2008
DOI: 10.1007/s00023-008-0355-y
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Tunnel Effect for Kramers–Fokker–Planck Type Operators

Abstract: We consider operators of Kramers-Fokker-Planck type in the semi-classical limit such that the exponent of the associated Maxwellian is a Morse function with two local minima and a saddle point. Under suitable additional assumptions we establish the complete asymptotics of the exponentially small splitting between the first two eigenvalues. RésuméOn considère des opérateurs du type de Kramers-Fokker-Planck dans la limite semi-classique tels que l'exposant du maxwellien associé soit une fonction de Morse avec de… Show more

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Cited by 28 publications
(140 citation statements)
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“…Now this result becomes a direct application of Theorem 11.6 to A := −P/h and we do not need any bounds on the resolvent in the region z > h ω. In [45,46] similar results were obtained for more general operators, for which we do not necessarily have any bound on the resolvent beyond a strip, and the proof was to use microlocal coercivity outside a compact set in slightly weighted L 2 -spaces. Again Theorem 11.6 would give some simplifications.…”
Section: Introductionsupporting
confidence: 59%
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“…Now this result becomes a direct application of Theorem 11.6 to A := −P/h and we do not need any bounds on the resolvent in the region z > h ω. In [45,46] similar results were obtained for more general operators, for which we do not necessarily have any bound on the resolvent beyond a strip, and the proof was to use microlocal coercivity outside a compact set in slightly weighted L 2 -spaces. Again Theorem 11.6 would give some simplifications.…”
Section: Introductionsupporting
confidence: 59%
“…We also let P denote the graph closure of P from S(R 2n ) which coincides with the maximal extension of P in L 2 (see [47,41,45]). We have P ≥ 0 and the spectrum of P is contained in the right half plane.…”
Section: Statement Of the Main Resultsmentioning
confidence: 99%
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“…The principal purpose of the present paper is to apply the spectral results of [12] to obtain a precise information concerning the large time behavior of the heat semigroup generated by the semiclassical Kramers-Fokker-Planck operator P = y · h∂ x − V ′ (x) · h∂ y + γ 2 (−h∂ y + y) · (h∂ y + y) , x, y ∈ R n , γ > 0. (1.1) In fact, as in [12], our main result will be valid for a large class of supersymmetric second order differential operators, including (1.1).…”
Section: Introduction and Statement Of The Main Resultsmentioning
confidence: 99%