Threshold phenomenon for a family of the generalized Friedrichs models with the perturbation of rank one Текст научной статьи по специальности «Математика»

ISSN 2074-1871 Уфимский математический журнал. Том 11. № 4 (2019). С. 139-149.

THRESHOLD PHENOMENON FOR A FAMILY OF THE GENERALIZED FRIEDRICHS MODELS WITH THE PERTURBATION OF RANK ONE.

S.N. LAKAEV, M. DARUS, S.T. DUSTOV

Abstract. In this work we consider a family H^(p), p. > 0, p £ T3, of the generalized Friedrichs models with the perturbation of rank one. This system describes a system of two particles moving on the three dimensional lattice Z3 and interacting via a pair of local repulsive potentials. One of the reasons to consider such family of the generalized Friedrichs models is that this family generalizes and involves some important behaviors of the Hamiltonians for systems of both bosons and fermions on lattices. In the work, we study the existence or absence of the eigenvalues of the operator H^(p) located outside the essential spectrum depending on the values of ^ > 0 and p £ Us (p o) C T3. We prove a analytic dependence on the parameters for such eigenvalue and an associated eigenfunction and the latter is found in a certain explicit form. We prove the existence of coupling constant threshold ^ = y(p) > 0 for the operator H^(p), p £ Us(p0), namely, we show that the operator H^(p) has no eigenvalue for all 0 < ^ < ^(p) and there exists a unique eigenvalue z(y, p) for each ^ > ^(p) and this eigenvalue is located above the threshold z = M(p). We find necessary and sufficient conditions allowing us to determine whether the threshold 2 = M(p) is an eigenvalue or a virtual level or a regular point in the essential spectrum of the operator H^(p), p £ Us(p0).

Keywords: coupling constant threshold, repulsive potential, eigenvalue, generalized Friedrichs model, regular point.

Mathematics Subject Classification: 35P15, 47A10

1. Introduction

In the present paper we consider a family of generalized Friedrichs models with rank one perturbations H^(p), ^ > 0,p £ Us(p0) C T3, where Us(p0) is a ^-neighborhood of the point p = p 0 £ T3, This family describes a system of two particles on the three-dimensional lattice Z3 interacting via a pair of local repulsive potentials.

We show that if the parameters of the generalized Friedrichs model satisfy some conditions, there exists a coupling constant threshold ^ = ^(p) > 0 such that the operator H^(p), p £ Us(p0) has no eigenvalue for all 0 < ^ < ^(p) and at the same time, it possesses a unique eigenvalue z(^,p) above the threshold z = M(p) of the essential spectrum for each ^ > ^(p). We find a certain explicit form for an associated eigenfunction and prove its analytic dependence on the parameters. We also find necessary and sufficient conditions determining whether the

S.N.Lakaev, M.Darus, S.T.Dustov, Threshold phenomenon for a family of the generalized Friedrichs models with the perturbation of rank one.

© S.N.Lakaev, M.Darus, S.T.Dustov 2018.

The work was supported by the Fundamental Science Foundation of Uzbekistan (grant no. OT-F4-66) and by the grant no. GUP-2019-032.

Submitted November 6, 2018.

threshold z = M(p) is an eigenvalue or a virtual level or a regular point in the essential spectrum of H^(p), p e Us(p0).

In [1] for a family of the generalized Friedriehs models H^(p), ¡i > 0,p e T2 either the existence or absence of a positive coupling constant threshold /j, = ¡i(p) > 0 depending on the parameters of the model has been proved.

One of the reasons to consider the family of the generalized Friedriehs models interacting via pair local repulsive potentials is as follows: this family generalizes and involves some important behaviors featured by the Schrodinger operators associated with the Hamiltonian of the systems of two arbitrary particles moving on R^r Zd,d ^ 1, as well as with the Hamiltonian for systems of both bosons and fermions [1], [2], [3], [4],

Moreover, as it was stated in [5], [6], physics stable composite objects are usually formed by attractive forces, which allow the constituents to lower their energy by binding together. The repulsive forces separates particles in free space. However, in structured environment such as a periodic potential and in the absence of dissipation, stable composite objects can exist even for repulsive interactions.

