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A behavior of the nucleon structure functions in the resonance region is investigated. Expressions for resonance production form factors, dependent on photon virtuality $Q^2$, which have correct threshold behavior and take into account…

High Energy Physics - Phenomenology · Physics 2007-05-23 V. V. Davidovsky , B. V. Struminsky

The capture of K$^-$ mesons on nucleons bound in nuclei offer a chance to study the $\Sigma \pi$ pairs below the kinematic threshold of the $\bar{\mathrm{K}}$N systems. Various hyperon-pion charged combination are presently under…

Nuclear Experiment · Physics 2017-11-22 Raffaele Del Grande , Kristian Piscicchia , Slawomir Wycech

Hadron electromagnetic form factors of hadrons in the time-like region at the boundary of the physical region is considered. The energy behaviour of the form factor is shown to be dominantely determined by the strong hadron-antihadron…

High Energy Physics - Phenomenology · Physics 2008-08-05 O. D. Dalkarov , P. A. Khakhulin , A. Yu. Voronin

In frame of a phenomenological approach based on Compton-like Feynman amplitudes, we study multi-pion production in antiproton nucleon collisions. The main interest of this reaction is related to the possibility to study the properties of…

High Energy Physics - Phenomenology · Physics 2008-11-26 E. A. Kuraev , C. Adamuscin , E. Tomasi-Gustafsson , F. Maas

We study the scaling regime of pion electroproduction in the backward region, eN->e'N'pi. We compute the leading-twist amplitude in the kinematical region, where it factorises into a short-distance matrix element and long-distance dominated…

High Energy Physics - Phenomenology · Physics 2014-11-18 J. P. Lansberg , B. Pire , L. Szymanowski

Considering the nucleon as a system of confined valence quarks surrounded by pions we derive a Galster-like parameterization of the neutron electric form factor $G_E^n$. Furthermore, we show that the proposed parameterization can be linked…

Nuclear Theory · Physics 2009-11-10 Murat M. Kaskulov , Peter Grabmayr

We derive novel low--energy theorems for single pion production off nucleons through the isovector axial current. We find that the $k^2$-dependence of the multipole $L_{0+}^{(+)}$ at threshold is given by the nucleon scalar form factor,…

High Energy Physics - Phenomenology · Physics 2011-07-19 V. Bernard , N. Kaiser , Ulf-G. Meißner

Effects due to non-pointlike behaviour of pions in the process $e^+e^-\to\pi^+\pi^-\gamma$ can arise for hard photons in the final state. By means of a Monte Carlo event generator, which also includes the contribution of the direct decay…

High Energy Physics - Phenomenology · Physics 2008-11-26 G. Pancheri , O. Shekhovtsova , G. Venanzoni

In this talk we report on two physical processes, the photoproduction of $\rho$ mesons in nuclei and the $\pi^0 \pi^0$ photoproduction in nuclei at low energies. In the first case the aim is to observe experimentally the theoretically…

Nuclear Theory · Physics 2007-05-23 E. Oset , L. Roca , M. J. Vicente Vacas , J. C. Nacher

Nucleon-nucleon (NN) forces from chiral perturbation theory at next-to-leading (NLO) and next-to-next-to-leading order (NNLO) are applied to systems with two, three and four nucleons. At NNLO, we consider two versions of the chiral…

Nuclear Theory · Physics 2007-05-23 E. Epelbaum , A. Nogga , W. Gloeckle , H. Kamada , U. -G. Meissner , H. Witala

The exclusive electroproduction process $ep \rightarrow e'p'\pi^{0}$ was measured in the range of photon virtualities $Q^{2} = 0.4 - 1.0$~GeV$^{2}$ and the invariant mass range of the $p\pi^{0}$ system of $W = 1.1 - 1.8$~GeV. These…

