Abstract
A time dependent approach to self-adjointness is presented and it is applied to quantum mechanical Hamiltonians which are not semi-bounded. Sufficient conditions are given for self-adjointness of Schrödinger and Dirac Hamiltonians with potentials which are unbounded at infinity. The method is the introduction of an auxiliary operatorN≧0 whose rate of change (commutator with the Hamiltonian) is bounded by a multiple ofN.
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Faris, W.G., Lavine, R.B. Commutators and self-adjointness of Hamiltonian operators. Commun.Math. Phys. 35, 39–48 (1974). https://doi.org/10.1007/BF01646453
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DOI: https://doi.org/10.1007/BF01646453