The family of the generalized Friedriehs models theoretically adequately describes this phenomenon relating to repulsive forces since the two-particle discrete Schrodinger operators with rank one interactions are a special case of this family.

The generalized Friedriehs model, i.e., the case, where the non-perturbed operator H0 is a multiplication operator by arbitrary function with Van Hove singularities (critical points) defined on the closed interval [a, b] was considered in [3], In this case, unlike to usual Friedriehs model, the multiplicity of continuous spectrum of the non-perturbed operator is not constant. The generalized Friedriehs models appear mostly in the problems of solid state physics [8], [9], quantum mechanics [10], and quantum field theory [11], [12] and in general settings have been studied in [2], [3], [7],

In [13], the family of generalized Friedriehs models with rank one perturbations H^(p), ¡i > 0, p e (-p,p]3, associated with a system of two particles on the three-dimensional lattice Z3 was considered. In a special case of multiplication operator and under the assumption that the operator H^(0), 0 e T3 has a coupling constant threshold fi0(0) > 0, the existence of a unique eigenvalue below the bottom of the essential spectrum of H^0(0)(p), p e (-p,p]3 for all nontrivial values of p e T3 was proved.

In [14], an expansion for an eigenvalue E(fi,p) of H^(p), ¡i > 0 P e (-p,p] was found in some neighborhood of the point /j, = ¡i(p) ^ 0. In [4], for a special family of the generalized Friedriehs models, the existence of eigenvalues was proved for some values of quasi-momentum p e Td in a neighborhood of p0 e Td,

In celebrated work [15], B.Simon and M.Klaus considered a family of Schrodinger operators H = —A + ¡iV in a situation, where as ^tended to fi0, some eigenvalue e^) tended to 0, i.e., this eigenvalue was absorbed by the essential spectrum, and vice versa, as /j, tended to from the right /i0, a new eigenvalue emerged from the essential spectrum. In [15], this phenomenon was called coupling constant threshold.

In [16] the Hamiltonian of a system of two identical quantum mechanical particles (bosons) moving on the d-dimensional lattice Zd,d ^ 3 and interacting via a pair zero-range repulsive pair potentials was considered. For the associated two-particle Schrodinger operator H^ (K), K e Td = (—n, n]d, the existence of coupling constant threshold ^ = ^0(K) > 0 was proven: the operator had no eigenvalue for all 0 < ^ < but for each ^ > it possessed a unique eigenvalue z(fi,K) above the upper edge of the essential spectrum of H^(K). An asvmptoties for z(n, K) was found as ^ ^ ^0(K) and K ^ 0.

In [17], for a wide class of two-bodv energy operators H2(k) on the d-dimensional lattice Zd, d > 3 k being the two-particle quasi-momentum, it was proved that for all nontrivial values

k = 0, the discrete speetrum of H2(k) below its threshold is non-empty provided the following two assumptions (i) and (ii) are satisfied:

(i) the operator #2(0) has either an eigenvalue or a virtual level at the bottom of its essential spectrum

(ii) the one-particle free Hamiltonian in the coordinate representation generates positivitv preserving semi-group.

In [15] the existence of a coupling constant threshold was assumed, while time in [16] the coupling constant threshold was determined by the given data of the Hamiltonian,

We note that for the Hamiltonian of a system of two identical particles moving on R2 or Z2 the coupling constant threshold vanishes if the particles are bosons and the coupling constant threshold is positive if particles are fermions,

2. Preliminaries and main results

Let Z3 be the three-dimensional hypercubes lattice and T3 = (—be the three-dimensional torus (Brillouin zone), the dual group of Z3. The operators of addition and multiplication by number of the elements of torus T3 = (—C R3 was defined as operations in R3 modulo (2^Z3).

