Spectral theory of ordinary linear differential operators (Q2734848)

From MaRDI portal





scientific article; zbMATH DE number 1637153
Language Label Description Also known as
English
Spectral theory of ordinary linear differential operators
scientific article; zbMATH DE number 1637153

    Statements

    0 references
    26 August 2001
    0 references
    fourth-order differential equation
    0 references
    selfadjoint realization
    0 references
    \(M\) matrix
    0 references
    defect indices
    0 references
    continuous spectrum
    0 references
    point spectrum
    0 references
    Titchmarsh-Weyl coefficient
    0 references
    Kummer-Liouville transform
    0 references
    Spectral theory of ordinary linear differential operators (English)
    0 references
    The formally selfadjoint differential expression NEWLINE\[NEWLINE\tau y=w^{-1}[(ry'')''-(py')'+qy]NEWLINE\]NEWLINE is considered on \([0,\infty)\), where \(p\), \(q\), \(r\), \(w\) are real-valued, \(r,w>0\), and \(r^{-1},p, q, w\in L_{1,loc}([0,\infty))\). The corresponding minimal operator has the defect indices \((m,m)\) with \(m=2\), \(3\), or \(4\). It is investigated how these defect indices and the spectra of selfadjoint realizations depend on the asymptotic behavior of the coefficients. A crucial role is played by the \(M\)-matrix, the analogon of the Titchmarsh-Weyl coefficient in the present case. According to \textit{H. Behncke} [Proc. Am. Math. Soc. 111, No. 2, 373-384 (1991; Zbl 0726.34072) and Manuscr. Math. 71, No. 2, 163-181 (1991; Zbl 0726.34073)], the coefficient functions can be written as sums of smooth (s), conditionally integrable (c), and integrable (i) functions. Introducing the functions \(\widetilde p=p_s/(rw)^{\frac 12}\), \(\widetilde q=q_s/w\), properties of the spectrum such as location of the continuous spectrum, point spectrum and limit points of the point spectrum are investigated in the following cases: \(\widetilde p\), \(\widetilde q\) bounded; \(\widetilde q\to \infty \); \(\widetilde q\to-\infty \), \(\widetilde p^2=O(\widetilde q)\); \(\widetilde p\to\pm\infty \), \(\widetilde q=o(\widetilde p^2)\). Finally, it is shown that the matrix version of the Kummer-Liouville transform is useful to obtain information on the spectrum.
    0 references

    Identifiers

    0 references
    0 references
    0 references
    0 references