scholarly journals Large mass limit of the continuum theories in Kaplan’s formulation

1994 ◽  
Vol 50 (8) ◽  
pp. 5365-5378 ◽  
Author(s):  
Teruhiko Kawano ◽  
Yoshio Kikukawa
1961 ◽  
Vol 463 (3-4) ◽  
pp. 121-136 ◽  
Author(s):  
R. S. Krishnan ◽  
E. S. Rajagopal

2000 ◽  
Vol 15 (29) ◽  
pp. 4655-4679 ◽  
Author(s):  
DANIEL G. BARCI ◽  
C. A. LINHARES ◽  
A. F. DE QUEIROZ ◽  
J. F. MEDEIROS NETO

We analyze the universality of the bosonization rules in nonrelativistic fermionic systems in (2+1)d. We show that, in the case of linear fermionic dispersion relations, a general fermionic theory can be mapped into a gauge theory in such a way that the fermionic density maps into a magnetic flux and the fermionic current maps into a transverse electric field. These are universal rules in the sense that they remain valid whatever the interaction considered. We also show that these rules are universal in the case of nonlinear dispersion relations provided we consider only density–density interactions. We apply the functional bosonization formalism to a nonrelativistic and nonlocal massive Thirring-like model and evaluate the spectrum of collective excitations in several limits. In the large mass limit, we are able to exactly calculate this spectrum for arbitrary density–density and current–current interactions. We also analyze the massless case and show that it has no collective excitations for any density–density potential in the Gaussian approximation. Moreover, the presence of current interactions may induce a gapless mode with a linear dispersion relation.


2018 ◽  
Vol 96 (9) ◽  
pp. 1004-1009 ◽  
Author(s):  
M.A. Valuyan

In this study, the Casimir energy for massive scalar field with periodic boundary condition was calculated on spherical surfaces with S1, S2, and S3 topologies. To obtain the Casimir energy on a spherical surface, the contribution of the vacuum energy of Minkowski space is usually subtracted from that of the original system. In the large mass limit for surface S2, however, some divergences would eventually remain in the obtained result. To remove these remaining divergences, a secondary renormalization program was manually performed. In the present work, a direct approach for calculation of the Casimir energy has been introduced. In this approach, two similar configurations were considered and then the vacuum energies of these configurations were subtracted from each other. This method provides more physical meaning than the other common methods. Additionally, in the large mass limit for surface S2, it provides a situation in which the second renormalization program is automatically conducted in the calculation procedure, and there was no longer a need to do so manually. Finally, by plotting the obtained values for the Casimir energy of the topologies and investigating their appropriate limits, the logic agreement between the results of our scheme and those of previous studies was discussed.


2007 ◽  
Vol 46 (10) ◽  
pp. 2560-2590 ◽  
Author(s):  
D. Bettinelli ◽  
R. Ferrari ◽  
A. Quadri

1992 ◽  
Vol 381 (1-2) ◽  
pp. 222-280 ◽  
Author(s):  
G. Giavarini ◽  
C.P. Martin ◽  
F. Ruiz Ruiz

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