Resonance widths for the molecular predissociation

preprint2012arXivOpen access

Abstract

We consider a semiclassical 2×22\times 2 matrix Schrödinger operator of the form P=−h2ΔI2+diag(V1(x),V2(x))+hR(x,hDx)P=-h^2Δ{\bf I}_2 + {\rm diag}(V_1(x), V_2(x)) +hR(x,hD_x), where V1,V2V_1, V_2 are real-analytic, V2V_2 admits a non degenerate minimum at 0, V1V_1 is non trapping at energy V2(0)=0V_2(0)=0, and R(x,hDx)=(rj,k(x,hDx))1≤j,k≤2R(x,hD_x)=(r_{j,k}(x,hD_x))_{1\leq j,k\leq 2} is a symmetric off-diagonal 2×22\times 2 matrix of first-order pseudodifferential operators with analytic symbols. We also assume that V1(0)>0V_1(0) >0. Then, denoting by e1e_1 the first eigenvalue of $-Δ+ \la V_2"(0)x,x\ra /2$, and under some ellipticity condition on r1,2r_{1,2} and additional generic geometric assumptions, we show that the unique resonance ρ1ρ_1 of PP such that ρ1=V2(0)+(e1+r2,2(0,0))h+O(h2)ρ_1 = V_2(0) + (e_1+r_{2,2}(0,0))h + {\mathcal O}(h^2) (as h→0+h\rightarrow 0_+) satisfies, ℑρ1=−hn0+(1−nΓ)/2f(h,ln⁡1h)e−2S/h, \Im ρ_1 = -h^{n_0+(1-n_Γ)/2}f(h,\ln\frac1{h})e^{-2S/h}, where f(h,ln⁡1h)∼∑0≤m≤ℓfℓ,mhℓ(ln⁡1h)mf(h,\ln\frac1{h}) \sim \sum_{0\leq m\leq\ell} f_{\ell,m}h^\ell(\ln\frac1{h})^m is a symbol with f0,0>0f_{0,0}>0, S>0S>0 is the so-called Agmon distance associated with the degenerate metric max⁡(0,min⁡(V1,V2))dx2\max(0, \min(V_1,V_2))dx^2, between 0 and {V1≤0}\{V_1\leq 0\}, and n0≥1n_0\geq 1, nΓ≥0n_Γ\geq 0 are integers that depend on the geometry.

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