Let L2(T3) be the Hilbert space of square-integrable functions defined on the torus T3 and C1 be the one-dimensional complex Hilbert space.

We consider a family of the generalized Friedrichs models acting in L2(T3) as follows:

#» = H0(p)+ /!$*$, /!> 0.

Here

$: L2(T3) ^ C1, $f = (/,^)L2(T3),

$* : C1 ^ L2(T3), $*/0 = V(q)f0,

where (■, -)l2(T3) is the scalar product in L2(T3) and H0(p), p £ T3 is a multiplication operator by a function Wp(-) := w(p, ■), that is,

(H0(p)f)(q) = wp(q)f (q), f £ L2(T3). (2.1)

We observe that for each f £ L2(T3) and g0 £ C1 the identity

($f,90)C1 = (f, $*90)L2(T3)

holds.

In the paper, we make the following assumption. Assumption 1. The following conditions are satisfied:

(i) the function <^(-) is nontrivial and real-analytic and has no singularities on the torus T3.

(ii) the function w(^, ■) is real-analytic function on (T3)2 = T3 x T3 and has a unique non-degenerated maximum at (p0,q0) £ (T3)2.

Remark 1. We identify the real-analytic functions on T3 with the real-analytic functions on R3 being 2n-periodic in each variable.

The perturbation v = $*$ is positive operator of rank one. Hence, by the well-known Weyl theorem [18], the essential spectrum fills the following segment on the real axis:

(Jess(H^(p)) = aess(H0(p)) = [m(p), M(p)],

where

m(p) = min wp(q), M (p) = max wp(q).

By Assumption 1, there exist a ^-neighborhood Us(po) C T3 of the point p = p0 E T3 and an analytic vector function q0 : U¿(p0) ^ T3 such that for each p E U¿(p0), the point q0(p) = (^"(p), q0)2(p), qO^"1 (p)) E T3 is a unique non-degenerated maximum of the function Wp(-), see Lemma 3.1. Moreover, the following integral

1 = f V2(s)ds > 0

¡(p) j M(p) - wp(s)

T3

is well-defined, see Lemma 3.4.

The positive number ¡(p) > 0 is called coupling constant threshold.

Definition 2.1. The threshold z = M(p) is called a regular point of the essential spectrum of the operator H^(p) if the equation H^(p)f = M(p)f has only trivial solution f = 0 in L2(T3).

Let L1(T3) be the Banach space of integrable functions on T3.

Definition 2.2. The threshold z = M(p) is called a M(p) energy resonance (virtual level) in the essential spectrum of the operator H^(p) if the equation H^(p)f = M(p)f has a non-trivial solution f E L1(T3) \ L2(T3). The solution f is called virtual state of the operator H^(p).

Remark 2. The set G of ¡ > 0, for which the threshold is a regular point of the essential spectrum aess(H^(p)) of H^(p), is an open set in (0, More precisely, G = (0, +<x>)\{¡(p)}.

Remark 3. If the threshold z = M(p) is a regular point of H^(p), then the number of eigenvalues of the operator H^(p) above the threshold M(p) does not change under small perturbations of ¡ E G, see Statements (i), (ii) and (iii) of Theorem 2.1.

Next theorem provides a necessary and sufficient conditions for existence of a unique eigenvalue E(n,p) above the threshold of the essential spectrum of H^(p), p E Us(p0). We prove that for a fixed p E Us(p0) the function E(■,p) is analytic in (¡(p), Moreover, for the

associated eigenfunction we find an explicit expression and prove its analyticity. Furthermore, in the case ¡ = ¡(p) > 0, we prove that the threshold M(p) of the essential spectrum is either a virtual level or eigenvalue for the operator H^(p), p E T3.

