2006
DOI: 10.1063/1.2168124
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Upper and lower bounds for an eigenvalue associated with a positive eigenvector

Abstract: When an eigenvector of a semi-bounded operator is positive, we show that a remarkably simple argument allows to obtain upper and lower bounds for its associated eigenvalue. This theorem is a substantial generalization of Barta-like inequalities and can be applied to non-necessarily purely quadratic Hamiltonians. An application for a magnetic Hamiltonian is given and the case of a discrete Schrödinger operator is also discussed. It is shown how this approach leads to some explicit bounds on the ground-state ene… Show more

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Cited by 4 publications
(8 citation statements)
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“…We did not find this problem listed in the more or less classical geometrical optimization problems posed in R 3 [1,51]. The following partial results have been obtained in ( [47], Sect. IV.B):…”
Section: Problem Minimization Of An Energy For a General Coulombian Pmentioning
confidence: 69%
See 3 more Smart Citations
“…We did not find this problem listed in the more or less classical geometrical optimization problems posed in R 3 [1,51]. The following partial results have been obtained in ( [47], Sect. IV.B):…”
Section: Problem Minimization Of An Energy For a General Coulombian Pmentioning
confidence: 69%
“…As interesting as the approximate resolution of (P N ) for some values of N , is the asymptotic behavior of the optimal value and solution sets of (P N ) when N → +∞. In that respect, the following general conjecture was posed in [47]:…”
Section: Problem Minimization Of An Energy For a General Coulombian Pmentioning
confidence: 99%
See 2 more Smart Citations
“…Besides the variational and perturbative techniques that are mentioned above, there exists a third very general method for approximating the ground-state energy of a quantum system, namely the differential method (see [15,16, and references therein for a historical track]) whose starting point is recalled in section 2. for the sake of completeness. As for the variational methods, the differential method call on a family of trial functions that supposedly mimic the ground-state and that allow for the construction of a function (the average of the Hamiltonian in the former case, the so-called local energy in the latter case) whose absolute extrema within the chosen trial family provide bounds on the exact ground-state energy E 0 .…”
Section: Introductionmentioning
confidence: 99%