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Related papers: Proton spin content from skyrmions

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We investigate the gluon distribution in a proton at very low $x$, both integrated and transverse momentum dependent, using the Laplace transform technique. By accounting for leading and main next-to-leading contributions, we derive compact…

High Energy Physics - Phenomenology · Physics 2026-05-22 G. R. Boroun , Phuoc Ha , A. V. Kotikov , A. V. Lipatov

Self-consistent mean field methods based on phenomenological Skyrme effective interactions are known to exhibit spurious spin and spin-isospin instabilities both at zero and finite temperatures when applied to homogeneous nuclear matter at…

Nuclear Theory · Physics 2010-11-03 N. Chamel , S. Goriely

Recent precision spin-structure data from Jefferson Lab have significantly advanced our knowledge of nucleon structure at low $Q^2$. Results on the neutron spin sum rules and polarizabilities in the low to intermediate $Q^2$ region are…

Nuclear Experiment · Physics 2010-01-15 Jian-ping Chen

In the Skyrme model of nucleons and nuclei, the spin excitation energy of the nucleon is traditionally calculated by a fit of the rigid rotor quantization of spin/isospin of the fundamental Skyrmion (the hedgehog) to the masses of the…

Nuclear Theory · Physics 2016-12-21 C. Adam , J. Sanchez-Guillen , A. Wereszczynski

We investigate some properties of the standard rotator approximation of the SU$(N)\times\,$SU$(N)$ sigma-model in the delta-regime. In particular we show that the isospin susceptibility calculated in this framework agrees with that computed…

High Energy Physics - Theory · Physics 2020-07-15 J. Balog , F. Niedermayer , P. Weisz

A minimal coupling quantum hydrodynamic model of spin-1/2 fermions at the full spin polarization corresponding to a nonlinear Schrodinger equation is considered. The nonlinearity is primarily caused by the Fermi pressure. It provides an…

Quantum Gases · Physics 2021-04-21 Pavel A. Andreev

The nucleon has been used as a laboratory to investigate its own spin structure and Quantum Chromodynamics. New experimental data on nucleon spin structure at low to intermediate momentum transfers combined with existing high momentum…

Nuclear Experiment · Physics 2009-11-11 J. -P. Chen , A. Deur , Zein-Eddine Meziani

Several spin and flavor dependent parameters characterizing the strangeness content of the nucleon have been calculated in the chiral constituent quark model with configuration mixing (\chiCQM_{config}) which is known to provide a…

High Energy Physics - Phenomenology · Physics 2008-11-26 Harleen Dahiya , Manmohan Gupta

The determination of the spin distribution functions for the neutron requires an understanding of the changes induced by a nuclear medium. We present the first estimates of the changes induced in the spin-dependent, valence parton…

Nuclear Theory · Physics 2010-03-26 F. M. Steffens , K. Tsushima , A. W. Thomas , K. Saito

We investigate the weak-interaction emission of spin-1/2 fermions from decaying (and non-decaying) particles endowed with uniform circular motion. The decay of swirling protons and the neutrino- antineutrino emission from circularly moving…

High Energy Physics - Theory · Physics 2007-05-23 George E. A. Matsas , Daniel A. T. Vanzella

From the parton distributions in the infinite momentum frame one finds that only about 30% of the nucleon spin is carried by spins of the valence quarks, which gave rise to the term "spin crisis". Similar results hold for the lowest mesons,…

High Energy Physics - Phenomenology · Physics 2015-06-03 L. Ya. Glozman , C. B. Lang , M. Limmer

We propose a new model for describing baryon semi-leptonic decays for estimating $F$ and $D$ values with explicit breaking effects of both SU(3) and SU(2) flavor symmetry, where all possible SU(3) and SU(2) breaking effects are induced from…

High Energy Physics - Phenomenology · Physics 2008-11-26 T. Yamanishi

Measuring the spin structure of protons and neutrons tests our understanding of how they arise from quarks and gluons, the fundamental building blocks of nuclear matter. At long distances the coupling constant of the strong interaction…

