scholarly journals Electroweak vacuum instability and renormalized vacuum field fluctuations in Friedmann-Lemaitre-Robertson-Walker background

2018 ◽  
Vol 98 (10) ◽  
Author(s):  
Kazunori Kohri ◽  
Hiroki Matsui
Author(s):  
Serge Reynaud ◽  
Astrid Lambrecht

The Casimir force is an effect of quantum vacuum field fluctuations, with applications in many domains of physics. The ideal expression obtained by Casimir, valid for perfect plane mirrors at zero temperature, has to be modified to take into account the effects of the optical properties of mirrors, thermal fluctuations, and geometry. After a general introduction to the Casimir force and a description of the current state of the art for Casimir force measurements and their comparison with theory, this chapter presents pedagogical treatments of the main features of the theory of Casimir forces for one-dimensional model systems and for mirrors in three-dimensional space.


Author(s):  
Peter W. Milonni

The atom-field interaction is formulated within the fully quantized-field theory, starting from a detailed analysis of the transformation from the fundamental minimal coupling interaction Hamiltonian to the electric dipole Hamiltonian used extensively in quantum optics. Spontaneous emission, radiative level shifts, and the natural radiative lineshape are treated in both the Schrodinger and Heisenberg pictures, with emphasis on the roles of vacuum field fluctuations, radiation reaction, and the fluctuation-dissipation relation between them. The shortcomings of semiclassical radiation theories are discussed.


The electromagnetic field is quantized on the basis of the complete set of spatial modes of a plane dielectric slab of arbitrary thickness and refractive index but infinite transverse dimensions, located in otherwise empty three-dimensional space. The vacuum field fluctuations and spontaneous emission rates are evaluated as functions of position both inside and outside the slab. The source-field operator is derived for emission by atoms inside the slab, in the direction perpendicular to its surfaces. Particular attention is given to the possibility of suppressing spontaneous emission by placing atoms in, or close to, a dielectric slab.


The electromagnetic field is quantized on the basis of the classical spatial modes of a system geometry in which half of space is filled by a dielectric of constant refractive index and the other half of space is empty. The vacuum field fluctuations and spontaneous emission rates are evaluated as functions of position and polarization both inside and outside the dielectric. Particular attention is given to the variations of these quantities in the vicinity of the interface. The source-field operator is derived for emission by atoms inside and outside the dielectric, in the direction perpendicular to the interface.


Author(s):  
Ileana-Cristina Benea-Chelmus ◽  
Francesca Fabiana Settembrini ◽  
Yannick Salamin ◽  
Yuriy Fedoryshyn ◽  
Wolfgang Heni ◽  
...  

2017 ◽  
Vol 880 ◽  
pp. 012064 ◽  
Author(s):  
F Armata ◽  
S Butera ◽  
G Fiscelli ◽  
R Incardone ◽  
V Notararigo ◽  
...  

1989 ◽  
Vol 44 (11) ◽  
pp. 1051-1056 ◽  
Author(s):  
A. O. Barut ◽  
Jonathan P. Dowling

A recently advanced theory of quantum electrodynamics which is not second quantized, but rather based on self-fields is adopted to a relativistic calculation of (g-2). In analogy to classical electrodynamics, radiative corrections are seen as arising from the back reaction of the self-field upon the source. Vacuum field fluctuations, assumed to be the physical cause of radiative correction in standard QED. are absent in the present self-field approach, which recently has been applied to calculate spontaneous emission, Lamb shift, vacuum polarization, and to a non-relativistic calculation of (g-2), all in free space as well as in cavities. We conclude that the self-field of the electron can be consistently considered to be the physical origin of all radiative processes, as an alternative picture to hypothetical vacuum fluctuations


2009 ◽  
Author(s):  
Jean Desforges ◽  
Tahar Ben-Messaoud ◽  
Martin Leblanc ◽  
Serge Gauvin ◽  
M. R. Singh ◽  
...  

Sign in / Sign up

Export Citation Format

Share Document