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KALIKOW-TYPE DECOMPOSITION FOR MULTICOLOR INFINITE RANGE PARTICLE SYSTEMS
(Inst Mathematical StatisticsClevelandEUA, 2013)
Perfect fluids: Field-theoretical description and gauge symmetry issue
(1999)
We show that combinations of (in general, non-linear) two-and three-form fields, analogous to the Maxwell (one-form) field, completely describe perfect fluids, including the rotating ones. In the non-rotating case, the ...
Perfect fluids: Field-theoretical description and gauge symmetry issue
(1999)
We show that combinations of (in general, non-linear) two-and three-form fields, analogous to the Maxwell (one-form) field, completely describe perfect fluids, including the rotating ones. In the non-rotating case, the ...
Perfect simulation for interacting point processes, loss networks and Ising models
(Elsevier Science BvAmsterdamHolanda, 2002)
Exact relativistic static charged perfect fluid disks
(American Physical SocCollege PkEUA, 2004)
Electromagnetism and perfect fluids interplay in multidimensional spacetimes
(2008)
We consider fields in (D > 2)-dimensional spacetime, whose potential is r-form (skew-symmetric tensor of rank r), the field tensor F being its exterior derivative and the Lagrangian, a function of the quadratic invariant ...
Electromagnetism and perfect fluids interplay in multidimensional spacetimes
(2008)
We consider fields in (D > 2)-dimensional spacetime, whose potential is r-form (skew-symmetric tensor of rank r), the field tensor F being its exterior derivative and the Lagrangian, a function of the quadratic invariant ...
A perfectly conducting surface in electrodynamics with Lorentz symmetry breaking
(2017-10-01)
In this paper we consider a model which exhibits explicit Lorentz symmetry breaking due to the presence of a single background vector vμ coupled to the gauge field. We investigate such a theory in the vicinity of a perfectly ...
Casimir interaction between a perfect conductor and graphene described by the Dirac model
(AMER PHYSICAL SOC, 2009)
We adopt the Dirac model for graphene and calculate the Casimir interaction energy between a plane suspended graphene sample and a parallel plane perfect conductor. This is done in two ways. First, we use the quantum-field-theory ...
n-dimensional FLRW quantum cosmology
(Amer Physical SocCollege PkEUA, 2010)