2011
DOI: 10.48550/arxiv.1110.1155
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Quantizing with a higher time derivative

Abstract: We review the classical and quantum theory of the Pais-Uhlenbeck oscillator as the toy-model for quantizing f (R) gravity theories.

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Cited by 5 publications
(5 citation statements)
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“…and where the P-U coefficients η i can be found in [31] and in (13). Note that the frequencies ω k are the roots of the polynomial equation p(ω k ) = 0, see (8).…”
Section: Arbitrary Nmentioning
confidence: 99%
“…and where the P-U coefficients η i can be found in [31] and in (13). Note that the frequencies ω k are the roots of the polynomial equation p(ω k ) = 0, see (8).…”
Section: Arbitrary Nmentioning
confidence: 99%
“…The Hamiltonians H α,β are derived from E α,β by substitution φ, φ, φ, ... φ in terms of the phase-space variables (20). The Ostrogradsky Hamiltonian and bracket correspond to α = 1, β = −1:…”
Section: Stability Of the Pais-uhlenbeck Oscillatormentioning
confidence: 99%
“…Due to the presence of the C2 term in the action (21), this quantum gravity theory is formally renormalizable but has ghosts in Minkowski background [6]. In the context of a fundamental theory of quantum gravity any presence of ghosts is unacceptable [35] so that the C 2 term may not be allowed. However, in the perturbative framework, when the gravity spectrum is determined by the leading (Einstein-Hilbert) action while all the other higher-derivative terms are considered as the interaction, the presence of the C2 term is not a problem.…”
Section: F (R C) Gravity In Einstein Framementioning
confidence: 99%