Nuclear Experiment · Physics 2022-01-13 X. Zheng , A. Deur , H. Kang , S. E. Kuhn , M. Ripani , J. Zhang , K. P. Adhikari , S. Adhikari , M. J. Amaryan , H. Atac , H. Avakian , L. Barion , M. Battaglieri , I. Bedlinskiy , F. Benmokhtar , A. Bianconi , A. S. Biselli , S. Boiarinov , M. Bondi , F. Bossu , P. Bosted , W. J. Briscoe , J. Brock , W. K. Brooks , D. Bulumulla , V. D. Burkert , C. Carlin , D. S. Carman , J. C. Carvajal , A. Celentano , P. Chatagnon , T. Chetry , J. -P. Chen , S. Choi , G. Ciullo , L. Clark , P. L. Cole , M. Contalbrigo , V. Crede , A. D'Angelo , N. Dashyan , R. De Vita , M. Defurne , S. Diehl , C. Djalali , V. A. Drozdov , R. Dupre , M. Ehrhart , A. El Alaoui , L. Elouadrhiri , P. Eugenio , G. Fedotov , S. Fegan , R. Fersch , A. Filippi , T. A. Forest , Y. Ghandilyan , G. P. Gilfoyle , K. L. Giovanetti , F. -X. Girod , D. I. Glazier , R. W. Gothe , K. A. Griffioen , M. Guidal , N. Guler , L. Guo , K. Hafidi , H. Hakobyan , M. Hattawy , T. B. Hayward , D. Heddle , K. Hicks , A. Hobart , T. Holmstrom , M. Holtrop , Y. Ilieva , D. G. Ireland , E. L. Isupov , H. S. Jo , K. Joo , S. Joosten , C. D. Keith , D. Keller , A. Khanal , M. Khandaker , C. W. Kim , W. Kim , F. J. Klein , A. Kripko , V. Kubarovsky , L. Lanza , M. Leali , P. Lenisa , K. livingston , E. Long , I. J. D. MacGregor , N. Markov , L. Marsicano , V. Mascagna , B. McKinnon , D. G. Meekins , T. Mineeva , M. Mirazita , V. Mokeev , C. Mullen , P. Nadel-Turonski , K. Neupane , S. Niccolai , M. Osipenko , A. I. Ostrovidov , M. Paolone , L. Pappalardo , K. Park , E. Pasyuk , W. Phelps , S. K. Phillips , O. Pogorelko , J. Poudel , Y. Prok , B. A. Raue , J. Ritman , A. Rizzo , G. Rosner , P. Rossi , J. Rowley , F. Sabatie , C. Salgado , A. Schmidt , R. A. Schumacher , M. L. Seely , Y. G. Sharabian , U. Shrestha , S. Sirca , K. Slifer , N. Sparveris , S. Stepanyan , I. I. Strakovsky , S. Strauch , V. Sulkosky , N. Tyler , M. Ungaro , L. Venturelli , H. Voskanyan , E. Voutier , D. P. Watts , X. Wei , L. B. Weinstein , M. H. Wood , B. Yale , N. Zachariou , Z. W. Zhao

There is no theoretical reason to think that the spin-flip component of the Pomeron is zero. One can measure the spin-flip part using Coulomb-nuclear interference (CNI). Perturbative QCD calculations show that the spin-flip component is…

High Energy Physics - Phenomenology · Physics 2011-04-15 B. Z. Kopeliovich , B. Povh

We show that the conditions which originate the spin and pseudospin symmetries in the Dirac equation are the same that produce equivalent energy spectra of relativistic spin-1/2 and spin-0 particles in the presence of vector and scalar…

Nuclear Theory · Physics 2008-11-26 P. Alberto , A. S. de Castro , M. Malheiro

The free energy and the entropy of magnetic skyrmions with respect to the collinear state are calculated for a (Pt$_{0.95}$Ir$_{0.05}$)/Fe bilayer on Pd(111) via atomistic spin model simulations. The simulations are carried out starting…

Statistical Mechanics · Physics 2021-06-16 Daniel Schick , Markus Weißenhofer , Levente Rózsa , Ulrich Nowak

The proton spin crisis still remains an unsolved problem in particle physics. It is suggested in the literature that the gauge invariant spin and orbital angular momentum of the quark and the gauge invariant total angular momentum of the…

High Energy Physics - Phenomenology · Physics 2019-05-10 Gouranga C Nayak

This talk consists of four parts. In part one, I give an elementary discussion on constructing a Lorentz-invariant spin sum rule for the nucleon. In part two, I discuss a gauge-dependent spin sum rule, explore its relation with the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Xiangdong Ji

In the past few years, a lot of evidences have been accumulated, which indicate that the gluon polarization inside the nucleon is likely to be small at least at the low renormalization scales. On the other hand, the recent lattice QCD…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. Wakamatsu , Y. Nakakoji

The spin structure of the nucleon is analyzed in the framework of a Lorentz-invariant formulation of baryon chiral perturbation theory. The structure functions of doubly virtual Compton scattering are calculated to one-loop accuracy (fourth…

High Energy Physics - Phenomenology · Physics 2009-11-07 Véronique Bernard , Thomas R. Hemmert , Ulf-G. Meißner
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