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Regular Sturm-Liouville problems have an infinite spectrum $\lambda_n \to \infty$, and their eigenfunctions are orthogonal and total. Because they are orthogonal and total, they can form an orthonormal basis (ONB) after normalization.

Conditions: The Sturm-Liouville problem is regular ($X=[a,b]$ and $p(x) \neq 0$ for all $x \in X$).

Regular Sturm-Liouville problems have an infinite spectrum $\lambda_n \to \infty$, and their eigenfunctions are orthogonal and total. Because they are orthogonal and total, they can form an orthonormal basis (ONB) after normalization.

Conditions: The Sturm-Liouville problem is regular ($X=[a,b]$ and $p(x) \neq 0$ for all $x \in X$).

Dirichlet boundary conditions correspond to setting the derivative coefficients to zero ($\alpha_2 = \beta_2 = 0$), leaving conditions on the values of $y$ at the endpoints. Neumann boundary conditions correspond to setting the function coefficients to zero ($\alpha_1 = \beta_1 = 0$), leaving conditions on the derivatives.

Conditions: The general boundary conditions are $\alpha_1 y(a) + \alpha_2 y'(a) = 0$ and $\beta_1 y(b) + \beta_2 y'(b) = 0$.; Dirichlet: $\alpha_2 = \beta_2 = 0$.; Neumann: $\alpha_1 = \beta_1 = 0$.

Dirichlet boundary conditions correspond to setting the derivative coefficients to zero ($\alpha_2 = \beta_2 = 0$), leaving conditions on the values of $y$ at the endpoints. Neumann boundary conditions correspond to setting the function coefficients to zero ($\alpha_1 = \beta_1 = 0$), leaving conditions on the derivatives.

Conditions: The general boundary conditions are $\alpha_1 y(a) + \alpha_2 y'(a) = 0$ and $\beta_1 y(b) + \beta_2 y'(b) = 0$.; Dirichlet: $\alpha_2 = \beta_2 = 0$.; Neumann: $\alpha_1 = \beta_1 = 0$.

A Sturm-Liouville problem is regular exactly when its domain is the finite closed interval $X=[a,b]$ and the coefficient $p$ does not vanish anywhere on $X$ ($p(x) \neq 0$ for all $x \in X$). A problem is singular when either the domain $X$ is infinite/unbounded or the coefficient $p$ vanishes at some point $x_0$ in $X$.

Conditions: Regular: $X=[a,b]$ and $p(x) \neq 0$ for all $x \in X$.; Singular: $X$ is infinite, or $p(x_0)=0$ for some $x_0 \in X$.; For unbounded $X$, boundary conditions are interpreted using limits.

A Sturm-Liouville problem is regular exactly when its domain is the finite closed interval $X=[a,b]$ and the coefficient $p$ does not vanish anywhere on $X$ ($p(x) \neq 0$ for all $x \in X$). A problem is singular when either the domain $X$ is infinite/unbounded or the coefficient $p$ vanishes at some point $x_0$ in $X$.

Conditions: Regular: $X=[a,b]$ and $p(x) \neq 0$ for all $x \in X$.; Singular: $X$ is infinite, or $p(x_0)=0$ for some $x_0 \in X$.; For unbounded $X$, boundary conditions are interpreted using limits.

Sturm-Liouville problems are the general class of boundary value problems that arise when the separation of variables technique is applied to a PDE or an initial-boundary value problem. They are also situated as part of the extension of the spectral theorem to infinite dimensions.

Conditions: The context is solving PDEs or initial-boundary value problems using separation of variables.

Sturm-Liouville problems are the general class of boundary value problems that arise when the separation of variables technique is applied to a PDE or an initial-boundary value problem. They are also situated as part of the extension of the spectral theorem to infinite dimensions.

Conditions: The context is solving PDEs or initial-boundary value problems using separation of variables.