2002
DOI: 10.1016/s0550-3213(02)00020-2
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Perturbative approach to higher derivative and nonlocal theories

Abstract: We review a perturbative approach to deal with Lagrangians with higher or infinite order time derivatives. It enables us to construct a consistent Poisson structure and Hamiltonian with only first time derivatives order by order in coupling. We show that, to the lowest order, the Hamiltonian is bounded from below whenever the potential is. We consider spacetime noncommutative field theory as an example.

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Cited by 57 publications
(65 citation statements)
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“…The most immediate possibility to proceed along the lines of maintaining the original number of degrees of freedom x,ẋ, is to simply neglect the acceleration term and compute the corrections to ω to first order in g. Nevertheless, this result does not coincide with the first order expansion of the exact frequency ω to that order. On the other hand, the application of the modified perturbative method proposed in [8] does indeed leads to the correct expression to that order. Moreover, in this simple case, the corrections can be calculated to all orders in g and the sum of this perturbation series can also be performed, leading to the exact expression for ω.…”
Section: Pos(qg-ph)040mentioning
confidence: 88%
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“…The most immediate possibility to proceed along the lines of maintaining the original number of degrees of freedom x,ẋ, is to simply neglect the acceleration term and compute the corrections to ω to first order in g. Nevertheless, this result does not coincide with the first order expansion of the exact frequency ω to that order. On the other hand, the application of the modified perturbative method proposed in [8] does indeed leads to the correct expression to that order. Moreover, in this simple case, the corrections can be calculated to all orders in g and the sum of this perturbation series can also be performed, leading to the exact expression for ω.…”
Section: Pos(qg-ph)040mentioning
confidence: 88%
“…A proof of self-consistency to all orders, in a mechanical setting 2 , is provided in Ref. [8]. It consists in showing that to each order in the expansion parameter, the Lagrangian constructed according to the summary described in the above paragraph reproduces exactly the corresponding equations obtained by the iteration procedure stating from the exact HOTD ones.…”
Section: Pos(qg-ph)040mentioning
confidence: 93%
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