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Related papers: $C_5^A$ form factor from ANL experiment

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We present our progress on the computation of the axial form factor of the nucleon with flavour structure $u+d-2s$ from lattice QCD. We employ a set of $N_f=2+1$ CLS ensembles with $O(a)$-improved Wilson fermions and the L\"uscher-Weisz…

We study the weak interaction axial form factors of the octet baryons, within the covariant spectator quark model, focusing on the dependence of four-momentum transfer squared, Q^2. In our model the axial form factors G_A(Q^2) (axial-vector…

High Energy Physics - Phenomenology · Physics 2016-07-05 G. Ramalho , K. Tsushima

The isovector axial form factor of the nucleon plays a key role in interpreting data from long-baseline neutrino oscillation experiments. We present a lattice QCD calculation of this form factor, introducing a new method to directly extract…

High Energy Physics - Lattice · Physics 2022-12-05 Jonna Koponen , Dalibor Djukanovic , Georg von Hippel , Harvey B. Meyer , Konstantin Ottnad , Tobias Schulz , Hartmut Wittig

We present results for the isovector axial vector form factors obtained using thirteen 2+1+1-flavor highly improved staggered quark (HISQ) ensembles generated by the MILC collaboration. The calculation of nucleon two- and three-point…

High Energy Physics - Lattice · Physics 2024-06-14 Yong-Chull Jang , Rajan Gupta , Tanmoy Bhattacharya , Boram Yoon , Huey-Wen Lin

The theoretical and experimental status of the isovector axial-vector current form factors G_A(q^2) and G_P(q^2) of the nucleon is reviewed. We also describe a new calculation of these form factors in manifestly Lorentz-invariant chiral…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. R. Schindler , S. Scherer

Precise knowledge of the nucleon's axial-current form factors is crucial for modeling GeV-scale neutrino-nucleus interactions. Unfortunately, the axial form factor remains insufficiently constrained to meet the precision requirements of…

Nuclear Theory · Physics 2020-11-04 Xilin Zhang , T. J. Hobbs , Gerald A. Miller

A covariant, composite scalar diquark, Fadde'ev amplitude model for the nucleon is used to calculate pseudoscalar, isoscalar- and isovector-vector, axial-vector and scalar nucleon form factors. The last yields the nucleon sigma-term and…

Nuclear Theory · Physics 2009-01-14 J. C. R. Bloch , C. D. Roberts , S. M. Schmidt

It is well established that the nucleon form factors can be related to Generalized Parton Distributions (GPDs) through sum-rules. On the other hand, GPDs can be expressed in terms of Parton Distribution Functions (PDFs) according to Diehl's…

High Energy Physics - Phenomenology · Physics 2019-07-17 Hadi Hashamipour , Muhammad Goharipour , Siamak S. Gousheh

The feasibility of a measurement of the electric and magnetic nucleon form factors at $B$-meson factories through the radiative return is studied. Angular distributions allow a separation of the contributions from the two form factors. The…

High Energy Physics - Phenomenology · Physics 2010-02-03 Henryk Czyz , Johann H. Kuhn , Elzbieta Nowak , German Rodrigo

We calculate electric and magnetic form factors of protons and neutrons in quenched Monte Carlo lattice QCD on a $16^3\times 24$ lattice at $\beta = 6.0$ using Wilson fermions. We employ a method which characterizes one of the nucleon…

High Energy Physics - Lattice · Physics 2008-11-26 Walter Wilcox , Terrence Draper , Keh-Fei Liu

A new value $b=0.0205\pm0.0017$ fm$^2$ of the slope of the neutron form factor $G_{En}(q^2)$ at $q^2=0$ compatible with deuteron properties has been extracted by using a linear relation between $b$ and $A^2_S(1+\eta^2)$ we found for a class…

Nuclear Theory · Physics 2007-05-23 M. M. Mustafa , E. M. Darwish , E. A. M. Sultan , E. M. Hassan

We extract Compton form factors (CFFs) from deeply virtual Compton scattering measurements at the Thomas Jefferson National Accelerator Facility (JLab) using quantum-inspired deep neural networks (QDNNs). The analysis implements the twist-2…

Machine Learning · Computer Science 2026-04-30 Brandon B. Le , Dustin Keller

We report on a new measurement of the parity-violating asymmetry in quasielastic electron scattering from the deuteron at backward angles at Q2= 0.038 (GeV/c)2. This quantity provides a determination of the neutral weak axial vector form…

Nuclear Experiment · Physics 2014-11-18 SAMPLE collaboration , T. M. Ito

We present results on the nucleon axial vector form factors $G_A(q^2)$ and $G_p(q^2)$ in the quenched theory and using two degenerate flavors of dynamical Wilson fermions for momentum transfer squared from about 0.1 to about 2 GeV^2 and for…

High Energy Physics - Lattice · Physics 2008-11-26 C. Alexandrou , G. Koutsou , Th. Leontiou , J. W. Negele , A. Tsapalis

A relation among the form factors of $<D \mid A_\mu \mid D^*>$ at $q^2 \to 0$ is derived. It is verified to lowest order in both the $1/m_c$ expansion and the expansion in number of derivatives using the effective lagrangian that…