Theorem 2.1. Let Assumption 1 hold and p E Us(p0). Then the following statements are true:

(i) The operator H^(p) has a unique eigenvalue E(¡,p) above the threshold M(p) of the essential spectrum if and only if ¡ > ¡(p). The function E(■,p) is a monotonically increasing real-analytic function on the interval (¡(p), and the function E(¡, ■) is real-analytic

in Us(p0). The associated eigenfunction

tf(¡; p,q,E (¡, p)) = C¡v(g)

E(¡p) -wP(q)

is analytic on T3, where C = 0 is a normalization constant. Moreover, the mappings tf : Us(p0) ^ L2(T3), p ^ tf(¡¡;p,q,E(¡,p)) E L2(T3)

and

tf : (¡(p), ^ L2(T3), ¡ ^ tf(¡¡;p,q,E(¡,p)) E L2(T3)

are vector-valued analytic functions in Us(p0) and (¡(p), respectively.

(ii) The operator H^(p) has no eigenvalues in a semi-infinite interval (M(p), to) if and only if 0 < ¡ < ¡(p).

(iii) The threshold z = M(p) is a regular point of the operator H^(p) if and only if ¡ = ¡(p).

(iv) The threshold z = M(p) is a virtual level of the operator H^(p) if and only if i = i(p) and f(q0(p)) = 0. The associated virtual state is of the form

f( ) = C^(p)y(g) 1 (Q) M(p) -Wp(q)'

where C = 0 is a normalizing constant and f E L1(T3) \ L2(T3).

(v) The threshold z = M(p) is an eigenvalue of the operator H^(p) if and only if i = i(p) and f(q0(p)) = 0. Moreover, if the threshold z = M(p) is an eigenvalue of the operator H^(p), then the associated eigenfunction reads as

M = .C^l E^2(T3), (2.2)

J(y) M(p) -wp(q) ( ^ ()

where C = 0 is a normalizing constant.

Remark 4. It follows from the positivity of $*$ that the operator H^(p) has no eigenvalues below m(p).

3. Proof

We begin with a series of auxiliary lemmata, which will be employed in the proof of the main result.

Lemma 3.1. Let Assumption 1 hold. Then there exist a 5-neighborhood Us(p0) C T3 of the point p = p0 and an analytic function q0 : Us(p0) ^ T3 such that for each p E Us(p0), the point q0(p) is a unique non-degenerated maximum of the function wp(^).

Proof. By Assumption 1, the square matrix

.4(0)= (^(<fc)Y < 0

Qid qj Jij=i

is negatively defined and Vwp0(q0) = 0. Then by the implicit function theorem for the analytic case there exist a ^-neighborhood Us(p0) C T3 of p = p0 E T3 and a unique analytic vector function q0(•) : Us(p0) ^ T3 such that Vwp(q0(p)) = 0 and

a(p) = ((q0(p)0 < 0, pE u(p0).

Hence, for each p E Us(p0), the point q0(p) is a unique non degenerated maximum of the function wp(•). □

For each | > 0 and p E T3 we define in C \ [m(p); M(p)] an analytic function A(|,p; •) (the Fredholm determinant A(|,p; •) associated with the operator H^(p)):

A(|,p; 0 = 1 -^(p; •), (3.1)

where

^(p; z)= i ^2(s)d{8. , PE T3, ze C \ [m(p); M (p)]. (3.2)

J z-wp(s)

T3

Lemma 3.2. A number z E C \ aess(H^(p)),p E T3 is an eigenvalue of the operator H^(p) if and only if A(i, p; z) = 0. The associated eigenfunction f E L2(T3) reads as

C№(q) . .

f(q) =-rr, (3.3)

z - wp(q)

where C = 0 is a normalizing constant.