Nuclear Experiment · Physics 2020-01-29 N. Markov , K. Joo , V. D. Burkert , V. I. Mokeev , L. C. Smith , M. Ungaro , S. Adhikari , M. J. ~Amaryan , G. Angelini , H. ~Atac , H. ~Avakian , C. Ayerbe Gayoso , N. A. ~Baltzell , L. Barion , M. ~Battaglieri , I. ~Bedlinskiy , I. ~Bedlinskiy , F. Benmokhtar , A. S. ~Biselli , F. ~Bossù , S. ~Boiarinov , W. J. ~Briscoe , W. K. ~Brooks , D. S. ~Carman , J. C. ~Carvajal , A. ~Celentano , P. ~Chatagnon , T. Chetry , P. L. ~Cole , M. ~Contalbrigo , V. ~Crede , G. Ciullo , A. ~D'Angelo , N. ~Dashyan , R. ~De~Vita , E. ~De~Sanctis , M. Defurne , A. ~Deur , S. Diehl , C. ~Djalali , R. ~Dupre , M. ~Ehrhart , A. ~El~Alaoui , L. ~El~Fassi , P. ~Eugenio , C. ~Evans , A. ~Filippi , Y. ~Ghandilyan , F. X. ~Girod , E. ~Golovatch , R. W. ~Gothe , K. A. ~Griffioen , M. ~Guidal , K. ~Hafidi , H. ~Hakobyan , M. ~Hattawy , T. B. ~Hayward , K. ~Hicks , M. ~Holtrop , Y. ~Ilieva , D. G. ~Ireland , B. S. ~Ishkhanov , E. L. ~Isupov , D. ~Jenkins , H. S. ~Jo , D. ~Keller , M. ~Khachatryan , A. ~Khanal , M. ~Khandaker , A. ~Kim , C. W. ~Kim , W. ~Kim , F. J. ~Klein , V. ~Kubarovsky , L. Lanza , M. ~Leali , K. ~Livingston , I . J . D. ~MacGregor , D. ~Marchand , V. ~Mascagna , B. ~McKinnon , T. ~Mineeva , M. ~Mirazita , P. ~Nadel-Turonski , S. ~Nanda , S. ~Niccolai , G. ~Niculescu , M. ~Osipenko , M. ~Paolone , L. L. ~Pappalardo , R. ~Paremuzyan , K. ~Park , E. ~Pasyuk , W. ~Phelps , O. ~Pogorelko , J. W. ~Price , Y. ~Prok , D. ~Protopopescu , M. ~Ripani , D. Riser , A. ~Rizzo , J. ~Rowley , F. ~Sabatié , C. ~Salgado , R. A. ~Schumacher , Y. G. ~Sharabian , U. ~Shrestha , D. ~Sokhan , O. ~Soto , N. ~Sparveris , S. ~Stepanyan , P. ~Stoler , I. I. ~Strakovsky , S. ~Strauch , M. ~Taiuti , J. A. ~Tan , N. ~Tyler , L. ~Venturelli , H. ~Voskanyan , E. ~Voutier , R. Wang , X. ~Wei , M. H. ~Wood , N. ~Zachariou

We study the electromagnetic structure of the nucleon within a hybrid constituent-quark model that comprises, in addition to the $3q$ valence component, also a $3q$+$\pi$ non-valence component. To this aim we employ a Poincar\'e-invariant…

High Energy Physics - Phenomenology · Physics 2016-04-20 Daniel Kupelwieser , Wolfgang Schweiger

We use recent data on K^+ -> pi^+e^+e^-, together with known values for the pion form factor, to derive the kaon electromagnetic form factor for 0 <q^2 <0.125 (GeV/c)^2. The results are then compared with predictions of the Linear sigma…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. Lowe , M. D. Scadron

In the fixed energy environment of the $e^{+}e^{-}$ collider DA$\Phi$NE, KLOE can measure the cross section of the process $e^{+}e^{-} \to hadrons$ as a function of the hadronic system energy using the radiative return method. At energies…

High Energy Physics - Experiment · Physics 2012-08-03 The KLOE Collaboration , B. Valeriani

We utilize precise weak interaction experiments on atomic muon capture and beta decay in the A = 3 nuclei, and take into account the effects of nuclear "anomalous thresholds" to extract the pseudoscalar pi-^3He-^3H coupling parameter,…

Nuclear Theory · Physics 2009-10-30 Nimai C. Mukhopadhyay , K. Junker

We performed a precise calculation of physical quantities related to the axial structure of the nucleon using 2+1 flavor lattice QCD gauge configuration (PACS10 configuration) generated at the physical point with lattice volume larger than…

The electromagnetic form factor of proton is studied following our previous calculation of the anomalous magnetic moment. The non-perturbative term is incorporated to correct the $Q^2$ dependence.

Nuclear Theory · Physics 2019-06-21 Susumu Kinpara

At the Frascati phi-factory DAPHNE the pion formfactor is measured by means of the 'radiative return', i.e. by using events in which one of the collider electrons (positrons) has radiated an initial state radiation photon, lowering in such…

High Energy Physics - Experiment · Physics 2007-05-23 Achim Denig , KLOE collaboration

The level structure of the very neutron rich and unbound $^9$He nucleus has been the subject of significant experimental and theoretical study. Many recent works have claimed that the two lowest energy $^9$He states exist with spins…

We study the annihilation process $p\bar{p} \to \pi^0 e^+ e^-$ within a Regge framework, as a means to provide constraints on timelike nucleon form factors. We present results for the $e^+e^-$ angular distributions and the differential…

High Energy Physics - Phenomenology · Physics 2013-03-11 J. Guttmann , M. Vanderhaeghen