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We measured angular distributions of differential cross section, beam analyzing power, and recoil polarization for neutral pion electroproduction at Q^2 = 1.0 (GeV/c)^2 in 10 bins of W across the Delta resonance. A total of 16 independent…

Nuclear Experiment · Physics 2010-05-27 J. J. Kelly

A new partial wave analysis of pion photoproduction has been obtained in the framework of fixed-t dispersion relations valid form threshold up to 500 MeV. It is based on new Mainz data for \pi^{0} and \pi^{+} production off the proton and…

Nuclear Theory · Physics 2011-04-15 L. Tiator

The recoil proton polarization in the $\pi^0$ production off the proton with longitudinally polarized electron beam has been studied as a means to measure quadrupole components in the N to $\Delta$ transition. On top of the $\Delta$…

Nuclear Theory · Physics 2011-07-19 H. Schmieden

The recoil proton polarization has been measured in the p (\vec e,e'\vec p) pi^0 reaction in parallel kinematics around W = 1232 MeV, Q^2 = 0.121 (GeV/c)^2 and epsilon = 0.718 using the polarized c.w. electron beam of the Mainz Microtron.…

We have analyzed the $M_{1+}^{(3/2)}$ and $E_{1+}^{(3/2)}$ multipole amplitudes of pion photoproduction in the framework of fixed-$t$ dispersion relations. Applying the speed plot technique to our results for these multipoles, we have…

Nuclear Theory · Physics 2008-11-26 O. Hanstein , D. Drechsel , L. Tiator

A fit to the existing pion electroproduction data is presented. This work builds upon our previous analyses of pion photoproduction and elastic pion-nucleon scattering over the Delta resonance region. We comment on the extraction of E_1+…

Nuclear Theory · Physics 2014-11-18 R. A. Arndt , I. I. Strakovsky , R. L. Workman

The study of exclusive $\pi^{\pm}$ electroproduction on the nucleon, including separation of the various structure functions, is of interest for a number of reasons. The ratio $R_L=\sigma_L^{\pi^-}/\sigma_L^{\pi^+}$ is sensitive to…

The production of neutral and charged pions as well as eta mesons is studied in the Delta and N* resonance region, respectively. Heavy A=3 recoils were measured with the GEM detector. The differential cross sections covering the full…

For high energy linearly polarized photon--proton scattering we have calculated the azimuthal and polar angle distributions in inclusive on recoil proton experimental setup. We have taken into account the production of lepton and…

High Energy Physics - Phenomenology · Physics 2008-11-26 E. Bartos , E. A. Kuraev , Yu. P. Peresunko , E. A. Vinokurov

Pion electroproduction off the proton is analyzed in a new framework based on a general parametrization of transition amplitudes, including constraints from gauge invariance and threshold behavior. Data with energies $1.13~{\rm…

Regge-pole based descriptions of pion-electroproduction on nucleons have given a very good description of the longitudinal components of the cross sections. However, these very same models grossly underestimate the transverse components. A…

Nuclear Theory · Physics 2015-06-03 Murat Kaskulov , Ulrich Mosel

We construct a model for the weak pion production off the nucleon, which in addition to the weak excitation of the $\Delta(1232)$ resonance and its subsequent decay into $N\pi$, it includes also some background terms required by chiral…

Nuclear Theory · Physics 2008-11-26 E. Hernandez , J. Nieves , M. Valverde

A partial wave analysis of pion photoproduction has been obtained in the framework of fixed-t dispersion relations valid from threshold up to 500 MeV. In the resonance region we have precisely determined the electromagnetic properties of…

Nuclear Theory · Physics 2009-11-06 L. Tiator , D. Drechsel , O. Hanstein , S. S. Kamalov , S. N. Yang

Hyperon recoil polarization measurements for the exclusive electroproduction of $K^+\Lambda$ and $K^+\Sigma^0$ final states from an unpolarized proton target have been carried out using the CLAS12 spectrometer at Jefferson Laboratory. The…

Nuclear Experiment · Physics 2025-05-20 D. S. Carman , A. D'Angelo , L. Lanza , V. I. Mokeev , P. Achenbach , J. S. Alvarado , M. J. Amaryan , H. Atac , H. Avakian , N. A. Baltzell , L. Barion , M. Bashkanov , M. Battaglieri , F. Benmokhtar , A. Bianconi , A. S. Biselli , M. Bondi , S. Boiarinov , F. Bossu , K. -Th. Brinkmann , W. J. Briscoe , S. Bueltmann , V. D. Burkert , T. Cao , R. Capobianco , A. Celentano , P. Chatagnon , V. Chesnokov , G. Ciullo , P. L. Cole , M. Contalbrigo , N. Dashyan , R. De Vita , A. Deur , S. Diehl , C. Dilks , C. Djalali , M. Dugger , R. Dupre , A. El Alaoui , L. El Fassi , L. Elouadrhiri , S. Fegan , A. Filippi , G. Gavalian , D. I. Glazier , R. W. Gothe , Y. Gotra , L. Guo , K. Hafidi , H. Hakobyan , M. Hattawy , F. Hauenstein , T. B. Hayward , D. Heddle , A. Hobart , M. Holtrop , Yu-Chun Hung , Y. Ilieva , D. G. Ireland , E. L. Isupov , H. Jiang , H. S. Jo , T. Kageya , V. Klimenko , A. Kripko , V. Kubarovsky , P. Lenisa , S. Liyanaarachchi , I. J. D. MacGregor , D. Marchand , V. Mascagna , D. Matamoros , M. Maynes , B. McKinnon , T. Mineeva , M. Mirazita , C. Munoz Camacho , P. Nadel-Turonski , T. Nagorna , K. Neupane , S. Niccolai , G. Niculescu , M. Osipenko , P. Pandey , M. Paolone , L. L. Pappalardo , R. Paremuzyan , E. Pasyuk , S. J. Paul , W. Phelps , N. Pilleux , S. Polcher Rafael , J. W. Price , Y. Prok , B. A. Raue , T. Reed , M. Ripani , J. Ritman , P. Rossi , C. Salgado , S. Schadmand , A. Schmidt , M. B. C. Scott , Y. G. Sharabian , S. Shrestha , D. Sokhan , N. Sparveris , N. Spreafico , S. Stepanyan , I. I. Strakovsky , S. Strauch , J. A. Tan , N. Trotta , R. Tyson , M. Ungaro , S. Vallarino , L. Venturelli , T. Vittorini , H. Voskanyan , E. Voutier , Y. Wang , D P. Watts , U. Weerasinghe , X. Wei , M. H. Wood , L. Xu , N. Zachariou , Z. W. Zhao , M. Zurek