U0= I = o + £(<), n = 0,1,2,■■■

Proof. If a number z E C \ aess(H^(p)),p E T3 is an eigenvalue of the operator H^(p) and f E L2(T3) is an associated eigenfunction, i.e., the equation

[wp(q) - z]f(q) - Mq)J <fi(t)f(t)dt = 0, (3.4)

T3

with

J f(t)f(t)dt = 0

T3

has solution, then the solution f of equation (3.4) is given by

CPf(q)

f(Q) =-rr, (3.5)

z - wp(q)

where C = 0 is a normalizing constant. The representation (3.5) of the solution of equation

(3.4) implies the identity A(p,p; z) = 0.

Let A(p,p; z) = 0 for some z E C \ aess(H^(p)), p E T3. Then the function f defined by

(3.5) belong to L2(T3) and solves the equation

H,(p)f = z f.

The analyticity of the eigenfunction /(■) defined by (3.5) is implied by the analyticity of f (■) and Wp(-) as well as by to the fact that the denominator z — wp(^) in (3.5) is non-zero. □

Lemma 3.3. For ( < 0 the following identities hold:

s

r2ndr o (r

^—c = 2 0

where In(() is an analytic function in a neighborhood of the origin. The proof of the above lemma can be found in [20, Lm. 5]. Lemma 3.4. Let Assumption 1 hold. Then for each p E Us(p0) the integral

fi(p) = fi(p ,M (p))= f f)(s)ds )

J M(p) - Wp(s)

T3

is well-defined and is an analytic function in Us(p0).

Proof. We note that by the parametrical Morse lemma [21, Lm. 3.3113], for each p E Us(p0), there exists a map s = —>(y, p) of the sphere W-y (0) C R3 centered at y = 0 of radius ff> 0 into a neighborhood U(q0(p)) of the point q0(p) such that in U(q0(p)), the function wp(—(y,p)) can be represented as

wP(—(y,p)) = M(p) - y2 - y\ - y2 = M(p) - y2. Here the function —>(y, ■) (respectively, — (■,p)) is analytic in Us(p0) (respectively, W-y(0)) and -0(0,p) = q0(p). Moreover, the Jacobian J(—(y,p)) of the mapping s = —>(y,p) is analytic in W-y(0) and positive, i.e., J(—(y,p)) > 0 for all y E W1 (0) and p E Us(p0). We represent

n.(p, *) = i = i + /

J z- wp(s) J z- wp(s) J z- wp(s) (3 6)

T3 U (qo (p)) T3W(qo(p)) (3.6)

= ^l(p, z) + ^2('P, z). Assumption 1 yields that the function Q2(p, M(p)) is analytic in p E Us(p0).

We change the variables s = ^(y,p) in the integral for Q1(p, z) and this gives

n.(P, *) = f f^M ) JM,P))"y-

J y2 + z — M (p)

W7 (0)

where J(ip(y,p)) is the Jacobian of the mapping ^>(y,p). Passing to spherical coordinates as y = ru, we obtain

, z) = f f2 + z — M(p) {j u,P))J(^(ru,P))du}dr, (3.7)

0 Us

where is a unit sphere in R3 and du is its area differential. The inner integral can be represented as

oo

/ V2(^(r //, p))J (iP(r », p))dv = Y, Tn(p) r2n, (3.8)

fia n=0

where the Pizetti coefficients rn(p), n = 0,1, 2,... are analytic in Us (p 0 ) [19]. Identities (3.7) and (3.8) yield that the limit

7

^ = Qi(p,z) = ^ r2 + „ _ m(n) = £ ônxr ^

z^M(p)+0 z^M(p)+0 ' J r2 + z — M(p) ^ 2n +1

n=0 0 v ' n=0

exists and the function Q(p) = Q1(p) + H2(p, M(p) is analytic in p E Us(p0). □

Lemma 3.5. Let Assumption 1 hold and p E Us(p0). Then the following statements are equivalent:

(i) the threshold M(p) is a resonance of the operator H^(p) and the associated resonance state is of the form

/fa) = MrT^TT, (3-9)

M (P) — ™p(q) where C = 0 is a normalizing constant.

