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Related papers: Valence Neutron-Proton Orientation in Atomic Nucle…

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We give an interpretation of the $u$ and $d$ quarks contributions to the nucleon electromagnetic form factors for values of the four-momentum transfer in the multi-GeV region where flavor separated data have been recently made available.…

High Energy Physics - Phenomenology · Physics 2015-06-05 J. Osvaldo Gonzalez-Hernandez , Simonetta Liuti , Gary R. Goldstein , Kunal Kathuria

We study the flow harmonic distribution in deformed nuclei. To do this, we use the standard Gram-Charlier method to find the higher-order correction to the well-known Bessel-Gaussian distribution. We find that, apart from the necessity of…

Nuclear Theory · Physics 2023-01-20 Hadi Mehrabpour , S. M. A. Tabatabaee

Quantum phase transitions between competing ground-state shapes of atomic nuclei with an odd number of protons or neutrons are investigated in a microscopic framework based on nuclear energy density functional theory and the…

Nuclear Theory · Physics 2017-02-17 K. Nomura , T. Nikšić , D. Vretenar

Most atomic nuclei are deformed with a quadrupole shape described by its overall strength $\beta_2$ and triaxiality $\gamma$. The deformation can be accessed in high-energy heavy-ion collisions by measuring the collective flow response of…

Nuclear Theory · Physics 2022-05-04 Jiangyong Jia

A complete characterization of the structure of nuclei can be obtained by combining information arising from inelastic scattering, Coulomb excitation and $\gamma-$decay, together with one- and two-particle transfer reactions. In this way it…

Nuclear Theory · Physics 2015-09-23 A. Idini , G. Potel , F. Barranco , E. Vigezzi , R. A. Broglia

A general expression for the double differential cross section of fluorescence radiation following photorecombination (PRF) of polarized electrons and polarized ions is derived by using usual atomic theory methods and is represented in the…

Atomic Physics · Physics 2009-11-11 A. Kupliauskiene

In heavy nuclei the spatial distribution of protons and neutrons is different. At CERN SPS energies production of $\pi^+$ and $\pi^-$ differs for $pp$, $pn$, $np$ and $nn$ scattering. These two facts lead to an impact parameter dependence…

Nuclear Theory · Physics 2009-11-10 Antoni Szczurek , Piotr Pawlowski

The beam-normal single-spin asymmetry, $B_n$, exists in the scattering of high energy electrons, polarized transverse to their direction of motion, from nuclear targets. To first order, this asymmetry is caused by the interference of the…

Nuclear Experiment · Physics 2015-10-07 Mark Macrae Dalton

Nuclear parton distribution functions (NPDFs) are determined by a global analysis of experimental measurements on structure-function ratios F_2^A/F_2^{A'} and Drell-Yan cross section ratios \sigma_{DY}^A/\sigma_{DY}^{A'}, and their…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. Hirai , S. Kumano , T. -H. Nagai

The study of rotation-alignment of quasiparticles probes sensitively the properties of high-j intruder orbits. The distribution of very high-j orbits, which are consequences of the fundamental spin-orbit interaction, links with the…

Nuclear Theory · Physics 2009-04-28 Falih Al-Khudair , Gui-Lu Long , Yang Sun

The freezing/melting transition is at the heart of many natural and industrial processes. In the classical picture, the transition proceeds via the nucleation of the new phase, which has to overcome a barrier associated to the free energy…

Soft Condensed Matter · Physics 2024-08-28 Patrice Porion , Joël Puibasset

We present a new global QCD analysis of nuclear parton distribution functions and their uncertainties. In addition to the most commonly analyzed data sets for the deep-inelastic scattering of charged leptons off nuclei and Drell-Yan…

High Energy Physics - Phenomenology · Physics 2013-05-30 Daniel de Florian , Rodolfo Sassot , Marco Stratmann , Pia Zurita

The atomic nucleus is composed of two different kinds of fermions, protons and neutrons. If the protons and neutrons did not interact, the Pauli exclusion principle would force the majority fermions (usually neutrons) to have a higher…