The reaction pp->pppi0pi0 has been investigated at a beam energy of 1.4 GeV using the WASA-at-COSY facility. The total cross section is found to be (324 +- 21_systematic +- 58_normalization) mub. In order to to study the production…

High Energy Physics - Experiment · Physics 2015-05-28 P. Adlarson , C. Adolph , W. Augustyniak , M. Bashkanov , T. Bednarski , F. S. Bergmann , M. Berłowski , H. Bhatt , K. --T. Brinkmann , M. Büscher , H. Calén , H. Clement , D. Coderre , E. Czerwiński , E. Doroshkevich , R. Engels , W. Erven , W. Eyrich , P. Fedorets , K. Föhl , K. Fransson , F. Goldenbaum , P. Goslawski , K. Grigoryevj , C. --O. Gullström , L. Heijkenskjöld , J. Heimlich , V. Hejny , F. Hinterberger , M. Hodana , B. Höistad , M. Jacewicz , M. Janusz , A. Jany , B. R. Jany , L. Jarczyk , T. Johansson , B. Kamys , G. Kemmerling , O. Khakimova , A. Khoukaz , S. Kistryn , J. Klaja , H. Kleines , B. Kłos , F. Kren , W. Krzemień , P. Kulessa , A. Kupść , K. Lalwani , B. Lorentz , H. Machner , A. Magiera , R. Maier , B. Mariański , P. Marciniewski , M. Mikirtychiants , H. --P. Morsch , P. Moskal , B. K. Nandi , S. Niedźwiecki , H. Ohm , A. Passfeld , C. Pauly , E. Perez del Rio , Y. Petukhov , N. Piskunov , P. Pluciński , P. Podkopał , A. Povtoreyko , D. Prasuhn , A. Pricking , K. Pysz , T. Rausmann , C. F. Redmer , J. Ritman , Z. Rudy , S. Sawant , S. Schadmand , A. Schmidt , T. Sefzick , V. Serdyuk , N. Shah , M. Siemaszko , T. Skorodko , M. Skurzok , J. Smyrski , V. Sopov , R. Stassen , J. Stepaniak , G. Sterzenbach , H. Stockhorst , A. Szczurek , A. Täschner , T. Tolba , A. Trzciński , R. Varma , P. Vlasov , G. J. Wagner , W. Weglorz , U. Wiedner , A. Winnemöller , M. Wolke , A. Wrońska , P. Wüstner , P. Wurm , X. Yuan , L. Yurev , J. Zabierowski , C. Zheng , M. J. Zieliński , W. Zipper , J. Złomańczuk , P. Zuprański

The beam-recoil double polarization P_{x'}^h and P_{z'}^h and the recoil polarization P_{y'} were measured for the first time for the p(\vec{e},e'\vec{p})\eta reaction at a four-momentum transfer of Q^2=0.1 GeV^2/c^2 and a center of mass…

We have performed a series of global and single-Q2 fits to the growing database for pion electroproduction. We compare to some other recent fits which have used different formalisms, more selective datasets, and truncated multipole…

Nuclear Theory · Physics 2017-08-23 R. Arndt , W. Briscoe , I. Strakovsky , R. Workman

The resonance $\Delta(1232)$ with spin-parity ${3 \over 2}^+$, which contributes dominantly to the reactions like $\gamma N \to \pi N$ and $NN \to NN\pi$ at intermediate energies, may be expected to be produced in characteristically…

Nuclear Theory · Physics 2009-01-07 G. Ramachandran , Venkataraya , M. S. Vidya , J. Balasubramanyam , G. Padmanabha

The dynamical model developed in [Phys. Rev. C 54, 2660 (1996)] has been applied to investigate the pion electroproduction reactions on the nucleon. It is found that the model can describe to a very large extent the recent data of p(e,e'…

Nuclear Theory · Physics 2009-11-06 T. Sato , T. -S. H. Lee

The polarized longitudinal-transverse structure function $\sigma_{LT^\prime}$ measures the interference between real and imaginary amplitudes in pion electroproduction and can be used to probe the coupling between resonant and non-resonant…

Nuclear Experiment · Physics 2010-04-06 CLAS Collaboration , K. Joo , L. C. Smith
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