(ii) p(q0(p)) = 0 and A(j,p ;M(p)) = 0.

(iii) <P(q0(p)) = 0 and j = j(p).

Proof. Let the threshold M(p) be a resonance of the operator HM(p). According to the definition of resonance, the equation

H,(p)f = M (p)f has a nontrivial solution f E L1(T3) \ L2(T3), i.e., the equation

[M (p) — wp(q)]f(q) — Mq)J <p(t)f(t)dt = 0 (3.10)

T3

with

j <p(t)f(t)dt = 0

T3

has a nontrivial solution. It is easy to check that the solution f of equation (3.10), i.e., the virtual state, is given by (3.9).

Expanding the function p(ip(ru,p)) in (3.7) to the Taylor series at r = 0, we obtain

!/,p)) =^(qc(p)) + ^ (qc(p)) ^ --y-(0,p) isjJ r ^^

+ g(r, u)r2, yj = rUj,

where g(■, v) is continuous in W-y(0) and uf + i/| + ff = 1. Since the solution f of the equation (3.10) belongs to L*(T3) \ L2(T3), asymptotics (3.11) yields the relation <p(q0(p)) = 0. Substituting expression (3.9) for f into equation (3.10), we obtain:

<P(Q) -MQ) i M ff(t)dt (f) =0, (3.12)

J M(p) - dp(t)

T3

which implies the identities A(p,p; M(p)) = 0 and p = p(p).

Let f(q0(p)) = 0 and p = p(p). Then it easy to confirm that A(p,p; M (p)) = 0 and the function f defined by (3.9) belongs to L(T3) \ L2(T3) and solves the equation

H,(p)f = M (p) f.

□

Lemma 3.6. Let Assumption 1 hold and p E Us(p0). Then the following statements are equivalent:

(i) The threshold z = M(p) is an eigenvalue of the operator H^(p) and the associated eigenvector is of the form

m = M (p) • <3-13»

where C = 0 is a normalizing constant.

(ii) <p(qo(p)) = 0 and A(n,p ;M(p)) = 0.

(iii) f(q0(p)) = 0 and p = p(p).

Proof. Let z = M(p) be an eigenvalue of the operator H^(p) and f E L2(T3) is an associated eigenfunction, i.e., the equation

[M (p) - dp(q)]f(q) - Mq) j <p(t)f(t)dt = 0 (3.14)

T3

with

J <p(t)f(t)dt = 0

T3

has a nontrivial solution. Then the associated eigenfunction f is given by (3.13). In this case the relation f E L2(T3) and asymptotics (3.11) yield the the identity f(q0(p)) = 0. Equation (3.14) implies the identity A(p,p; M(p)) = 0, which implies p = p(p).

Let f(q0(p)) = 0 and p = p(p). Then A(p,p ;M (p)) = 0 and the function f defined by (3.13) solves the equation

H,(p)f = M (p) f.

□

Corollary 1. The equation H^(p)f = M(p)f has only trivial solution f = 0 in L2(T3) if and only if p = p(p).

In the next lemma we find an expansion for A(/i,p; z) in a half-neighborhood ( M(p), M(p)+$) of the point z = M (p).

Lemma 3.7. Let Assumption 1 hold. Then for each j > 0, p E Us(p0) and sufficiently small z — M(p) > 0 the function A(j,p; ■) can be represented as the following convergent series:

A(j,p; z) = 1 — jfi(p) + ¡^^(z — M(p))1/2 — j £ cn(p)(z — M(p))n/2, (3.15)

n=2

T0(p) = ^2(q0(p))J (q0(P)). Proof. According to (3.7), (3.8) and Lemma 3.3, the function Q1(p;z) can be represented as

fii(p, z) = — — M(p))1/2 + £ Cn(p)(z — M(p))n+1/2 + F(p, z), (3.16)

n=1

where F(p, z) is an analytic function at the point z = M(p) and

. (p) = .

