Recoil corrections to magnetic moments of octet baryons in the MIT bag model

1983 ◽  
Vol 16 (4) ◽  
pp. 327-330 ◽  
Author(s):  
W-Y. P. Hwang
1988 ◽  
Vol 205 (2-3) ◽  
pp. 128-134 ◽  
Author(s):  
Kazuo Tsushima ◽  
Tetsuya Yamaguchi ◽  
Makoto Takizawa ◽  
Y. Kohyama ◽  
K. Kubodera

1980 ◽  
Vol 22 (3) ◽  
pp. 773-775 ◽  
Author(s):  
S. K. Bose ◽  
L. P. Singh

1988 ◽  
Vol 489 (4) ◽  
pp. 557-611 ◽  
Author(s):  
Kazuo Tsushima ◽  
Tetsuya Yamaguchi ◽  
Y. Kohyama ◽  
K. Kubodera

Author(s):  
Salil Joshi ◽  
Sovan Sau ◽  
Soma Sanyal
Keyword(s):  

1983 ◽  
Vol 27 (11) ◽  
pp. 2708-2714 ◽  
Author(s):  
P. J. Mulders ◽  
G. Bhamathi ◽  
L. Heller ◽  
A. T. Aerts ◽  
A. K. Kerman
Keyword(s):  

2010 ◽  
Vol 81 (1) ◽  
Author(s):  
A. Bhattacharya ◽  
A. Sagari ◽  
B. Chakrabarti ◽  
S. Mani

1997 ◽  
Vol 12 (07) ◽  
pp. 1373-1384 ◽  
Author(s):  
P. R. Silva

An extension of the MIT bag model, developed to describe the strong interaction inside the hadronic matter (nucleons), is proposed as a means to account for the confinement of matter in the universe. The basic hypotheses of the MIT bag model are worked out in a very simplified way and are also translated in terms of the gravitational force. We call the nucleon "microcosmos" and the bag-universe "macrocosmos." We have found a vacuum pressure of 10-15 atm at the boundary of the bag-universe as compared with a pressure of 1029 atm at the boundary of the nucleon. Both universes are also analyzed in the light of Sciama's theory of inertia, which links the inertial mass of a body to its interaction with the rest of the universe. One of the consequences of this work is that the Weinberg mass can be interpreted as a threshold mass, namely the mass where the frequency of the small oscillations of a particle coupled to the universe matches its de Broglie frequency. Finally, we estimate an averaged density of matter in the universe, corresponding to [Formula: see text] of the critical or closure density.


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