Nuclear Experiment · Physics 2014-12-02 O. Hen , M. Sargsian , L. B. Weinstein , E. Piasetzky , H. Hakobyan , D. W. Higinbotham , M. Braverman , W. K. Brooks , S. Gilad , K. P. Adhikari , J. Arrington , G. Asryan , H. Avakian , J. Ball , N. A. Baltzell , M. Battaglieri , A. Beck , S. May-Tal Beck , I. Bedlinskiy , W. Bertozzi , A. Biselli , V. D. Burkert , T. Cao , D. S. Carman , A. Celentano , S. Chandavar , L. Colaneri , P. L. Cole , V. Crede , A. DAngelo , R. De Vita , A. Deur , C. Djalali , D. Doughty , M. Dugger , R. Dupre , H. Egiyan , A. El Alaoui , L. El Fassi , L. Elouadrhiri , G. Fedotov , S. Fegan , T. Forest , B. Garillon , M. Garcon , N. Gevorgyan , Y. Ghandilyan , G. P. Gilfoyle , F. X. Girod , J. T. Goetz , R. W. Gothe , K. A. Griffioen , M. Guidal , L. Guo , K. Hafidi , C. Hanretty , M. Hattawy , K. Hicks , M. Holtrop , C. E. Hyde , Y. Ilieva , D. G. Ireland , B. I. Ishkanov , E. L. Isupov , H. Jiang , H. S. Jo , K. Joo , D. Keller , M. Khandaker , A. Kim , W. Kim , F. J. Klein , S. Koirala , I. Korover , S. E. Kuhn , V. Kubarovsky , P. Lenisa , W. I. Levine , K. Livingston , M. Lowry , H. Y. Lu , I. J. D. MacGregor , N. Markov , M. Mayer , B. McKinnon , T. Mineeva , V. Mokeev , A. Movsisyan , C. Munoz Camacho , B. Mustapha , P. Nadel-Turonski , S. Niccolai , G. Niculescu , I. Niculescu , M. Osipenko , L. L. Pappalardo , R. Paremuzyan , K. Park , E. Pasyuk , W. Phelps , S. Pisano , O. Pogorelko , J. W. Price , S. Procureur , Y. Prok , D. Protopopescu , A. J. R. Puckett , D. Rimal , M. Ripani , B. G. Ritchie , A. Rizzo , G. Rosner , P. Rossi , P. Roy , F. Sabatie , D. Schott , R. A. Schumacher , Y. G. Sharabian , G. D. Smith , R. Shneor , D. Sokhan , S. S. Stepanyan , S. Stepanyan , P. Stoler , S. Strauch , V. Sytnik , M. Taiuti , S. Tkachenko , M. Ungaro , A. V. Vlassov , E. Voutier , D. Watts , N. K. Walford , X. Wei , M. H. Wood , S. A. Wood , N. Zachariou , L. Zana , Z. W. Zhao , X. Zheng , I. Zonta

Isoscalar Cooper pairing in isospin asymmetric nuclear matter occurs between states populating two distinct Fermi surfaces, each for neutrons and protons. The transition from a BCS-like to the normal (unpaired) state, as the isospin…

Nuclear Theory · Physics 2009-11-07 Herbert Müther , Armen Sedrakian

Nuclear parton distribution functions are obtained by a chi^2 analysis of lepton deep inelastic experimental data. It is possible to determine valence-quark distributions at medium x and antiquark distributions at small x; however, the…

High Energy Physics - Phenomenology · Physics 2017-08-23 S. Kumano

We introduce the concept of the nucleon energy correlators, a set of novel objects that encode the microscopic details of a nucleon, such as the parton angular distribution in a nucleon, the collinear splitting to all orders, as well as the…

High Energy Physics - Phenomenology · Physics 2023-03-08 Xiaohui Liu , Hua Xing Zhu

At a low resolution scale with $Q^2={\mu}^2$ corresponding to the nucleon bound state; deep inelastic unpolarized structure functions $F_1(x,{\mu}^2)$ and $F_2(x,{\mu}^2)$ are derived with correct support using the symmetric part of the…

High Energy Physics - Phenomenology · Physics 2014-11-17 N. Barik , R. N. Mishra

Deep-inelastic $e/\mu$ scattering data off targets ranging from deuterium to lead indicate that the nuclear modifications to the structure functions of bound nucleons are minimal in the kinematic region around the peak of the valence quark…

Nuclear Theory · Physics 2026-04-28 S. A. Kulagin , R. Petti

A symmetry-preserving analysis of strong interaction quantum field equations is used to complete a unified treatment of pion, kaon, nucleon electromagnetic and gravitational form factors. Findings include a demonstration that the pion…

High Energy Physics - Phenomenology · Physics 2024-10-10 Z. -Q. Yao , Y. -Z. Xu , D. Binosi , Z. -F. Cui , M. Ding , K. Raya , C. D. Roberts , J. Rodríguez-Quintero , S. M. Schmidt

Using the NMC and E665 nuclear structure function ratios $F_2^A/F_2^D$ and $F_2^A/F_2^{C}$ from deep inelastic lepton-nucleus collisions, and the E772 Drell--Yan dilepton cross sections from proton-nucleus collisions, and incorporating…

High Energy Physics - Phenomenology · Physics 2014-11-17 K. J. Eskola , V. J. Kolhinen , P. V. Ruuskanen
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