Abstract
We derive semiclassical upper bounds for the number of bound states and the sum of negative eigenvalues of the one-particle Hamiltoniansh=f(−i∇)+V(x) acting onL 2(ℝn). These bounds are then used to derive a lower bound on the kinetic energy\(\sum\limits_{j = 1}^N {\left\langle {\psi ,f( - i\nabla _j )\psi } \right\rangle }\) for anN-fermion wavefunction ψ. We discuss two examples in more detail:f(p)=|p| andf(p)=(p 2+m 2)1/2−m, both in three dimensions.
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Communicated by B. Simon
Work parially supported by US National Science Foundation Grant PHY-8116101-A01
On leave from Vrije Universiteit Brussel, and Interuniversitair Instituut voor Kernwetenschappen, Belgium
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Daubechies, I. An uncertainty principle for fermions with generalized kinetic energy. Commun.Math. Phys. 90, 511–520 (1983). https://doi.org/10.1007/BF01216182
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DOI: https://doi.org/10.1007/BF01216182