Buslaev, Vladimir; Grigis, Alain Imagrinary parts of Stark-Wannier resonances. (English) Zbl 1001.34075 J. Math. Phys. 39, No. 5, 2520-2550 (1998). Summary: We consider a one-dimensional Stark-Wannier Hamiltonian, \(H=-d^2/dx^2+p(x)-\epsilon x\), \(x\in\mathbb R\), where \(p\) is a smooth periodic, finite-gap potential, and \(\epsilon>0\) is small enough. We compute rigorously the imaginary parts of the spectral resonances. For this purpose we develop some related elements of the adiabatic approach to the equations of the form \(-\psi''+p(x)\psi+q(\epsilon x)\psi=E\psi\), \(\epsilon\to 0\). Cited in 1 ReviewCited in 8 Documents MSC: 34L40 Particular ordinary differential operators (Dirac, one-dimensional Schrödinger, etc.) 81Q20 Semiclassical techniques, including WKB and Maslov methods applied to problems in quantum theory 34L05 General spectral theory of ordinary differential operators 81U05 \(2\)-body potential quantum scattering theory PDF BibTeX XML Cite \textit{V. Buslaev} and \textit{A. Grigis}, J. Math. Phys. 39, No. 5, 2520--2550 (1998; Zbl 1001.34075) Full Text: DOI OpenURL References: [1] Buslaev V. S., Alg. Anal. 23 pp 1– (1989) [2] Buslaev V. S., Math. J. 1 pp 287– (1990) [3] Buslaev V. S., Usp. Mat. Nauk 42 pp 77– (1987) [4] DOI: 10.1016/0003-4916(82)90213-5 [5] DOI: 10.1007/BF01212445 · Zbl 0651.47006 [6] DOI: 10.1007/BF02099175 · Zbl 0743.35053 [7] DOI: 10.1007/BF02099501 · Zbl 0737.34060 [8] DOI: 10.1007/BF02102626 · Zbl 0770.47030 [9] DOI: 10.1007/BF01206948 · Zbl 0493.47009 [10] DOI: 10.1007/BF02100105 · Zbl 0851.34078 [11] DOI: 10.1007/BF01017921 · Zbl 0557.34053 [12] Firsova N. E., Zap. Nauchn. Sem. Leningrad. Otdel. Mat. Inst. Steklov. (LOMI) 51 pp 183– (1975) [13] Marchenko V. A., Mat. Sb. 97 pp 540– (1975) This reference list is based on information provided by the publisher or from digital mathematics libraries. Its items are heuristically matched to zbMATH identifiers and may contain data conversion errors. It attempts to reflect the references listed in the original paper as accurately as possible without claiming the completeness or perfect precision of the matching.