On the weak coupling limit problem

1989 ◽  
pp. 20-58 ◽  
Author(s):  
L. Accardi ◽  
A. Frigerio ◽  
Yun Gang Lu
Keyword(s):  
Weak Coupling ◽  
Limit Problem ◽  
Weak Coupling Limit

scholarly journals An obstacle to sub-AdS holography for SYK-like models

2021 ◽  
Vol 2021 (3) ◽  
Author(s):  
Pengfei Zhang ◽  
Yingfei Gu ◽  
Alexei Kitaev
Keyword(s):  
Lyapunov Exponent ◽  
Weak Coupling ◽  
Kinetic Coefficient ◽  
Weak Coupling Limit ◽  
Branching Time ◽  
Quasiparticle Lifetime

Abstract We argue that “stringy” effects in a putative gravity-dual picture for SYK-like models are related to the branching time, a kinetic coefficient defined in terms of the retarded kernel. A bound on the branching time is established assuming that the leading diagrams are ladders with thin rungs. Thus, such models are unlikely candidates for sub-AdS holography. In the weak coupling limit, we derive a relation between the branching time, the Lyapunov exponent, and the quasiparticle lifetime using two different approximations.

ENERGY BAND OVERLAPPING IN HIGH-Tc SUPERCONDUCTORS

1996 ◽  
Vol 10 (30) ◽  
pp. 1483-1490 ◽  
Author(s):  
M. MORENO ◽  
R. M. MÉNDEZ-MORENO ◽  
M. A. ORTIZ ◽  
S. OROZCO
Keyword(s):  
Weak Coupling ◽  
Cuprate Superconductors ◽  
Weak Coupling Limit ◽  
Band Model ◽  
Coupling Constant ◽  
High Tc Superconductors ◽  
Energy Bands ◽  
Effective Coupling ◽  
High Tc ◽  
Two Band Model

Multi-band superconductors are analyzed and the relevance of overlapping energy bands to the high-T c of these materials is studied. Within the BCS framework, a two band model with generalized Fermi surface topologies is developed. Values of the overlapped occupancy parameters for typical cuprate superconductors are obtained as a function of the ratio R and the effective coupling constant, λ, in the weak-coupling limit. The overlap scale is of the order or lower than the cutoff (Debye) energy. The typical behavior of the isotope effect is obtained. As these superconductors have transition temperatures above the phonon barrier, the results of this approach are important to the generic understanding of the high-T c superconducting mechanism.

scholarly journals Squeezing noises as weak coupling limit of Hamiltonian system

1991 ◽  
Vol 29 (2) ◽  
pp. 227-256
Author(s):  
L. Accardi ◽  
Y.G. Lu
Keyword(s):  
Hamiltonian System ◽  
Weak Coupling ◽  
Weak Coupling Limit

Exciton Dynamics from Strong to Weak Coupling Limit Illustrated on a Series of Squaraine Dimers

2018 ◽  
Vol 122 (15) ◽  
pp. 8082-8093 ◽  
Author(s):  
Merle I. S. Röhr ◽  
Henning Marciniak ◽  
Joscha Hoche ◽  
Maximilian H. Schreck ◽  
Harald Ceymann ◽  
...  
Keyword(s):  
Weak Coupling ◽  
Weak Coupling Limit ◽  
Exciton Dynamics

On radiative and non-radiative decay times in the weak coupling limit

Physica B+C ◽  
1984 ◽  
Vol 123 (2) ◽  
pp. 131-155 ◽  
Author(s):  
M.F.H. Schuurmans ◽  
J.M.F. van Dijk
Keyword(s):  
Weak Coupling ◽  
Radiative Decay ◽  
Weak Coupling Limit ◽  
Decay Times

A simple analytical eigenvalue calculation for barrier crossing rates in the weak coupling limit

1987 ◽  
Vol 87 (6) ◽  
pp. 3611-3617 ◽  
Author(s):  
Shoichi Okuyama ◽  
David W. Oxtoby
Keyword(s):  
Weak Coupling ◽  
Weak Coupling Limit ◽  
Barrier Crossing

Reorganizing Finite Temperature Field Theory: Part I.: Scalar Field Theory

2001 ◽  
Vol 16 (supp01c) ◽  
pp. 1277-1280 ◽  
Author(s):  
Michael Strickland
Keyword(s):  
Field Theory ◽  
Perturbation Theory ◽  
Temperature Field ◽  
Finite Temperature ◽  
Weak Coupling ◽  
Weak Coupling Limit ◽  
Finite Temperature Field Theory ◽  
Expansion Point ◽  
Perturbative Limit ◽  
Standard Perturbation Theory

I present a method for self-consistently including the effects of screening in finite-temperature field theory calculations. The method reproduces the perturbative limit in the weak-coupling limit and for intermediate couplings this method has much better convergence than standard perturbation theory. The method relies on a reorganization of perturbation theory accomplished by shifting the expansion point used to calculate quantum loop corrections. I will present results from a three-loop calculation within this formalism for scalar λϕ4.

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