Eigenvalue problem of the form Sturm-Liouville

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Discussion Overview

The discussion revolves around an eigenvalue problem of the Sturm-Liouville form, specifically examining boundary conditions and their implications for the solutions of the differential equation. Participants explore the relationships between solutions, their complex conjugates, and the properties of the associated Wronskian.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant presents an eigenvalue problem and asks for hints on how to show that specific boundary conditions lead to a Sturm-Liouville form.
  • Another participant discusses the relationships between two solutions of the eigenvalue problem and how these relate to the Wronskian, questioning the role of the determinant of the transformation matrix S.
  • There is a clarification about the correct application of the transformation matrix S to the solutions of the eigenvalue problem.
  • Participants discuss whether the complex conjugate of a solution, denoted as v*, is also a solution, leading to a conditional statement regarding the real-valued nature of the coefficients p and q.
  • There is a query about the necessity of using the Wronskian in the context of Sturm-Liouville problems and whether both u and v* must be considered as solutions.
  • One participant expresses confusion about how to incorporate the boundary conditions for v* when assuming v is a solution.

Areas of Agreement / Disagreement

Participants express uncertainty regarding the implications of the boundary conditions and the roles of the solutions and their conjugates. There is no consensus on whether v* must satisfy the boundary conditions or how to properly relate the Wronskian to the Sturm-Liouville framework.

Contextual Notes

Participants reference specific mathematical properties and relationships without resolving the implications of these properties on the solutions or boundary conditions. The discussion includes assumptions about the nature of the coefficients and the conditions under which the conjugate solutions apply.

mathmari
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Hey! :o

I have the following exercise and I need some help..

$"\text{The eigenvalue problem } Ly=(py')'+qy=λy, a \leq x \leq b \text{ is of the form Sturm-Liouville if it satisfies the boundary conditions } p(a)W(u(a),v^*(a))=p(b)W(u(b),v^*(b)). \text{ Show that the boundary conditions of the form: }$
$$ \begin{pmatrix}
y(b)\\
y'(b)
\end{pmatrix}=S\begin{pmatrix}
y(a)\\
y'(a)
\end{pmatrix}, S=\begin{pmatrix}
A & B\\
C & D
\end{pmatrix} $$
$\text{ lead to an eigenvalue problem of the form Sturm-Liouville if } detS=\frac{p(a)}{p(b)}."$

Could you give a hint what to do?
 
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My idea is the following:

Let $u, v$ two solutions of the eigenvalue problem.
These two solutions satisfy the following relation:
$u(b)=Su(a)$ and $u'(b)=Su'(a)$
$v^*(b)=Sv^*(a)$ and $ v^{*'} (b)=S v^{*'} (a)$

So $p(b)W(u(b), v^*(b))=p(b)(u(b)v^{*'}(b)-u'(b)v^*(b))=p(b)(S u(a) Sv^{*'}(a)-Su'(a) Sv^*(a))=p(b)S^2(u(a)v^{*'}(a)-u'(a) v^*(a))=p(b)S^2W(u(a), v^*(a))$.

Is it correct do far?

But how does $detS$ appear?

So that this relation is equal to $p(a)W(u(a), v^*(a))$, shouldn't it be $S^2=\frac{p(a)}{p(b)}$? How can I use the determinant of $S$?
 
mathmari said:
My idea is the following:

Let $u, v$ two solutions of the eigenvalue problem.
These two solutions satisfy the following relation:
$u(b)=Su(a)$ and $u'(b)=Su'(a)$
$v^*(b)=Sv^*(a)$ and $ v^{*'} (b)=S v^{*'} (a)$

So $p(b)W(u(b), v^*(b))=p(b)(u(b)v^{*'}(b)-u'(b)v^*(b))=p(b)(S u(a) Sv^{*'}(a)-Su'(a) Sv^*(a))=p(b)S^2(u(a)v^{*'}(a)-u'(a) v^*(a))=p(b)S^2W(u(a), v^*(a))$.

Is it correct do far?

But how does $detS$ appear?

