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We offer a detailed treatment of spectral and Weyl–Titchmarsh–Kodaira theory for all self-adjoint Jacobi operator realizations of the differential expression $$\begin{aligned} \tau _{\alpha ,\beta } =&- (1-x)^{-\alpha } (1+x)^{-\beta }(d/dx) \big ((1-x)^{\alpha +1}(1+x)^{\beta +1}\big ) (d/dx), \\&\alpha , \beta \in {\mathbb {R}}, \, x \in (-1,1), \end{aligned}$$ τ α , β = - ( 1 - x ) - α ( 1 + x ) - β ( d / d x ) ( ( 1 - x ) α + 1 ( 1 + x ) β + 1 ) ( d / d x ) , α , β ∈ R , x ∈ ( - 1 , 1 ) , in $$L^2\big ((-1,1); (1-x)^{\alpha } (1+x)^{\beta } dx\big )$$ L 2 ( ( - 1 , 1 ) ; ( 1 - x ) α ( 1 + x ) β d x ) , $$\alpha , \beta \in {\mathbb {R}}$$ α , β ∈ R . In addition to discussing the separated boundary conditions that lead to Jacobi orthogonal polynomials as eigenfunctions in detail, we exhaustively treat the case of coupled boundary conditions and illustrate the latter with the help of the general $$\eta $$ η -periodic and Krein–von Neumann extensions. In particular, we treat all underlying Weyl–Titchmarsh–Kodaira and Green’s function induced m-functions and revisit their Nevanlinna–Herglotz property. We also consider connections to other differential operators associated with orthogonal polynomials such as Laguerre, Gegenbauer, and Chebyshev.
We offer a detailed treatment of spectral and Weyl–Titchmarsh–Kodaira theory for all self-adjoint Jacobi operator realizations of the differential expression $$\begin{aligned} \tau _{\alpha ,\beta } =&- (1-x)^{-\alpha } (1+x)^{-\beta }(d/dx) \big ((1-x)^{\alpha +1}(1+x)^{\beta +1}\big ) (d/dx), \\&\alpha , \beta \in {\mathbb {R}}, \, x \in (-1,1), \end{aligned}$$ τ α , β = - ( 1 - x ) - α ( 1 + x ) - β ( d / d x ) ( ( 1 - x ) α + 1 ( 1 + x ) β + 1 ) ( d / d x ) , α , β ∈ R , x ∈ ( - 1 , 1 ) , in $$L^2\big ((-1,1); (1-x)^{\alpha } (1+x)^{\beta } dx\big )$$ L 2 ( ( - 1 , 1 ) ; ( 1 - x ) α ( 1 + x ) β d x ) , $$\alpha , \beta \in {\mathbb {R}}$$ α , β ∈ R . In addition to discussing the separated boundary conditions that lead to Jacobi orthogonal polynomials as eigenfunctions in detail, we exhaustively treat the case of coupled boundary conditions and illustrate the latter with the help of the general $$\eta $$ η -periodic and Krein–von Neumann extensions. In particular, we treat all underlying Weyl–Titchmarsh–Kodaira and Green’s function induced m-functions and revisit their Nevanlinna–Herglotz property. We also consider connections to other differential operators associated with orthogonal polynomials such as Laguerre, Gegenbauer, and Chebyshev.
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