1978
DOI: 10.1098/rspa.1978.0060
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Quantum field theory in de Sitter space: renormalization by point-splitting

Abstract: We examine the modes of a scalar field in de Sitter space and construct quantum two-point functions. These are then used to compute a finite stress tensor by the technique of covariant point-splitting. We propose a renormalization ansatz based on the DeWitt-Schwinger expansion, and show that this removes all am biguities previously present in pointsplitting regularization. The results agree in detail with previous work by dimensional regularization, and give rise to an anomalous trace with the conventional coe… Show more

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Cited by 1,038 publications
(494 citation statements)
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“…The mode in (2.11) is generally called the adiabatic mode, which in curved space in many instances is the closest to the usual definition of vacuum in Minkowski space [59,73]. The "in" solution (2.8) can be recognized as the Bunch-Davies vacuum [74,75]. Its asymptotic behavior as k ph → ∞ coincides with the adiabatic mode (2.11), which implies that it is the solution that describes a mode that was in the vacuum at early times.…”
Section: Jhep01(2017)133mentioning
confidence: 99%
“…The mode in (2.11) is generally called the adiabatic mode, which in curved space in many instances is the closest to the usual definition of vacuum in Minkowski space [59,73]. The "in" solution (2.8) can be recognized as the Bunch-Davies vacuum [74,75]. Its asymptotic behavior as k ph → ∞ coincides with the adiabatic mode (2.11), which implies that it is the solution that describes a mode that was in the vacuum at early times.…”
Section: Jhep01(2017)133mentioning
confidence: 99%
“…A much more stringent constraint is obtained from the requirement that the field φ is effectively massless during (at least) the last 50 − 60 inflationary e-foldings so that it receives a superhorizon spectrum of perturbations [42] …”
Section: The Pq Field As Curvatonmentioning
confidence: 99%
“…At first sight this seems hard to imagine, as the Bunch-Davies/HartleHawking vacuum wave function of a massless free scalar is an almost trivial Gaussian at all times [16,17]. Nevertheless, we will show in this paper that it emerges in a very sharp sense.…”
Section: Jhep06(2016)181mentioning
confidence: 88%
“…We can however approximate its logarithm by an integral, taking into account the momentum quantization k i ∈ 2π L Z: 16) where for dS d+1 in the late time limit η 0 → 0, according to (3.9), we have β(k) = The chosen value of the IR cutoff β 0 corresponds to k 0 ≡ 2π L . This integral is easily computed, and we can evaluate the inverse Laplace transform again in saddle point approximation, yielding again a Gumbel distribution: with ψ the digamma function.…”
Section: Ds D+1mentioning
confidence: 99%
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