High Energy Physics - Phenomenology · Physics 2020-03-17 Claudio O. Dib , J. Taron

The anapole form factor of the nucleon is calculated in chiral perturbation theory in leading order. To this order, the form factor originates from the pion cloud, and is proportional to the non-derivative parity-violating pion-nucleon…

High Energy Physics - Phenomenology · Physics 2009-10-31 C. M. Maekawa , U. van Kolck

The electric dipole form factor (EDFF) of the nucleon stemming from the QCD theta term and from the quark color-electric dipole moments is calculated in chiral perturbation theory to sub-leading order. This is the lowest order in which the…

High Energy Physics - Phenomenology · Physics 2011-01-27 E. Mereghetti , J. de Vries , W. H. Hockings , C. M. Maekawa , U. van Kolck

We report a calculation of the nucleon axial form factors $G_A^q(Q^2)$ and $G_P^q(Q^2)$ for all three light quark flavors $q\in\{u,d,s\}$ in the range $0\leq Q^2\lesssim 1.2\text{ GeV}^2$ using lattice QCD. This work was done using a single…

Quasielastic neutrino-nucleon scattering is a basic signal process for neutrino oscillation studies. At accelerator energies, the corresponding cross section is subject to significant uncertainty due to the poorly constrained axial-vector…

High Energy Physics - Phenomenology · Physics 2013-05-29 Bhubanjyoti Bhattacharya , Richard J. Hill , Gil Paz

We report the first extraction of the pion-nucleon multipoles near the production threshold for the $n\pi^+$ channel at relatively high momentum transfer ($Q^2$ up to 4.2 $\rm{GeV^2}$). The dominance of the s-wave transverse multipole…

Nuclear Experiment · Physics 2015-06-03 Kijun Park , Ralf Gothe , Krishna Adhikari , Dasuni Adikaram-Mudiyanselage , Marco Anghinolfi , Hovhannes Baghdasaryan , Jacques Ball , Marco Battaglieri , Vitaly Baturin , Ivan Bedlinskiy , Robert Bennett , Angela Biselli , Craig Bookwalter , Sergey Boyarinov , Derek Branford , William Briscoe , William Brooks , Volker Burkert , Daniel Carman , Andrea Celentano , Shloka Chandavar , Gabriel Charles , Philip Cole , Marco Contalbrigo , Volker Crede , Annalisa D'Angelo , Aji Daniel , Natalya Dashyan , Raffaella De Vita , Enzo De Sanctis , Alexandre Deur , Chaden Djalali , David Doughty , Raphael Dupre , Ahmed El Alaoui , Lamiaa Elfassi , Paul Eugenio , Gleb Fedotov , Ahmed Fradi , Marianna Gabrielyan , Nerses Gevorgyan , Gerard Gilfoyle , Kevin Giovanetti , Francois-Xavier Girod , John Goetz , Wesley Gohn , Evgeny Golovach , Lewis Graham , Keith Griffioen , Michel Guidal , Lei Guo , Kawtar Hafidi , Hayk Hakobyan , Charles Hanretty , David Heddle , Kenneth Hicks , Maurik Holtrop , Yordanka Ilieva , David Ireland , Boris Ishkhanov , Evgeny Isupov , David Jenkins , Hyon-Suk Jo , Kyungseon Joo , Mahbubul Khandaker , Puneet Khetarpal , Andrey Kim , Wooyoung Kim , Andreas Klein , Franz Klein , A. Kubarovsky , Valery Kubarovsky , Sebastian Kuhn , Sergey Kuleshov , Nicholas Kvaltine , Kenneth Livingston , Haiyun Lu , Ian MacGregor , Nikolai Markov , Michael Mayer , Bryan McKinnon , Mac Mestayer , Curtis Meyer , Taisiya Mineeva , Marco Mirazita , Viktor Mokeev , Herve Moutarde , Edwin Munevar Espitia , Pawel Nadel-Turonski , Rakhsha Nasseripour , Silvia Niccolai , Gabriel Niculescu , Maria-Ioana Niculescu , Mikhail Osipenko , Alexander Ostrovidov , Michael Paolone , Luciano Pappalardo , Rafayel Paremuzyan , Seungkyung Park , Sergio Pereira , Evan Phelps , Silvia Pisano , Oleg Pogorelko , Sergey Pozdnyakov , John Price , Sebastien Procureur , Yelena Prok , Giovanni Ricco , Dipak Rimal , Marco Ripani , Barry Ritchie , Guenther Rosner , Patrizia Rossi , Franck Sabatie , Mukesh Saini , Carlos Salgado , Diane Schott , Reinhard Schumacher , Heghine Seraydaryan , Youri Sharabian , Elton Smith , Gregory Smith , Daniel Sober , Daria Sokhan , Samuel Stepanyan , Stepan Stepanyan , Paul Stoler , Igor Strakovski , Steffen Strauch , Mauro Taiuti , Wei Tang , Charles Taylor , Ye Tian , Svyatoslav Tkachenko , Arjun Trivedi , Maurizio Ungaro , Brian Vernarsky , Alexander Vlasov , Eric Voutier , Daniel Watts , Dennis Weygand , Michael Wood , Nicholas Zachariou , Bo Zhao , Zhiwen Zhao , N. Kalantarians , C. E. Hyde
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