'} total cross section from its threshold, can only be explained by a strong coupling of the poorly known N(1895)1/2^{-} state to both ηp and η^{'}p. Including the new high-accuracy results in the ηMAID fit to available η and η^{'} photoproduction data allows the determination of the N(1895)1/2^{-} properties.

Published
2017
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9. Measurements of double-polarized compton scattering asymmetries and extraction of the proton spin polarizabilities.

Author

Martel PP, Miskimen R, Aguar-Bartolome P, Ahrens J, Akondi CS, Annand JR, Arends HJ, Barnes W, Beck R, Bernstein A, Borisov N, Braghieri A, Briscoe WJ, Cherepnya S, Collicott C, Costanza S, Denig A, Dieterle M, Downie EJ, Fil'kov LV, Garni S, Glazier DI, Gradl W, Gurevich G, Hall Barrientos P, Hamilton D, Hornidge D, Howdle D, Huber GM, Jude TC, Kaeser A, Kashevarov VL, Keshelashvili I, Kondratiev R, Korolija M, Krusche B, Lazarev A, Lisin V, Livingston K, MacGregor IJ, Mancell J, Manley DM, Meyer W, Middleton DG, Mushkarenkov A, Nefkens BM, Neganov A, Nikolaev A, Oberle M, Ortega Spina H, Ostrick M, Ott P, Otte PB, Oussena B, Pedroni P, Polonski A, Polyansky V, Prakhov S, Rajabi A, Reicherz G, Rostomyan T, Sarty A, Schrauf S, Schumann S, Sikora MH, Starostin A, Steffen O, Strakovsky II, Strub T, Supek I, Thiel M, Tiator L, Thomas A, Unverzagt M, Usov Y, Watts DP, Witthauer L, Werthmüller D, and Wolfes M

Abstract

The spin polarizabilities of the nucleon describe how the spin of the nucleon responds to an incident polarized photon. The most model-independent way to extract the nucleon spin polarizabilities is through polarized Compton scattering. Double-polarized Compton scattering asymmetries on the proton were measured in the Δ(1232) region using circularly polarized incident photons and a transversely polarized proton target at the Mainz Microtron. Fits to asymmetry data were performed using a dispersion model calculation and a baryon chiral perturbation theory calculation, and a separation of all four proton spin polarizabilities in the multipole basis was achieved. The analysis based on a dispersion model calculation yields γ(E1E1)=-3.5±1.2, γ(M1M1)=3.16±0.85, γ(E1M2)=-0.7±1.2, and γ(M1E2)=1.99±0.29, in units of 10(-4)  fm(4).

Published
2015
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10. Measurement of the transverse target and beam-target asymmetries in η meson photoproduction at MAMI.

Author

Akondi CS, Annand JR, Arends HJ, Beck R, Bernstein A, Borisov N, Braghieri A, Briscoe WJ, Cherepnya S, Collicott C, Costanza S, Downie EJ, Dieterle M, Fix A, Fil'kov LV, Garni S, Glazier DI, Gradl W, Gurevich G, Hall Barrientos P, Hamilton D, Hornidge D, Howdle D, Huber GM, Kashevarov VL, Keshelashvili I, Kondratiev R, Korolija M, Krusche B, Lazarev A, Lisin V, Livingston K, MacGregor IJ, Mancel J, Manley DM, Martel P, McNicoll EF, Meyer W, Middleton D, Miskimen R, Mushkarenkov A, Nefkens BM, Neganov A, Nikolaev A, Oberle M, Ostrick M, Ortega H, Ott P, Otte PB, Oussena B, Pedroni P, Polonski A, Polyanski VV, Prakhov S, Reicherz G, Rostomyan T, Sarty A, Schumann S, Steffen O, Strakovsky II, Strub T, Supek I, Tiator L, Thomas A, Unverzagt M, Usov YA, Watts DP, Werthmüller D, Witthauer L, and Wolfes M

Abstract

We present new data for the transverse target asymmetry T and the very first data for the beam-target asymmetry F in the γ[over →]p[over →]→ηp reaction up to a center-of-mass energy of W=1.9  GeV. The data were obtained with the Crystal-Ball/TAPS detector setup at the Glasgow tagged photon facility of the Mainz Microtron MAMI. All existing model predictions fail to reproduce the new data indicating a significant impact on our understanding of the underlying dynamics of η meson photoproduction. The peculiar nodal structure observed in existing T data close to threshold is not confirmed.

Published
2014
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