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   <subfield code="a">Gamow Vectors and Borel Summability in a Class of Quantum Systems</subfield>
   <subfield code="h">[Elektronische Daten]</subfield>
   <subfield code="c">[O. Costin, M. Huang]</subfield>
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   <subfield code="a">We analyze the detailed time dependence of the wave function ψ(x,t) for one dimensional Hamiltonians $H=-\partial_{x}^{2}+V(x)$ where V (for example modeling barriers or wells) and ψ(x,0) are compactly supported. We show that the dispersive part of ψ(x,t) is the Borel sum of its asymptotic series in powers of t −1/2, t→∞. The remainder, the difference between ψ and the Borel sum, i.e., the exponential part of the transseries of ψ, is a convergent expansion of the form $\sum_{k=0}^{\infty}g_{k}\Gamma_{k}(x)e^{-\gamma_{k} t}$ , where Γ k are the Gamow vectors of H, and iγ k are the associated resonances; generically, all g k are nonzero. For large k, γ k ∼const⋅klog k+k 2 π 2 i/4. The effect of the Gamow vectors is visible when time is not very large, and the decomposition defines rigorously resonances and Gamow vectors in a nonperturbative regime, in a physically relevant way. The decomposition allows for calculating ψ for moderate and large t, to any prescribed exponential accuracy, using optimal truncation of power series plus finitely many Gamow vectors contributions. The analytic structure of ψ is perhaps surprising: in general (even in simple examples such as square wells), ψ(x,t) turns out to be C ∞ in t but nowhere analytic on ℝ+. In fact, ψis t-analytic in a sector in the lower half plane and has the whole of ℝ+ a natural boundary. In the dual space, we analyze the resurgent structure of ψ.</subfield>
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   <subfield code="a">Gamow vectors</subfield>
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   <subfield code="a">Costin</subfield>
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   <subfield code="u">Mathematics Department, The Ohio State University, 43210, Columbus, OH, USA</subfield>
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   <subfield code="u">Department of Mathematics, The University of Chicago, 5734 S. University Avenue, 60637, Chicago, IL, USA</subfield>
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   <subfield code="t">Journal of Statistical Physics</subfield>
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   <subfield code="g">144/4(2011-08-01), 846-871</subfield>
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