“…Recently, i.e., in the 2000s, many authors [36,[44][45][46]40,47,50,67,26,49,51] focused on the problem of convergence of eigenfunction (or more generally root function) decompositions in the case of regular but not strictly regular bc.…”
We study the system of root functions (SRF) of Hill operator Ly = −y + vy with a singular (complexvalued) potential v ∈ H −1 per and the SRF of 1D Dirac operator Ly = i 1 0Q 0 , subject to periodic or anti-periodic boundary conditions. Series of necessary and sufficient conditions (in terms of Fourier coefficients of the potentials and related spectral gaps and deviations) for SRF to contain a Riesz basis are proven. Equiconvergence theorems are used to explain basis property of SRF in L p -spaces and other rearrangement invariant function spaces.
“…Recently, i.e., in the 2000s, many authors [36,[44][45][46]40,47,50,67,26,49,51] focused on the problem of convergence of eigenfunction (or more generally root function) decompositions in the case of regular but not strictly regular bc.…”
We study the system of root functions (SRF) of Hill operator Ly = −y + vy with a singular (complexvalued) potential v ∈ H −1 per and the SRF of 1D Dirac operator Ly = i 1 0Q 0 , subject to periodic or anti-periodic boundary conditions. Series of necessary and sufficient conditions (in terms of Fourier coefficients of the potentials and related spectral gaps and deviations) for SRF to contain a Riesz basis are proven. Equiconvergence theorems are used to explain basis property of SRF in L p -spaces and other rearrangement invariant function spaces.
“…Hence the system of the root functions of T 1 1 (q) does not form a Riesz basis (see [20]). Note that (b) follows also from (a) and Theorem 2 of [12,13].…”
Section: Lemmamentioning
confidence: 86%
“…Case (c) The cases β 2 , β 4 = 0 and β 1 , β 3 = (−1) σ are investigated in [12,13] and [19]. We call the boundary conditions (7) and (9) for β 2 , β 4 = 0 and β 1 , β 3 = (−1) σ which are different from the special cases (a) , (b) and (c) as general regular boundary conditions that are not strongly regular.…”
Section: Introduction and Preliminary Factsmentioning
confidence: 99%
“…Theorem 5 (a) If (12) holds, then the large eigenvalues of T 1 2 (q) are simple and the square roots (with nonnegative real part) of these eigenvalues consist of two sequences {ρ n,1 } and {ρ n,2 } satisfying…”
We obtain the asymptotic formulas for the eigenvalues and eigenfunctions of the Sturm-Liouville operators with general regular boundary conditions. Using these formulas, we find sufficient conditions on the potential q such that the root functions of these operators do not form a Riesz basis.
“…It is proved in that the system of root functions of the differential operator forms an unconditional basis of the space L 2 (0,1), where q ( x ) ∈ L 1 (0,1) is an arbitrary complex‐valued function, γ is an arbitrary nonzero complex constant and σ = 0,1. Under the condition γ = 0 (periodic and antiperiodic boundary conditions) in and , necessary and sufficient conditions of unconditional basicity in L 2 (0,1) of the system of root functions of the earlier differential operator were obtained in terms of the Fourier coefficients of the potential q (x) (see also ).…”
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