Fluctuation-induced forces in critical fluids

M Krech - Journal of Physics: Condensed Matter, 1999 - iopscience.iop.org
The current knowledge about fluctuation-induced long-ranged forces is summarized.
Reference is made in particular to fluids near critical points, for which some new insight has …

[图书][B] Ten physical applications of spectral zeta functions

E Elizalde - 2012 - Springer
The years elapsed since the First Edition was issued have witnessed an impressive
evolution of some of the applications here considered, maybe not so of the mathematical …

[图书][B] Spectral functions in mathematics and physics

K Kirsten - 2001 - taylorfrancis.com
The literature on the spectral analysis of second order elliptic differential operators contains
a great deal of information on the spectral functions for explicitly known spectra. The same is …

Heat kernel coefficients of the Laplace operator on the D‐dimensional ball

M Bordag, E Elizalde, K Kirsten - Journal of Mathematical Physics, 1996 - pubs.aip.org
We present a very quick and powerful method for the calculation of heat kernel coefficients. It
makes use of rather common ideas, as integral representations of the spectral sum, Mellin …

Resource letter CF-1: Casimir force

SK Lamoreaux - American Journal of Physics, 1999 - ui.adsabs.harvard.edu
Resource Letter CF-1: Casimir Force - NASA/ADS Now on home page ads icon ads Enable full
ADS view NASA/ADS Resource Letter CF-1: Casimir Force Lamoreaux, SK Abstract This …

Nucleation rates in flat and curved space

J Garriga - Physical Review D, 1994 - APS
Nucleation rates for tunneling processes in Minkowski and de Sitter space are investigated,
taking into account one loop prefactors. In particular, we consider the creation of membranes …

Analysis of an inhomogeneous generalized Epstein–Hurwitz zeta function with physical applications

E Elizalde - Journal of Mathematical Physics, 1994 - pubs.aip.org
The inhomogeneous generalized (Epstein–Hurwitz‐like) multidimensional series E m (s; a
1,..., am; c 1,..., cm; c 2)≡∑ n 1,..., nm= 0∞[a 1 (n 1+ c 1) 2+...+ am (nm+ cm) 2+ c 2]− s is …

Bulk versus boundary (gravitational Casimir) effects in the quantum creation of an inflationary brane-world universe

S Nojiri, SD Odintsov, S Zerbini - Classical and Quantum Gravity, 2000 - iopscience.iop.org
The role of bulk matter quantum effects (via the corresponding effective potential discussed
using the example of a conformal scalar) and of boundary matter quantum effects (via the …

Casimir energy of massless fermions in the slab-bag

RDM De Paola, RB Rodrigues… - Modern Physics Letters …, 1999 - World Scientific
The zero-point energy of a massless fermion field in the interior of two parallel plates in a D-
dimensional space–time at zero temperature is calculated. In order to regularize the model …

Instantons for vacuum decay at finite temperature in the thin wall limit

J Garriga - Physical Review D, 1994 - APS
In N+ 1 dimensions, false vacuum decay at zero temperature is dominated by the O (N+ 1)-
symmetric instanton, a sphere of radius R 0, whereas at temperatures T≫ R 0− 1, the decay …