Therefore, decomposition (3.6) yields the following representation for Q(p, z),z E [ M (p), M (p) + 5) :

fi(p, z) = — — M(p))1/2 + ^ c,n(p)(z — M(p))n+1 + F(p, z),

n=1

where F(p, z) = F(p, z) + H2(p, z) is a function analytic at the point z = M(p). Since

F(p, M(p)) = Q(p) and (z — M(p))1/2 > 0 for z > M(p),

we obtain

fi(p, z) = fi(p) — ^^(z — M(p))1/2 + £ cn(p)(z — M(p))n/2.

n=2

Identity (3.1) completes the proof. □

Now we are in position to prove our main result. Proof of Theorem 2.1. We begin with proving (i). Let j > j(p). Then Lemma 3.7 implies that

lim A(j,p; z) = A(j,p; M(p)) = 1 — < 0.

z^M(p)+0 j(p)

The function A(j,p; ■) is continuous and monotonically increasing in zE ( M (p), and

lim A(j,p; z) = 1. (3.17)

Hence, A(j,p; z) = 0 for a unique z E ( M(p),

Let A(j,p; z) = 0 for some z E ( M(p), +ro). Then

1 — = A(j,p ;M(p)) < A(j,p; z) = 0 (3.18)

J(P)

which yields that j > j( ). Applying Lemma 3.6, we arrive at the desired statement.

Since z = E(j,p) is a solution of the equation A(j,p; z) = 0 and A(j, ■; z) (resp. A(-,p; z)) is real-analytic in Us(p0) (resp. (j(p), +ro)), the implicit function theorem implies that E(j, ■) (respectively, E(■,p)) is real analytic in Us(p0) (respectively, (j(p), +ro)).

Note that for each p E Us(p0) the determinant A(-,p; z) is monotonically decreasing function in (j(p), and hence, the solution (eigenvalue) E(j,p) is also monotonically decreasing function in (j(p), +ro).

Lemma 3.2 implies that if a number E(j,p) is an eigenvalue of H^(p), p E Us(p0), then the function

p, ■,E(j,p)) = CjjP(') , E (j, P) — Wp(0

where C = 0 is a normalization constant, is a solution of the equation

H^(p)^(j; pa,e (j, p)) = E (j, p)^(j; pa,e (j, p)).

The analyticity of ^(j; p, ■, E(j,p)) follows the analyticity of <^(-) and (wp(^ — E(j,p))-1 in T3.

Since the functions E(j, ■) (respectively, E(■,p)) and w(^, q) are analytic in Us(p0) (respectively, (j(p), +ro)) and wp(q) — E(j,p) > 0 the mappings m- ^(j;P,q,E(j,p)) (respectively, j M- ^(j;p,q,E(j,p))) is also analytic mapping in Us(p0) (respectively, (j(p), +ro)).

The rest of statements of Theorem 2.1 can be proven by applying Lemmata 3.5 and 3.6 in the same way as in the above proof of (i). □

4. Acknowledgments Authors thank the referees for a number of constructive comments and useful suggestions.

REFERENCES

1. S.N. Lakaev, A. Ibrahim, Sh.H. Kurbanov. Threshold effects for the generalized Friedrichs model with the perturbation of rank one // Abstr. Appl. Anal. 2012, 180953 (2012).

2. S.N. Lakaev. The stucture of resonances of the Generalized Friedrichs model // Funkts. Anal. Pril. 17:4, 88-89(1983). [FUnct. Anal. Appl. 17:4, 317-319 (1983).]

3. S.N. Lakaev. Some spextra! properties of the Generalized Friedrichs model // Trudy Sem. Petrovsk. 11, 210-238 (1986). [J.Soviet Math. 45:6, 1540-1565 (1989).]

4. E.L. Lakshtanov, R.A. Minlos. The spectrum of two-particle bound states of transfer matrices of Gibbs fields (an isolated bound state) // Funkts. Anal. Prilozhen. 38:3, 52-69(2004). [Funct. Anal. Appl. 38:3, 202-216 (2004).]

