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Coulomb and mass difference corrections to low-energy pion-nucleon scattering are calculated and compared with previous work including potential models, dispersion relation methods and chiral perturbation theory calculations. Particular…

Nuclear Theory · Physics 2011-08-17 W. R. Gibbs , R. Arceo

It is supposed that the electron neutrino mass is related to the structures and masses of the $W^\pm$ and $Z^0$ bosons. Using a composite model of fermions (described elsewhere), it is shown that the massless neutrino is not consistent with…

General Physics · Physics 2007-05-23 V. N. Yershov

Alvarado, Aranda, and Bonilla propose a sub-GeV U(1)R gauge boson model to explain the proton charge radius discrepancy. Their model assumes opposite sign U(1)R charge assignments for up and down quarks in the nucleon. I point out that…

High Energy Physics - Phenomenology · Physics 2022-03-16 Michael J. Longo

We determine theoretically the relation between the total number of protons $N_{p}$ and the mass number $A$ (the charge to mass ratio) of nuclei and neutron cores with the model recently proposed by Ruffini et al. (2007) and we compare it…

Astrophysics · Physics 2009-11-13 Barbara Patricelli , Michael Rotondo , Remo Ruffini

Accepted values of the masses of several subatomic particles have been under debate since recent measurements in Penning traps produced more precise yet incompatible results, implying possible inconsistencies in closely related physical…

Lattice QCD simulations are now reaching a precision where isospin breaking effects become important. Previously, we have developed a program to systematically investigate the pattern of flavor symmetry beaking within QCD and successfully…

High Energy Physics - Lattice · Physics 2016-10-12 R. Horsley , Y. Nakamura , H. Perlt , D. Pleiter , P. E. L. Rakow , G. Schierholz , A. Schiller , R. Stokes , H. Stüben , R. D. Young , J. M. Zanotti

Only photons are needed to explain the masses of the pi(0), eta, Lambda, Sigma(0), Xi(0), Omega(-), Lambda(c,+), Sigma(c,0), Xi(c,0), and Omega(c,0) mesons and baryons. Only neutrinos are needed to explain the mass of the pi(+-) mesons.…

General Physics · Physics 2015-06-26 E. L. Koschmieder

We study the electromagnetic contribution to the proton-neutron mass splitting by combining lattice simulations and the modified Cottingham sum rule of Walker-Loud, Carlson and Miller. This analysis yields an estimate of the isovector…

Nuclear Theory · Physics 2015-03-05 A. W. Thomas , X. G. Wang , R. D. Young

Understanding the differences between the distribution of quarks bound in protons and neutrons is key for constraining the mechanisms of SU(6) spin-flavor symmetry breaking in Quantum Chromodynamics (QCD). While vast amounts of proton…

High Energy Physics - Phenomenology · Physics 2021-04-16 E. P. Segarra , J. R. Pybus , F. Hauenstein , T. Kutz , D. Higinbotham , G. A. Miller , E. Piasetzky , A. Schmidt , M. Strikman , L. B. Weinstein , O. Hen

We compute the electromagnetic mass differences of mesons containing a single heavy quark in terms of measurable data using QCD-based arguments in heavy-quark effective theory. We derive an unsubtracted dispersion relation that shows that…

High Energy Physics - Phenomenology · Physics 2016-09-01 Markus A. Luty , Raman Sundrum

What is the size of the atomic nucleus? This deceivably simple question is difficult to answer. While the electric charge distributions in atomic nuclei were measured accurately already half a century ago, our knowledge of the distribution…

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

The weak interaction contribution to the proton neutron mass difference is computed using a generalization of Cottingham's formula. When included in the analysis of the Eotvos experiment, this contribution reduces the bound on a possible…

High Energy Physics - Phenomenology · Physics 2009-10-31 N. Chamoun , H. Vucetich

General Relativity makes a distinction between mass and space. Mass tells space how to curve and space tells mass how to move. Newtonian gravity equation makes a distinction between them by having its numerator as mass effect and its…

General Physics · Physics 2007-05-23 Shantilal G. Goradia

We study the effect of the splitting of neutron and proton effective masses with isospin asymmetry on the properties of the Skyrme energy density functional. We discuss the ability of the latter to predict observable of infinite matter and…

Nuclear Theory · Physics 2009-11-11 T. Lesinski , K. Bennaceur , T. Duguet , J. Meyer

A method for quantization of the proton mass is here addressed, which provides a plausible explanation for the origin of mass and leads to the unification of mass and electric charge through their coupling. By means of an electromagnetic…

General Physics · Physics 2007-05-23 G. Sardin

The difference between the electromagnetic self-energies of proton and neutron can be calculated with the Cottingham formula, which expresses the self-energies as an integral over the electroproduction cross sections---provided the nucleon…

High Energy Physics - Phenomenology · Physics 2020-03-31 J. Gasser , M. Hoferichter , H. Leutwyler , A. Rusetsky

The ratio between the proton and electron masses is shown to be close to the ratio between the strong and electromagnetic interaction coupling constants at Extremely Low Energy (ELE). Based on the experimental data, this relation has been…

High Energy Physics - Phenomenology · Physics 2010-03-09 Dimitar Valev

We derive constraints on the coupling constants of axion-like particles to nucleons and on the Yukawa-type corrections to Newton's gravitational law from the results of recent experiment on measuring the difference of Casimir forces between…

High Energy Physics - Phenomenology · Physics 2017-07-05 G. L. Klimchitskaya , V. M. Mostepanenko

The X-ray cascade from antiprotonic atoms was studied for 208Pb and 209Bi. Widths and shifts of the levels due to the strong interaction were determined. Using modern antiproton-nucleus optical potentials the neutron densities in the…