Criterion of Bari basis property for 2×22 \times 2 Dirac-type operators with strictly regular boundary conditions

preprint2022arXivOpen access

Abstract

The paper is concerned with the Bari basis property of a boundary value problem associated in L2([0,1];C2)L^2([0,1]; \mathbb{C}^2) with the following 2×22 \times 2 Dirac-type equation for y=col(y1,y2)y = {\rm col}(y_1, y_2): LU(Q)y=−iB−1y′+Q(x)y=λy,B=(b100b2),b1<0<b2,L_U(Q) y =-i B^{-1} y' + Q(x) y = λy , \quad B = \begin{pmatrix} b_1 & 0 \\ 0 & b_2 \end{pmatrix}, \quad b_1 < 0 < b_2, with a potential matrix Q∈L2([0,1];C2×2)Q \in L^2([0,1]; \mathbb{C}^{2 \times 2}) and subject to the strictly regular boundary conditions Uy:={U1,U2}y=0Uy :=\{U_1, U_2\}y=0. If b2=−b1=1b_2 = -b_1 =1 this equation is equivalent to one dimensional Dirac equation. We show that the system of root vectors {fn}n∈Z\{f_n\}_{n \in \mathbb{Z}} of the operator LU(Q)L_U(Q) forms a Bari basis in L2([0,1];C2)L^2([0,1]; \mathbb{C}^2) if and only if the unperturbed operator LU(0)L_U(0) is self-adjoint. We also give explicit conditions for this in terms of coefficients in the boundary conditions. The Bari basis criterion is a consequence of our more general result: Let Q∈Lp([0,1];C2×2)Q \in L^p([0,1]; \mathbb{C}^{2 \times 2}), p∈[1,2]p \in [1,2], boundary conditions be strictly regular, and let {gn}n∈Z\{g_n\}_{n \in \mathbb{Z}} be the sequence biorthogonal to the system of root vectors {fn}n∈Z\{f_n\}_{n \in \mathbb{Z}} of the operator LU(Q)L_U(Q). Then {∥fn−gn∥2}n∈Z∈(ℓp(Z))∗⇔LU(0)=LU(0)∗. \{\|f_n - g_n\|_2\}_{n \in \mathbb{Z}} \in (\ell^p(\mathbb{Z}))^* \quad\Leftrightarrow\quad L_U(0) = L_U(0)^*. These abstract results are applied to non-canonical initial-boundary value problem for a damped string equation.

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