Abstract
The most known trace formula in mathematical physics is certainly the Gutzwiller trace formula linking the eigenvalues of the Schrödinger operator \(\hat{H}\) as Planck’s constant goes to zero (the semi-classical régime) with the closed orbits of the corresponding classical mechanical system. Gutzwiller gave a heuristic proof of this trace formula, using the Feynman integral representation for the propagator of \(\hat{H}\). In mathematics this kind of trace formula was first known as Poisson formula. It was proved first for the Laplace operator on a compact manifold, then for more general elliptic operators using the theory of Fourier-integral operators. Our goal here is to show how the use of coherent states allows us to give a rather simple and direct rigorous proof.
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- 1.
See the definition in Sect. 5.2.
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Combescure, M., Robert, D. (2012). Trace Formulas and Coherent States. In: Coherent States and Applications in Mathematical Physics. Theoretical and Mathematical Physics. Springer, Dordrecht. https://doi.org/10.1007/978-94-007-0196-0_5
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