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Mass formula

About: Mass formula is a research topic. Over the lifetime, 1248 publications have been published within this topic receiving 22043 citations.


Papers
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Journal ArticleDOI
TL;DR: In this paper, a semi-empirical mass formula for all medium and heavy nuclei has been used to analyze experimental results of mass measurements for both medium and light nuclei.
Abstract: Experimental results of mass measurements for all medium and heavy nuclei have been analyzed using a semiempirical mass formula. The analysis indicates the existence of a universal dependence on the neutron number for the shell-effects term in the neutron separation energies, and the existence of a similar universal dependence on the proton number for the shell-effects term in proton separation energies.

2 citations

Book ChapterDOI
J. J. Sakurai1
01 Jan 1982
TL;DR: In this article, all the low-energy successes of the standard electroweak gauge model are shown to follow in a more phenomenological model based on global SU(2) broken by γ-W° mixing.
Abstract: All the low-energy successes of the standard electroweak gauge model are shown to follow in a more phenomenological model based on global SU(2) broken by γ-W° mixing. Weinberg’s mass predictions need not be valid. Connections with recent composite models of W and Z are also discussed.

2 citations

Posted Content
TL;DR: In this article, the authors proposed the body center cubic quark lattice model and showed that the system of 3 excited quarks is a baryon, and deduced the spectrum in terms of the sum laws.
Abstract: From the Dirac sea concept, the BCC model infers that the quarks u and d constitute a body center cubic quark lattice in the vacuum; when a quark $q^*$ is excited from the vacuum, the nearest primitive cell u' and d' is accompanying excited by the quark $q^*$. Using the energy band theory, the model deduces the quantum numbers (I, S, C, b, and Q) and the masses of all quarks using a united mass formula. Then, it shows that the system of} 3 excited quarks ($q^*u'd'$$) is a baryon, and it deduces the baryon spectrum in terms of the sum laws. This theoretical baryon spectrum is in accordance with the experimental results. It also shows that there are only two elementary quarks (u and d), while the other quarks (s, c, b, ...) are the excited states of the elementary quarks, hence the SU(3) (u, d, and s), the SU(4) (u, d, s, and c), and the SU(5) (u, d, s, c, and b) are the natural extensions of the SU(2) (u and d). The BCC model provides the physical foundation (quarks, SU(N) groups, and that a baryon is made of 3 quarks) for the Quark Model. The Quark Model is the SU(N) approximation of the BCC model. The confinement concept is not needed in the BCC model, because it is replaced by the accompanying excitation concept. The SU(N)} groups are also not} necessary, as they are replaced by the body center cubic groups. We also predict some new baryons: }$\Lambda(2560)$, $\Sigma_{C}(2280)$, $\Omega^{-}(3720)$, $\Lambda_{C}^{+}(6600)$, $\Lambda_{b}^{0}(9960)$...

2 citations

Journal ArticleDOI
M. Yamazaki1
TL;DR: The Christodoulou-Ruffini mass formula of a black hole also holds true in case of the charged Kerr-Tomimatsu-Sato family of fields with arbitrary odd δ.

2 citations


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Performance
Metrics
No. of papers in the topic in previous years
YearPapers
20235
202212
202113
202025
201917
201823