2021
DOI: 10.17586/2220-8054-2021-12-6-657-663
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Monotonicity of the eigenvalues of the two-particle Schrödinger operatoron a lattice

Abstract: We consider the two-particle Schrödinger operator H(k), (k ∈ T 3 ≡ (−π, π] 3 is the total quasimomentum of a system of two particles) corresponding to the Hamiltonian of the two-particle system on the three-dimensional lattice Z 3 . It is proved that the number N (k) ≡ N (k (1) , k (2) , k (3) ) of eigenvalues below the essential spectrum of the operator H(k) is nondecreasing function in each k (i) ∈ [0, π], i = 1, 2, 3. Under some additional conditions potential v, the monotonicity of each eigenvalue zn(k) ≡ … Show more

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Cited by 4 publications
(1 citation statement)
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“…In [19], the authors considered the two-particle Schrödinger operator H(k), (k ∈ T 3 ≡ (−π, π] 3 is the total quasimomentum of a system of two particles) corresponding to the Hamiltonian of the two-particle system on the threedimensional lattice Z 3 . It was proved that the number N (k) ≡ N (k (1) , k (2) , k (3) ) of eigenvalues below the essential spectrum of the operator H(k) is a nondecreasing function in each k (i) ∈ [0, π], i = 1, 2, 3.…”
Section: Introductionmentioning
confidence: 99%
“…In [19], the authors considered the two-particle Schrödinger operator H(k), (k ∈ T 3 ≡ (−π, π] 3 is the total quasimomentum of a system of two particles) corresponding to the Hamiltonian of the two-particle system on the threedimensional lattice Z 3 . It was proved that the number N (k) ≡ N (k (1) , k (2) , k (3) ) of eigenvalues below the essential spectrum of the operator H(k) is a nondecreasing function in each k (i) ∈ [0, π], i = 1, 2, 3.…”
Section: Introductionmentioning
confidence: 99%