So that this relation is equal to $p(a)W(u(a), v^*(a))$, shouldn't it be $S^2=\frac{p(a)}{p(b)}$? How can I use the determinant of $S$?
$S = \begin{pmatrix}A&B \\ C&D \end{pmatrix}$ is a matrix, so it makes no sense to talk about $Su(a)$ or $S{v^*}'(a)$. In fact, $\begin{pmatrix}u(b) \\u'(b) \end{pmatrix} = S\begin{pmatrix}u(a) \\u'(a) \end{pmatrix} = \begin{pmatrix}A&B \\ C&D \end{pmatrix}\begin{pmatrix}u(a) \\u'(a) \end{pmatrix} = \begin{pmatrix}Au(a) + Bu'(a) \\Cu(a) + Du'(a) \end{pmatrix}.$ Therefore $u(b) = Au(a) + Bu'(a)$, $u'(b) = Cu(a) + Du'(a)$, and similarly for the other solution $v$. Substitute those values into the given boundary condition, and you should end up with an equation involving $\det S = AD-BC.$
 
Opalg said:
$S = \begin{pmatrix}A&B \\ C&D \end{pmatrix}$ is a matrix, so it makes no sense to talk about $Su(a)$ or $S{v^*}'(a)$. In fact, $\begin{pmatrix}u(b) \\u'(b) \end{pmatrix} = S\begin{pmatrix}u(a) \\u'(a) \end{pmatrix} = \begin{pmatrix}A&B \\ C&D \end{pmatrix}\begin{pmatrix}u(a) \\u'(a) \end{pmatrix} = \begin{pmatrix}Au(a) + Bu'(a) \\Cu(a) + Du'(a) \end{pmatrix}.$ Therefore $u(b) = Au(a) + Bu'(a)$, $u'(b) = Cu(a) + Du'(a)$, and similarly for the other solution $v$. Substitute those values into the given boundary condition, and you should end up with an equation involving $\det S = AD-BC.$

Ok! I got it! (Yes)

I have also an other question.

$v^*$ is the complex conjugate of $v$.
At the beginning of the solution do I have to suppose that $v$ is a solution or $v^*$?
 
When $v$ is a solution of the eigenvalue problem, then is the complex conjugate $v^*$ also a solution? (Wondering)
 
mathmari said:
When $v$ is a solution of the eigenvalue problem, then is the complex conjugate $v^*$ also a solution? (Wondering)

That depends.
Let's see...

If $v$ is a solution, then we have:
\begin{array}{}
(pv')' + qv &=& \lambda v \\

((pv')' + qv)^* &=& (\lambda v)^* \\

(p^* {v^*}')' + q^* v^* &=& \lambda^* v^* \\
\end{array}

In other words, $v^*$ is the solution of:
$$(p^*y')' + q^*y = \lambda^* y$$

So we can only expect $v^*$ to be a solution of the original ODE if $p=p^*$ and $q=q^*$ (both real-valued).
The associated eigenvalue would then be the conjugate of the original eigenvalue.
 
I like Serena said:
That depends.
Let's see...

If $v$ is a solution, then we have:
\begin{array}{}
(pv)' + qv &=& \lambda v \\

((pv')' + qv)^* &=& (\lambda v)^* \\

(p^* {v^*}')' + q^* v^* &=& \lambda^* v^* \\
\end{array}

In other words, $v^*$ is the solution of:
$$(p^*y')' + q^*y = \lambda^* y$$

So we can only expect $v^*$ to be a solution of the original ODE if $p=p^*$ and $q=q^*$ (both real-valued).
The associated eigenvalue would then be the conjugate of the original eigenvalue.

Aha! Ok! So to use the sentence with the Wronskian, I have to suppose that $u$ and $v^*$ are solutions, right?
 
mathmari said:
Aha! Ok! So to use the sentence with the Wronskian, I have to suppose that $u$ and $v^*$ are solutions, right?

I don't know, since I haven't found useful references linking the Wronskian to Sturm-Liouville (yet).
My expectation is that $v$ should be the solution.
But what does your course material say exactly?
 
I like Serena said:
I don't know, since I haven't found useful references linking the Wronskian to Sturm-Liouville (yet).
My expectation is that $v$ should be the solution.
But what does your course material say exactly?

