2019
DOI: 10.1103/physrevd.100.085014
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Breaking of adiabatic invariance in the creation of particles by electromagnetic backgrounds

Abstract: Particles are spontaneously created from the vacuum by time-varying gravitational or electromagnetic backgrounds. It has been proven that the particle number operator in an expanding universe is an adiabatic invariant. In this paper we show that, in some special cases, the expected adiabatic invariance of the particle number fails in presence of electromagnetic backgrounds. Furthermore, we also show a close relation between the breaking of the adiabatic invariance and the emergence of the axial anomaly.

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Cited by 12 publications
(20 citation statements)
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“…Finally, in section V, we provide an explicit example of the application of the procedure developed in the previous sections to the scalar Schwinger effect in a concrete external potential, the Sauter pulse [1]. In particular, we show explicitly how our method allows for a well defined particle number density of created particles via Schwinger effect at any instant of time, which also agrees in the asymptotic limit with the one obtained in previous works using the asymptotic approach [8,29]. We conclude in section VI with a recap of the main results achieved in this paper.…”
Section: Introductionsupporting
confidence: 72%
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“…Finally, in section V, we provide an explicit example of the application of the procedure developed in the previous sections to the scalar Schwinger effect in a concrete external potential, the Sauter pulse [1]. In particular, we show explicitly how our method allows for a well defined particle number density of created particles via Schwinger effect at any instant of time, which also agrees in the asymptotic limit with the one obtained in previous works using the asymptotic approach [8,29]. We conclude in section VI with a recap of the main results achieved in this paper.…”
Section: Introductionsupporting
confidence: 72%
“…Substitution of this solution (5.5) into (4.37) gives an explicit expression for |β k (t)| 2 as a function of time in terms of hypergeometric functions (indeed, since the derivative of a hypergeometric function is proportional to other hypergeometric function). Thus, using the asymptotic properties of these functions [34], it is straightforward to check that in the asymptotic future t → ∞, when the electric field vanishes, we recover the result of [8,29]:…”
Section: Schwinger Effectmentioning
confidence: 99%
“…The above arguments make it necessary to reconsider the problem of adiabatic regularization for fermions in timevarying electric backgrounds in four dimensions. We will adopt the view of considering A μ of adiabatic order 1, as advocated in [31,35,36,38], and in contrast to the view adopted in [34]. The main reasons, as exposed above, are (i) expected agreement with the Schwinger-DeWitt adiabatic expansion of the two-point function at coincidence; (ii) consistency with the covariant conservation of the energy-momentum tensor when gravity is turned on.…”
Section: A Adiabatic Regularization For Fermions In Two-dimensionsmentioning
confidence: 99%
“…In this context, the most important physical local expectation value is the electric current hj μ i, which also possesses ultraviolet divergences and has to be renormalized in a proper way. Recent discussions on foundational issues related to the particle number density of the created particles, adiabatic invariance, and unitary evolution can be seen in [29][30][31].…”
Section: Introductionmentioning
confidence: 99%
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