Monotonicity of the eigenvalues of the two-particle Schrödinger operatoron a lattice
Annotatsiya
We consider the two-particle Schrdinger operator H(k), (k T 3 (-, ] 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, ], i = 1, 2, 3. Under some additional conditions potential v, the monotonicity of each eigenvalue zn(k) zn(k (1) , k (2) , k (3) ) of the operator H(k) in k (i) [0, ] with other coordinates k being fixed is proved.