$$1/(N - 1)$$ Expansion for an SU(N) Impurity Anderson Model: A New Large-N Scheme Based on a Perturbation Theory in U

Author(s):  
Akira Oguri ◽  
Rui Sakano ◽  
Tatsuya Fujii
1990 ◽  
Vol 76 (10) ◽  
pp. 1177-1181 ◽  
Author(s):  
Giuseppe E. Santoro ◽  
Gabriele F. Giuliani

1992 ◽  
Vol 07 (29) ◽  
pp. 7305-7338 ◽  
Author(s):  
A.N. IVANOV ◽  
M. NAGY ◽  
N.I. TROITSKAYA

The chiral perturbation theory is developed at the quark level within the extended Nambu-Jona-Lasinio model, which we used for the low-energy approximation of QCD in the leading order of the large N expansion. In terms of constituent-quark loop diagrams we analyze all of the main low-energy effects caused by the first order corrections in the current-quark-mass expansions. For the correct description of the η→3π decays we confirm the important role of the final-state interaction quoted by Gasser and Leutwyler.


1985 ◽  
Vol 47-48 ◽  
pp. 257-259 ◽  
Author(s):  
Richard M. Martin ◽  
J.W. Allen
Keyword(s):  

2001 ◽  
Vol 16 (27) ◽  
pp. 1761-1773
Author(s):  
OLINDO CORRADINI ◽  
ALBERTO IGLESIAS ◽  
ZURAB KAKUSHADZE ◽  
PETER LANGFELDER

We discuss nonconformal nonsupersymmetric large-N gauge theories with vanishing vacuum energy density to all orders in perturbation theory. These gauge theories can be obtained via a field theory limit of type IIB D3-branes embedded in orbifolded space–times. We also discuss gravity in this setup.


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