Abstract

The paper deals with the Dirac operator generated on the finite interval [0, π] by the differential expression −By′ + Q(x)y, where $$B = \left( {\begin{array}{*{20}c} 0 { - 1} \end{array} \begin{array}{*{20}c} 1 0 \end{array} } \right), Q(x) = \left( {\begin{array}{*{20}c} {q_1 (x)} {q_3 (x)} \end{array} \begin{array}{*{20}c} {q_2 (x)} {q_4 (x)} \end{array} } \right),$$ and the entries qj(x) belong to Lp[0, π] for some p ≥ 1. The classes of regular and strongly regular operators of this form are defined, depending on the boundary conditions. The asymptotic formulas for the eigenvalues and eigenfunctions of such operators are obtained with remainders depending on p. It it is proved that the system of eigen and associated functions of a regular operator forms a Riesz basis with parentheses in the space (L2[0, π])2 and the usual Riesz basis, provided that the operator is strongly regular.

Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call