2014
DOI: 10.1103/physrevd.90.025034
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Thermal effective Lagrangian of generalized electrodynamics in static gravitational fields

Abstract: In this paper we compute the effective Lagrangian of static gravitational fields interacting with thermal fields of generalized electrodynamics at high temperature. We employ the usual Matsubara imaginary-time formalism to obtain a closed form expression to the thermal effective Lagrangian at one-loop and two-loop order, in an arbitrary ω-dimensional spacetime, in which the equivalence between the static hard thermal loops and those with zero external energy momentum is widely explored. Afterwards, the symmetr… Show more

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Cited by 6 publications
(11 citation statements)
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“…[42] that the natural condition in the Bopp-Podolsky electrodynamics is the generalized Lorentz condition, Ω[A] = 1 + a 2 ∂ µ A µ . However, there are alternative gauge conditions that allow the same identification, in particular, and in order to preserve the order of the field equation, the so-called non-mixing gauge term [43,44],…”
Section: Introductionmentioning
confidence: 99%
“…[42] that the natural condition in the Bopp-Podolsky electrodynamics is the generalized Lorentz condition, Ω[A] = 1 + a 2 ∂ µ A µ . However, there are alternative gauge conditions that allow the same identification, in particular, and in order to preserve the order of the field equation, the so-called non-mixing gauge term [43,44],…”
Section: Introductionmentioning
confidence: 99%
“…In this sense, our work implies that the standard cosmological model does not rule out Bopp-Podolsky massive photon gas as a real possibility. This very fact, along with the success of predictions by generalized quantum electrodynamics [23][24][25]28], motivates the continuing study of Bopp-Podolsky theory. In addition, the massive mode of Bopp-Podolsky photon may interact with charged particles present in the cosmic soup [54].…”
Section: Final Remarksmentioning
confidence: 99%
“…Moreover, in Bopp-Podolsky the extra term generates a massive mode which preserves the U (1) gauge invariance without the necessity of introducing new fields. Literature offers references with classical [22] and quantum [23][24][25] developments of Bopp-Podolsky's proposal; some of those works impose bounds on the massive Bopp-Podolsky photon [26][27][28].…”
Section: Introductionmentioning
confidence: 99%
“…Hence, a study of Podolsky equations in the vacuum may shed some light on the question of the existence of monopoles as two Dirac strings (solenoids) have an interaction associated with the Podolsky mass [26]. Besides, the fact that the Podolsky characteristic length is associated with the size of the electron [44] could lead us to explore, by electron-positron scattering, the existence of Maxwell → Podolsky transition from the point of view of a mechanism which breaks the dual symmetry and generate mass. These speculations derive from our ignorance associated with the mechanisms behind the self-interaction of the particles and their sizes and deserve rigorous scientific analysis.…”
Section: Final Remarksmentioning
confidence: 99%