5. J. Hecker Denschlag, A.J. Daley. Exotic atom pairs: Repulsively bound states in an optical lattice //in "Proceedings of the International School of Physics "Enrico Fermi"". 164. 677-696 (2007).

6. K. Winkler, G. Thalhammer, F. Lang, R. Grimm, J. Hecker Denschlag, A. J. Daley, A. Kantian, H. P. Bchler, P. Zoller. Repulsively bound atom pairs in an optical lattice. // Nature. 441, 853-856 (2006).

7. Zh.I. Abdullaev, I.A. Ikromov, S.N. Lakaev. Embedded eigenvalues and resonances of a generalized Friedrichs model // Teor. Matem. Fiz. 103:1, 54-62 (1995). [Theor. Math. Phys. 103:1, 390-397 (1995).]

8. A. Mogilner. Hamiltonians in solid state physics as multi-particle discrete Schrodinger operators: Problems and results // Adv. Soviet Math. 5, 139-194 (1991).

9. M. Reed, B. Simon. Methods of modern mathematical physics. III: Scattering theory. Academic Press, New York (1979).

10. K.O. Friedrichs. On the perturbation of continuous spectra // Comm. Appl. Math. 1:4, 361-406 (1948).

11. K.O. Friedrichs. Perturbation of spectra in Hilbert space, Amer. Math. Soc., Providence, RI (2008).

12. V.A. Malishev, R.A. Minlos. Linear infinite-particle operators. Transl. Math. Monogr. 143. Amer. Math. Soc., Providence, RI (1995).

13. S. Albeverio, S.N. Lakaev, Z.I. Muminov. The threshold effects for a family of Generalized Friedrichs models under rank one perturbations //J. Math. Anal. Appl. 330:2, 1152-1168 (2007).

14. S.N. Lakaev, M. Darus, Sh.H. Kurbanov. Puiseux series expansion for an eigenvalue of the generalized Friedrichs model with perturbation of rank 1 //J. Phys. A: Math. Theor. 46:20, 205304 (2013).

15. M. Klaus, B. Simon. Coupling constant thresholds in nonrelativistic quantum mechanics. I. Short-range two-body case // Ann. Phys. 130:2, 251-281 (1980).

16. S.N. Lakaev, Sh.Yu. Holmatov. Asymptotics of Eigenvalues of a two-particle Schrodinger operators on lattices with zero range interaction //J. Phys. A: Math. Theor. 44:13, 135304 (2011).

17. S. Albeverio, S.N. Lakaev, K.A. Makarov, Z.I. Muminov. The threshold effects for the two-particle Hamiltonians on lattices // Comm. Math. Phys. 262:1, 91-115 (2006).

18. M. Reed, B. Simon. Methods of modern mathematical physics. IV: Analysis of operators, Academic Press, New York (1978).

19. R. Courant, D. Hilbert. Methods of mathematical physics. V. 2. Partial differential equations, John Wiley & Sons, New York (1966).

20. S.N. Lakaev. Bound states and resonances of N -particle discrete Schrodinger operator // Theor. Matem. Fiz. 91:1, 51-65(1992). [Theor. Math. Phys. 91:1, 362-372 (1992).]

21. M.V. Fedoryuk. Asymptotics of integrals and series, Nauka, Moscow (1987). (in Russian).

Saidakhmat Norjigitovich Lakaev, Samarkand State University, University Boulvard 15, 140104, Samarkand, Uzbekistan E-mail: [email protected]

Maslina Darus,

University Kebangsaan Malaysia, 43600, Selangor, Malaysia E-mail: [email protected]

Said T. Dustov,

Navoi State Pedagogical Institute, Janubiy 1-A, Navoi, 210102, Navoi, Uzbekistan E-mail: [email protected]