On the Riesz basis property of the eigen- and associated functions of periodic and antiperiodic Sturm-Liouville problems

By A. Shkalikov, O. Veliev. 2008

72 citations recorded by the source corpus.

AbstractThe paper deals with the Sturm-Liouville operator $$ Ly = - y'' + q(x)y, x \in [0,1], $$ generated in the space L2 = L2[0, 1] by periodic or antiperiodic boundary conditions. Several theorems on the Riesz basis property of the root functions of the operator L are proved. One of the main results is the following. Let q belong to the Sobolev spaceW1p [0, 1] for some integer p ≥ 0 and satisfy the conditions q(k)(0) = q(k)(1) = 0 for 0 ≤ k ≤ s − 1, where s ≤ p. Let the functions Q and S be defined by the equalities $$ Q(x) = \int_0^x {q(t)dt, S(x) = Q^2 (x)} $$ and let qn, Qn, and Sn be the Fourier coefficients of q, Q, and S with respect to the trigonometric system $$ \{ e^{2\pi inx} \} _{ - \infty }^\infty $$. Assume that the sequence q2n − S2n + 2Q0Q2n decreases not faster than the powers n−s−2. Then the system of eigenfunctions and associated functions of the operator L generated by periodic boundary conditions forms a Riesz basis in the space L2[0, 1] (provided that the eigenfunctions are normalized) if and only if the condition $$ q_{2n} - s_{2n} + 2Q_0 Q_{2n} \asymp q_{ - 2n} - s_{2n} + 2Q_0 Q_{ - 2n} , n > 1, $$ holds.

Subfields: Applied Mathematics, Mathematical Physics

View Paper: https://www.semanticscholar.org/paper/4421a19659f05c4b38421bc799b7c5a9e3761fc5

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In Applied Mathematics

  1. V. Tkachenko
  2. Fritz Gesztesy
  3. Plamen Djakov
  4. Boris Mityagin
  5. M. Malamud
  6. L. Oridoroga
  7. A. Lunyov
  8. Olaf Post

In Mathematical Physics

  1. Plamen Djakov
  2. Boris Mityagin
  3. V. Tkachenko
  4. Fritz Gesztesy
  5. M. Malamud
  6. A. Lunyov
  7. L. Oridoroga
  8. Olaf Post

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