Difference between revisions of "Titchmarsh-Weyl m-function"
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A function arising in an attempt to properly determine which singular boundary-value problems are self-adjoint (cf. also [[Self-adjoint differential equation|Self-adjoint differential equation]]). Begin with a formally symmetric differential expression | A function arising in an attempt to properly determine which singular boundary-value problems are self-adjoint (cf. also [[Self-adjoint differential equation|Self-adjoint differential equation]]). Begin with a formally symmetric differential expression | ||
− | + | $$ | |
+ | L y = \frac{-(p y')' + q y}{w} , | ||
+ | $$ | ||
− | where | + | where $p\ne 0$, $q,w>0$ are measurable coefficients over $[a,b)$, and which is defined on a domain within $L^2(a,b;w)$. The Titchmarsh–Weyl $m$-function is defined as follows: For $\lambda = \mu + i \nu$, $\nu\ne 0$, let $\phi$ and $\psi$ be solutions of $L y = \lambda y$ satisfying |
− | + | $$ | |
+ | \begin{aligned} | ||
+ | \phi(a,\lambda) &= \sin\alpha, & \psi(a,\lambda) &= \cos\alpha, \\ | ||
+ | p\phi'(a,\lambda) &= -\cos\alpha, & p\psi'(a,\lambda) &= \sin\alpha . | ||
+ | \end{aligned} | ||
+ | $$ | ||
<table class="eq" style="width:100%;"> <tr><td valign="top" style="width:94%;text-align:center;"><img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t120/t120120/t12012014.png" /></td> </tr></table> | <table class="eq" style="width:100%;"> <tr><td valign="top" style="width:94%;text-align:center;"><img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/t/t120/t120120/t12012014.png" /></td> </tr></table> |
Revision as of 12:44, 29 October 2012
A function arising in an attempt to properly determine which singular boundary-value problems are self-adjoint (cf. also Self-adjoint differential equation). Begin with a formally symmetric differential expression
$$ L y = \frac{-(p y')' + q y}{w} , $$
where $p\ne 0$, $q,w>0$ are measurable coefficients over $[a,b)$, and which is defined on a domain within $L^2(a,b;w)$. The Titchmarsh–Weyl $m$-function is defined as follows: For $\lambda = \mu + i \nu$, $\nu\ne 0$, let $\phi$ and $\psi$ be solutions of $L y = \lambda y$ satisfying
$$ \begin{aligned} \phi(a,\lambda) &= \sin\alpha, & \psi(a,\lambda) &= \cos\alpha, \\ p\phi'(a,\lambda) &= -\cos\alpha, & p\psi'(a,\lambda) &= \sin\alpha . \end{aligned} $$
Now consider a real boundary condition at , , of the form
and let satisfy it. Then
If , is a meromorphic function in the complex -plane; indeed, it is a bilinear transformation. As varies over real values , varies over the real -axis, and describes a circle in the -plane.
It can be shown that if increases, the circles become nested. Hence there is at least one point inside all. For such a point ,
There exists at least one solution of , which is square-integrable.
If the limit of the circles is a point, then is unique and only is square-integrable. This is the limit-point case. If the limit of the circles is itself a circle, then is not unique and all solutions of are square-integrable. This is the limit-circle case.
Nonetheless, the differential operator
whose domain satisfies
where on the limit circle or limit point, is a self-adjoint differential operator (cf. also Self-adjoint operator; Self-adjoint differential equation) on .
If the circle limit is a point, the second boundary condition (at ) is automatic.
The spectral measure of is given by
The spectral resolution of arbitrary functions in is
where the limit is in the mean-square sense, and
References
[a1] | E.A. Coddington, N. Levinson, "Theory of ordinary differential equations" , McGraw-Hill (1955) |
[a2] | A.M. Krall, " theory for singular Hamiltonian systems with one singular point" SIAM J. Math. Anal. , 20 (1989) pp. 644–700 |
Titchmarsh-Weyl m-function. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Titchmarsh-Weyl_m-function&oldid=28680