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We derive the separate helicity amplitudes involving the partial wave analysis in the process of pseudo-scalar meson photon productions with $J^P=3/2^+$, which is independent on model. According to parity, the general amplitude in the case…

High Energy Physics - Phenomenology · Physics 2015-08-24 Leihua Liu , Liye Xiao

We review the last two decades of using photon beams to measure the production of mesons, and in particular the information that can be obtained on the spectrum of light, non-strange baryons. This is a compendium of experimental results,…

Nuclear Experiment · Physics 2020-02-19 David G. Ireland , Eugene Pasyuk , Igor Strakovsky

This review treats the advances in Light Baryon Spectroscopy of the last two decades, which were mainly obtained by measuring meson-production reactions at photon facilities all over the world. We provide a consistent compendium of…

Nuclear Experiment · Physics 2022-03-14 Annika Thiel , Farah Afzal , Yannick Wunderlich

Ambiguities in pseudoscalar-meson photoproduction, arising from incomplete experimental data, have analogs in pion-nucleon scattering. Amplitude ambiguities have important implications for the problems of amplitude extraction and resonance…

Nuclear Theory · Physics 2008-11-26 Greg Keaton , Ron Workman

In general there are nine observables in the decay of a B meson to two vector mesons defined in terms of polarization correlations of these mesons. Only six of these can be detected via the subsequent decay angular distributions because of…

High Energy Physics - Phenomenology · Physics 2009-10-31 Cheng-Wei Chiang , Lincoln Wolfenstein

We study the strangeness $+1$ meson-baryon systems to obtain improved $KN$ and $K^*N$ amplitudes and to look for a possible resonance formation by the $KN$-$K^*N$ coupled interaction. We obtain amplitudes for light vector meson-baryon…

Nuclear Theory · Physics 2015-12-01 K. P. Khemchandani , A. Martinez Torres , F. S. Navarra , M. Nielsen , L. Tolos

In this talk I show recent results on how many excited baryon resonances appear as systems of one meson and one baryon, or two mesons and one baryon, with the mesons being either pseudoscalar or vectors. Connection with experiment is made…

Two methods for creating arbitrary two-photon polarization pure states are introduced. Based on these, four schemes for creating two-photon polarization mixed states are proposed and analyzed. The first two schemes can synthesize completely…

The contributions of direct knockout processes, in addition to the diffractive production and one-pion-exchange processes associated with the phi-rho-pi and phi-gamma-pi couplings, to the polarization observables of the phi photoproduction…

Nuclear Theory · Physics 2010-11-19 Alexander I. Titov , Yongseok Oh , Shin Nan Yang

General expressions for the unpolarized differential cross section and for various polarization observables in the coherent pseudoscalar meson photo- and electroproduction on the deuteron target have been obtained in one-photon-exchange…

High Energy Physics - Phenomenology · Physics 2019-08-07 G. I. Gakh , A. G. Gakh , E. Tomasi-Gustafsson

With the advent of new photon tagging facilities and novel experimental technologies it has become possible to perform photoproduction cross section measurements of pseudoscalar mesons on nuclei with a percent level accuracy. The extraction…

High Energy Physics - Phenomenology · Physics 2009-11-10 S. Gevorkyan , A. Gasparian , L. Gan , I. Larin , M. Khandaker

Recent advances in the photon tagging facilities together with the novel, high resolution fast calorimetry made possible to perform photoproduction cross section measurements of pseudoscalar mesons on nuclei with a percent level accuracy.…

High Energy Physics - Phenomenology · Physics 2015-05-13 S. Gevorkyan , A. Gasparian , L. Gan , I. Larin , M. Khandaker

Starting from a bound-state model of weakly bound quarks for ($q \bar{q}$) mesons, we derive a formalism for computing the production or decay of such mesons, whatever the value of their internal orbital angular momentum L. That approach…

High Energy Physics - Phenomenology · Physics 2008-02-03 L. Houra-Yaou , P. Kessler , J. Parisi , F. Murgia , J. Hansson

We study the pair production of $B_c$ mesons in the photon-photon interaction in the framework of perturbative quantum chromodynamics and the relativistic quark model. The production amplitudes of a pair of pseudoscalar and vector $B_c$…

High Energy Physics - Phenomenology · Physics 2020-08-05 A. E. Dorokhov , R. N. Faustov , A. P. Martynenko , F. A. Martynenko

