Abstract

In this paper, the spectrum and the resolvent of the operator $L_{\lambda}$ which is generated by the differential expression $\ell_{\lambda }(y)=y^{(m)}+\sum_{\gamma=1}^{m} ( \sum_{k=0}^{\gamma }\lambda^{k}p_{\gamma k}(x) ) y^{(m-\gamma)}$ has been investigated in the space $L_{2}(\mathbb{R})$ . Here the coefficients $p_{\gamma k}(x)=\sum_{n=1}^{\infty }p_{\gamma kn}e^{i\alpha_{n}x}$ , $k=0,1,\ldots,\gamma-1$ ; $p_{\gamma\gamma }(x)=p_{\gamma\gamma}$ , $\gamma=1,2,\ldots,m$ , are constants, $p_{mm}\neq0$ and $p_{\gamma k}^{(\nu)}(x)$ , $\nu=0,1,2,\ldots,m-\gamma$ , are Bohr almost-periodic functions whose Fourier series are absolutely convergent. The sequence of Fourier exponents of coefficients (these are positive) has a unique limit point at +∞. It has been shown that if the polynomial $\phi (z)=z^{m}+p_{11}z^{m-1}+p_{22}z^{m-2}+\cdots+p_{m-1,m-1}z+p_{mm}$ has the simple roots $\omega_{1},\omega_{2},\ldots,\omega_{m}$ (or one multiple root $\omega_{0}$ ), then the spectrum of operator $L_{\lambda}$ is pure continuous and consists of lines $\operatorname{Re}(\lambda\omega _{k})=0$ , $k=1,2,\ldots,m$ (or of line $\operatorname{Re}(\lambda\omega_{0})=0$ ). Moreover, a countable set of spectral singularities on the continuous spectrum can exist which coincides with numbers of the form $\lambda=0$ , $\lambda _{sjn}=i\alpha_{n} ( \omega_{j}-\omega_{s} ) ^{-1}$ , $n\in \mathbb{N}$ , $s,j=1,2,\ldots,m$ , $j\neq s$ . If $\phi(z)=(z-\omega_{0})^{m}$ , then the spectral singularity does not exist. The resolvent $L_{\lambda}^{-1}$ is an integral operator in $L_{2}(\mathbb{R})$ with the kernel of Karleman type for any $\lambda\in\rho (L_{\lambda})$ .

Highlights

  • 1 Introduction In this study, we investigate the spectrum and the resolvent of the maximal differential operator Lλ which is generated by the linear differential expression m λ(y) = y(m) + pγ (x, λ)y(m–γ )

  • In order to obtain other solutions which form a fundamental system of solutions of equation ( ) together with f (x, λ), let us use the properties of the linear differential operator L : Cm(R) → C(R), which is defined as

  • 3 The spectrum and resolvent of the operator Lλ Here we investigate the structure of the spectrum of the operator Lλ and the resolvent operator L–λ

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Summary

Introduction

We investigate the spectrum and the resolvent of the maximal differential operator Lλ which is generated by the linear differential expression m λ(y) = y(m) + pγ (x, λ)y(m–γ ). In the space L (R), where λ is a complex parameter, γ pγ (x, λ) = λkpγ k(x), pγ γ (x) = pγ γ , k=. Orujov Boundary Value Problems (2015) 2015:238 with pγ γ , pγ kn ∈ C, pmm = and the condition m γ – ∞. (αn)∞ n= is an increasing sequence of positive numbers with αn → +∞ and the set {αn : n ∈ N} is an additive semigroup

The operator Lλ is defined in the domain
It is clear that
Akm pγ
Then the resolvent set of operator
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