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On the Polyharmonic Operator with a Periodic Potential
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On the Polyharmonic Operator with a
Periodic Potential
O. A. Veliev
Dept. of Math, Fen-Ed. Fak, Dogus University.,
Acibadem, Kadikoy, Istanbul, Turkey,
e-mail: oveliev@dogus.edu.tr
Abstract
In this paper we obtain the asymptotic formulas of arbitrary order for
the Bloch eigenvalues and Bloch functions of the d-dimensional polyhar-
monic operator L(l, q(x)) = (??)l + q(x) with periodic, with respect to
arbitrary lattice, potential q(x), where l ≥ 1 and d ≥ 2. Then we prove
that the number of gaps in the spectrum of the operator L(l, q(x)) is finite.
In particular, taking l = 1, we get the proof of the Bethe -Sommerfeld
conjecture for arbitrary dimension and arbitrary lattice.
1 Introduction
In this paper we consider the operator
L(l, q(x)) = (??)l + q(x), x ∈ Rd, d ≥ 2, l ≥ 1 (1)
with a periodic (relative to a lattice ?) potential q(x) ∈ W s2 (F ), where
s ≥ s0 = 3d?12 (3d+d+2)+ 14d3d+d+6, F ≡ Rd/? is a fundamental domain
of ?. Without loss of generality it can be assumed that the measure μ(F ) of F
is 1 and
∫
F
q(x)dx = 0. Let Lt(l, q(x)) be the operator generated in F by (1)
and the conditions:
u(x+ ω) = ei(t,ω)u(x), ?ω ∈ ?, (2)
where t ∈ F ? ≡ Rd/Γ and Γ is the lattice dual to ?, that is, Γ is the set of all
vectors γ ∈ Rd satisfying (γ, ω) ∈ 2πZ for all ω ∈ ?. It is well-known that the
spectrum of the operator Lt(l, q(x)) consists of the eigenvalues
Λ1(t) ≤ Λ2(t) ≤ ....The function Λn(t) is called n-th band function and its
range An = {Λn(t) : t ∈ F ?} is called the n-th band of the spectrum Spec(L) of
L and Spec(L) = ∪∞n=1An. The eigenfunction Ψn,t(x) of Lt(l, q(x)) correspond-
ing to the eigenvalue Λn(t) is known as Bloch functions. In the case q(x) = 0
these eigenvalues and eigenfunctions are | γ + t |2l and ei(γ+t,x) for γ ∈ Γ.
1
This paper consists of 4 section. First section is the introduction, where we
describe briefly the scheme of this paper and discuss the related papers.
Let the potent
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