Particles in a hidden sector can potentially acquire a small electric charge through their interaction with the Standard Model and can consequently be observed as millicharged particles. We systematically compute the production of…

High Energy Physics - Phenomenology · Physics 2016-11-30 Emidio Gabrielli , Luca Marzola , Edoardo Milotti , Hardi Veermäe

The discrete ambiguities appearing in the complete experiment problem for single pseudoscalar meson photoproduction within truncated partial-wave analysis are discussed. It is shown that, in addition to the double ambiguity known from…

Nuclear Theory · Physics 2023-04-26 A. Fix , I. Dementjev

Developments in strangeness photo- and electro- production off the proton, as investigated using the CLAS system in Hall B at Jefferson Lab, are discussed in this paper. By measuring sufficient spin observables one can decompose the…

Nuclear Experiment · Physics 2011-02-01 Reinhard Schumacher

For pseudoscalar meson electroproduction off the nucleon in parallel kinematics a relation between three polarization observables is derived. It is shown that, without Rosenbluth separation, a measurement of the longitudinal strength can be…

Nuclear Theory · Physics 2009-10-31 Hartmut Schmieden , Lothar Tiator

The photoproduction of $\pi^+\pi^-$ meson pairs off the proton has been studied in the reaction $\gamma p\to p\,\pi^+\pi^-$ using the CEBAF Large Acceptance Spectrometer (CLAS) and the frozen-spin target (FROST) in Hall B at the Thomas…

Nuclear Experiment · Physics 2025-05-01 P. Roy , S. Cao , V. Crede , E. Klempt , V. A. Nikonov , A. V. Sarantsev , V. D. Burkert , V. Mokeev , P. Achenbach , J. S. Alvarado , W. R. Armstrong , H. Atac , H. Avakian , N. A. Baltzell , L. Barion , M. Bashkanov , M. Battaglieri , F. Benmokhtar , A. Bianconi , A. S. Biselli , M. Bondi , F. Bossu , S. Boiarinov , K. -T. Brinkmann , W. J. Briscoe , W. K. Brooks , T. Cao , R. Capobianco , D. S. Carman , P. Chatagnon , G. Ciullo , P. L. Cole , M. Contalbrigo , A. D'Angelo , N. Dashyan , R. DeVita , M. Defurne , A. Deur , S. Diehl , C. Djalali , M. Dugger , R. Dupre , H. Egiyan , A. El Alaoui , L. El Fassi , P. Eugenio , S. Fegan , I. P. Fernando , A. Filippi , G. Gavalian , R. W. Gothe , L. Guo , K. Hafidi , H. Hakobyan , M. Hattawy , T. B. Hayward , D. Heddle , A. Hobart , M. Holtrop , Y. Ilieva , D. G. Ireland , E. L. Isupov , D. Jenkins , H. Jiang , H. S. Jo , K. Joo , S. Joosten , D. Keller , M. Khandaker , A. Kim , W. Kim , F. J. Klein , V. Klimenko , A. Kripko , V. Kubarovsky , L. Lanza , P. Lenisa , X. Li , K. Livingston , I. J. D. MacGregor , D. Marchand , D. Martiryan , V. Mascagna , D. Matamoros , M. E. McCracken , B. McKinnon , T. Mineeva , C. Munoz Camacho , P. Nadel-Turonski , K. Neupane , D. Nguyen , G. Niculescu , M. Osipenko , A. I. Ostrovidov , M. Ouillon , P. Pandey , M. Paolone , L. L. Pappalardo , R. Paremuzyan , E. Pasyuk , S. J. Paul , W. Phelps , N. Pilleux , S. Polcher Rafael , J. Price , Y. Prok , D. Protopopescu , J. Richards , M. Ripani , B. Ritchie , J. Ritman , G. Rosner , P. Rossi , A. A. Rusova , C. Salgado , S. Schadmand , A. Schmidt , R. A. Schumacher , Y. G. Sharabian , E. V. Shirokov , S. Shrestha , D. Sokhan , N. Sparveris , M. Spreafico , I. I. Strakovsky , S. Strauch , J. A. Tan , M. Tenorio , N. Trotta , R. Tyson , M. Ungaro , S. Vallarino , L. Venturelli , T. Vittorini , H. Voskanyan , E. Voutier , D. P. Watts , U. Weerasinghe , X. Wei , M. H. Wood , L. Xu , N. Zachariou , Z. W. Zhao , M. Zurek