Abstract
Abstract
We study the discrete spectrum of the two-particle Schrödinger operator
H
̂
μ
λ
(
K
)
,
K
∈
T
2
, associated to the Bose–Hubbard Hamiltonian
H
̂
μ
λ
of a system of two identical bosons interacting on site and nearest-neighbor sites in the two dimensional lattice
Z
2
with interaction magnitudes
μ
∈
R
and
λ
∈
R
, respectively. We completely describe the spectrum of
H
̂
μ
λ
(
0
)
and establish the optimal lower bound for the number of eigenvalues of
H
̂
μ
λ
(
K
)
outside its essential spectrum for all values of
K
∈
T
2
. Namely, we partition the (μ, λ)-plane such that in each connected component of the partition the number of bound states of
H
̂
μ
λ
(
K
)
below or above its essential spectrum cannot be less than the corresponding number of bound states of
H
̂
μ
λ
(
0
)
below or above its essential spectrum.
Funder
Austrian Science Fund
Foundation for Basic Research of the Republic of Uzbekistan
Subject
General Physics and Astronomy,Mathematical Physics,Modeling and Simulation,Statistics and Probability,Statistical and Nonlinear Physics
Cited by
14 articles.
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