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Related papers: The masses of the mesons and baryons. Part IV. Int…

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From the well-known decays of the particles follows that the mesons and baryons consist of a $\gamma$-branch and a neutrino branch. From the well-known masses of the particles follows that the masses of the $\gamma$-branch particles are…

High Energy Physics - Phenomenology · Physics 2007-05-23 E. L. Koschmieder

In order to explain the empirical integer multiple rule for the stable mesons and baryons presented in the preceding paper we assume that the particles are held together in a cubic nuclear lattice. This is a novel approach to the particles,…

High Energy Physics - Lattice · Physics 2007-05-23 E. L. Koschmieder , T. H. Koschmieder

In this paper we give a computation of the mass spectrum of mesons and baryons. By this computation we show that there is a consecutive numbering of the mass spectrum of mesons and baryons. We show that in this numbering many stable mesons…

High Energy Physics - Phenomenology · Physics 2007-05-23 Sze Kui Ng

A mass formula for all the Baryons and Mesons is proposed. A comparison with the actual masses shows that about 63 % of the errors are less than 1 % while in about 93 % of the cases errors are less than 2 %. In all cases the error is less…

General Physics · Physics 2007-05-23 B. G. Sidharth

Empirical mass formulae for the baryon octet and decuplet are presented. These formulae are functions of one integer variable and charge state of the baryons. With an exception of Lambda(1116), the formulae generate masses within 0.1% of…

High Energy Physics - Phenomenology · Physics 2007-05-23 Sung La

We have determined theoretically the rest mass of the muon neutrino at 50 milli-eV and the rest mass of the electron neutrino at 5 meV, as well as, to 1% accuracy, the ratio of the masses of the stable elementary particles which decay by…

High Energy Physics - Lattice · Physics 2007-05-23 E. L. Koschmieder , T. H. Koschmieder

The rest masses of the stable mesons and baryons and the rest masses of their antiparticles, as well as the rest masses of the mu (+,-) and tau (+,-) leptons can be explained, within 1% accuracy, with the standing wave model, which uses…

General Physics · Physics 2007-05-23 E. L. Koschmieder

The rest masses of the electron, the muon and of the stable mesons and baryons can be explained, within 1% accuracy, with the standing wave model, which uses only photons, neutrinos, charge and the weak nuclear force. We do not need…

General Physics · Physics 2009-09-29 E. L. Koschmieder

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

Light-baryon resonances with u,d, and s quarks only can be classified using the non-relativistic quark model. When we assign to baryon resonances with total angular momenta J intrinsic orbital angular momenta L and spin S we make the…

High Energy Physics - Experiment · Physics 2009-11-07 Eberhard Klempt

Sum rules relating the masses of ground-state baryons and mesons are obtained in a constituent quark model. The interaction is assumed to be independent of quark spins except for a spin-dependent part that can be treated as a perturbation.…

High Energy Physics - Phenomenology · Physics 2009-10-28 D. B. Lichtenberg , R. Roncaglia

Masses and decay constants of mesons containing a single $c$ or $b$ quark are described within the framework of heavy-quark symmetry. The $B_s^* - B_s$ and $\bar B^{*0} - \bar B^0$ mass splittings are found equal to within a fraction of an…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jonathan L. Rosner

We present the results of the nucleon and $\Omega$ baryon masses using staggered action for both valence and sea quarks. Three ensembles with the physical pion mass at approximate lattice spacings of $0.15$, $0.12$, and $0.088$fm are…

High Energy Physics - Lattice · Physics 2019-12-03 Ciaran Hughes , Yin Lin , Aaron S. Meyer

Mass differences between octet strange baryons, octet and decuplet strange baryons, and nonet vector mesons and octet baryons of equal strangeness coincide (within the small experimental uncertainties) with the levels of a recently proposed…

General Physics · Physics 2007-05-23 B. F. Riley

This study appertains to the extraction of estimates for the masses and for the partial decay widths to pion-nucleon final states of the well-established (four-star) $s$ and $p$ baryon resonances below $2$ GeV. These estimates are…

High Energy Physics - Phenomenology · Physics 2020-08-18 Evangelos Matsinos

Current measurements of isospin splittings in mesons and baryons are sufficiently precise that they allow estimates of the mass difference between constituent up and down quarks. Some previous results are updated in the light of these new…

High Energy Physics - Phenomenology · Physics 2019-10-23 Marek Karliner , Jonathan L. Rosner

We present results on the masses of the low-lying baryons using ten ensembles of gauge configurations with $N_f =2+1+1$ dynamical twisted mass fermions, at three values of the lattice spacing, spanning a pion mass range from about 210 MeV…

High Energy Physics - Lattice · Physics 2014-12-03 C. Alexandrou , V. Drach , K. Hadjiyiannakou , K. Jansen , C. Kallidonis , G. Koutsou

It is shown that the spin of pi (0), eta, Lambda, Sigma (+,-,0), Xi (-,0), Lambda-c (+), Sigma-c (0), Xi-c (0), and Omega-c (0) mesons and baryons can be explained by the sum of the angular momentum vectors and spin vectors of the…

General Physics · Physics 2007-05-23 E. L. Koschmieder

The effective mass and decay width of the $\phi$ meson in the isospin asymmetric hot and dense resonance matter are studied using the effective Lagrangian framework considering the $\phi K \bar K $ interactions at one-loop level. In…

High Energy Physics - Phenomenology · Physics 2025-05-13 Manpreet Kaur , Arvind Kumar

We show that the mass and width of an unstable particle are precisely defined by the pole in the complex energy plane, $\mu = m - (i/2)\Gamma$, by identifying the width, $\Gamma$, with the particle's decay rate and the mass, $m$, with the…

High Energy Physics - Phenomenology · Physics 2024-02-09 Scott Willenbrock
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