Proton-Neutron Mass Difference in a Unified Gauge Model of Leptons and Hadrons

1973 ◽  
Vol 7 (2) ◽  
pp. 459-465 ◽  
Author(s):  
T. Hagiwara ◽  
Benjamin W. Lee
Keyword(s):  
1976 ◽  
Vol 31 (11) ◽  
pp. 1429-1430
Author(s):  
Satya N. Sinha

Abstract Pion mass difference has been calculated in the renormalizable gauge model of Bars-Halpern-Yoshimura. It is found that the soft pion mass difference is finite in the lowest order perturbative calculation, similar to the result obtained in the unified model of Salam-Weinberg. The mass difference of Kaon has also been discussed.


Author(s):  
Steven E. Vigdor

Chapter 4 deals with the stability of the proton, hence of hydrogen, and how to reconcile that stability with the baryon number nonconservation (or baryon conservation) needed to establish a matter–antimatter imbalance in the infant universe. Sakharov’s three conditions for establishing a matter–antimatter imbalance are presented. Grand unified theories and experimental searches for proton decay are described. The concept of spontaneous symmetry breaking is introduced in describing the electroweak phase transition in the infant universe. That transition is treated as the potential site for introducing the imbalance between quarks and antiquarks, via either baryogenesis or leptogenesis models. The up–down quark mass difference is presented as essential for providing the stability of hydrogen and of the deuteron, which serves as a crucial stepping stone in stellar hydrogen-burning reactions that generate the energy and elements needed for life. Constraints on quark masses from lattice QCD calculations and violations of chiral symmetry are discussed.


2021 ◽  
Vol 103 (6) ◽  
Author(s):  
Z. Ge ◽  
T. Eronen ◽  
A. de Roubin ◽  
D. A. Nesterenko ◽  
M. Hukkanen ◽  
...  

2021 ◽  
Vol 2021 (1) ◽  
Author(s):  
Hyun Min Lee

Abstract Motivated by the recent excess in the electron recoil from XENON1T experiment, we consider the possibility of exothermic dark matter, which is composed of two states with mass splitting. The heavier state down-scatters off the electron into the lighter state, making an appropriate recoil energy required for the Xenon excess even for the standard Maxwellian velocity distribution of dark matter. Accordingly, we determine the mass difference between two component states of dark matter to the peak electron recoil energy at about 2.5 keV up to the detector resolution, accounting for the recoil events over ER = 2 − 3 keV, which are most significant. We include the effects of the phase-space enhancement and the atomic excitation factor to calculate the required scattering cross section for the Xenon excess. We discuss the implications of dark matter interactions in the effective theory for exothermic dark matter and a massive Z′ mediator and provide microscopic models realizing the required dark matter and electron couplings to Z′.


2010 ◽  
Vol 3 ◽  
pp. 06008 ◽  
Author(s):  
U.-G. Meißner ◽  
A.M. Rakhimov ◽  
A. Wirzba ◽  
U.T. Yakhshiev

1981 ◽  
Vol 23 (4) ◽  
pp. 1713-1716 ◽  
Author(s):  
T. Saito ◽  
T. Toriyama ◽  
M. Kanbe ◽  
K. Hisatake
Keyword(s):  

1983 ◽  
Vol 225 (4) ◽  
pp. 505-522 ◽  
Author(s):  
Hiroshi Hasegawa ◽  
Sung-Kil Yang

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