Fuzzy bag model: nucleon self-energy due to pion interaction

1984 ◽  
Vol 62 (6) ◽  
pp. 554-561 ◽  
Author(s):  
Y. Nogami ◽  
Akira Suzuki ◽  
Naoko Yamanishi

As pointed out earlier, the pion–quark interaction based on a bag model with a sharp, fixed surface gives rise to the divergence of various quantities such as the nucleon self-energy. This is due to quark excitation in the intermediate states. We examine how this difficulty can be moderated in a "fuzzy bag model" in which the surface is smeared. The nucleon self-energy due to pion interaction converges in the fuzzy bag model. We find, however, that the convergence is quite slow, and the contribution of processes such as [Formula: see text] pair creation, which have not been considered in earlier calculations, is very important.

1987 ◽  
Vol 36 (11) ◽  
pp. 3527-3527 ◽  
Author(s):  
K. G. Horacsek ◽  
Y. Iwamura ◽  
Y. Nogami

1985 ◽  
Vol 32 (11) ◽  
pp. 3001-3009 ◽  
Author(s):  
K. G. Horacsek ◽  
Y. Iwamura ◽  
Y. Nogami

1984 ◽  
Vol 30 (11) ◽  
pp. 2426-2428
Author(s):  
Morihiro Kadoya ◽  
Tadashi Miyazaki
Keyword(s):  

1984 ◽  
Vol 3 (2) ◽  
pp. 231-244 ◽  
Author(s):  
X.H. Yang ◽  
A.K. Kerman
Keyword(s):  

2015 ◽  
Vol 30 (33) ◽  
pp. 1550181 ◽  
Author(s):  
N. N. Achasov ◽  
E. V. Rogozina

Contrary to almost standard opinion that the [Formula: see text]) resonance is the [Formula: see text] molecule or the [Formula: see text] four-quark state, we discuss the scenario where the [Formula: see text] resonance is the [Formula: see text] charmonium which “sits on” the [Formula: see text] threshold. We explain the shift of the mass of the [Formula: see text] resonance with respect to the prediction of a potential model for the mass of the [Formula: see text] charmonium by the contribution of the virtual [Formula: see text] intermediate states into the self energy of the [Formula: see text] resonance. This allows us to estimate the coupling constant of the [Formula: see text] resonance with the [Formula: see text] channel, the branching ratio of the [Formula: see text] decay, and the branching ratio of the [Formula: see text] decay into all non-[Formula: see text] states. We predict a significant number of unknown decays of [Formula: see text] via two gluon: [Formula: see text]. We suggest a physically clear program of experimental researches for verification of our assumption.


2011 ◽  
Vol 08 (05) ◽  
pp. 1007-1019 ◽  
Author(s):  
V. P. NEZNAMOV

The electron self-energy (self-mass) is calculated on the basis of the model of quantum field theory with maximal mass M, developed by V. G. Kadyshevsky et al. within the pseudo-Hermitian quantum electrodynamics in the second order of the perturbation theory. In theory, there is the natural cut-off of large transmitted momentum in intermediate states because of presence of the universal mass M. As a result, the electron self-mass is finite and depends on the transmitted maximum momentum [Formula: see text]. Two interpretations of the obtained results are possible at defined M and A. The first interpretation allows confirming quantitatively the old concept of elementary particle mass sources defined by interaction of particles with self-gauge fields. The second interpretation results in the possibility not to renormalize the mass (at least in the second order of perturbation theory) owing to the zero mass operator ∑(p).


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