$L$ is the differential operator.

$$Lu(x)=P_o(x)\frac{d^2u}{dx^2}+P_1(x)\frac{du}{dx}+P_2(x)u$$
We suppose that $P_j(x) \in C^2(\mathbb{R})$

We define the dot product $(v(x),u(x))=\int_a^b{v^*(x) u(x)}dx$, where $v^*(x)$ is the complex conjugate.

$(v,Lu)=\int_a^b{v^*(P_o(x)\frac{d^2u}{dx^2}+P_1(x)\frac{du}{dx}+P_2(x)u)}dx= \cdots =[P_o(v^*u'-v^{*'}u)+(P_1-P_0')v^*u]_a^b+\int_a^b{[\frac{d}{dx^2}(P_0v^*)-\frac{d}{dx}(P_1v^*)+P_2v^*]u}dx$

We define the conjugate operator
$$\widetilde{L}u=\frac{d^2}{dx^2}(P_0u)-\frac{d}{dx}(P_1u)+P_2u$$

$$(v,Lu)=[P_0(v^*u'-v^{*'}u)+(P_1-P_0')v^*u]_a^b+(\widetilde{L}v,u)$$

Now we take the special case where:
$a) P_1=P_0'$
$b) \text{Boundary Conditions } [P_0(x)(v^*u'-v^{*'}u)]_a^b=0$

$$(v,Lu)=(\widetilde{L}v,u)$$

Self-adjoint is called an operator when $L=\widetilde{L}$

$\widetilde{L}u=\frac{d^2}{dx^2}(P_0u)-\frac{d}{dx}(P_1u)+P_2u=P_0u''+(2P_0'-P_1)u'+(P_0''-P_1'+P_2)u$

When $(a)$ stands, then:
$\widetilde{L}u=P_0u''+P_1u'+P_2u=Lu$

When $(a)$ and $(b)$ stand, then the operator is indeed self-adjoint.

$=\frac{d}{dx}(P_0\frac{du}{dx})+P_2u=Lu$

$P_0=p, P_2=q$
$\frac{d}{dx}(p\frac{du}{dx})+qu=Lu=\widetilde{L}u$

The eigenvalue problem $Lu=λu$, where the operator $L$ is given by the relation:
$\frac{d}{dx}(p\frac{du}{dx})+qu=Lu=\widetilde{L}u$ and the boundary conditions satisfy $[p(uv^{*'}-u'v^*)]_a^b=0 (*)$, where $u(x), v(x)$ are solutions of the eigenvalue problem, is called Sturm-Liouville problem.

The relation $(*)$ can be written as $P_0(x)W(u(x), v^*(x)) |_a^b=0$
 
  • #10
mathmari said:
The eigenvalue problem $Lu=λu$, where the operator $L$ is given by the relation:
$\frac{d}{dx}(p\frac{du}{dx})+qu=Lu=\widetilde{L}u$ and the boundary conditions satisfy $[p(uv^{*'}-u'v^*)]_a^b=0 (*)$, where $u(x), v(x)$ are solutions of the eigenvalue problem, is called Sturm-Liouville problem.

The relation $(*)$ can be written as $P_0(x)W(u(x), v^*(x)) |_a^b=0$

That's a whole lot to digest. (Whew)

Either way, I'm reading: "$u(x), v(x)$ are solutions of the eigenvalue problem".
That clearly means the $v$ is the solution of the ODE and $v^*$ is merely its conjugate, which shows up when taking an inner product.
 
  • #11
I like Serena said:
That's a whole lot to digest. (Whew)

Either way, I'm reading: "$u(x), v(x)$ are solutions of the eigenvalue problem".
That clearly means the $v$ is the solution of the ODE and $v^*$ is merely its conjugate, which shows up when taking an inner product.

Ok! But at the exercise I have to use that $v^*$ satisfies the given boundary conditions, how can I use this when I suppose that $v$ is a solution? (Wondering)
 
  • #12
Supposing that $v$ is a solution of the eigenvalue problem, can I just use that $v^{*}$ satisfies the boundary conditions or do I have to write also something from the theory according to the dot product? (Wondering)
 
  • #13
Let's suppose that $v$ is a solution.
So, $$\begin{pmatrix}
v(b)\\
v'(b)
\end{pmatrix}=\begin{pmatrix}
A & B\\
C & D
\end{pmatrix} \begin{pmatrix}
v(a)\\
v'(a)
\end{pmatrix} \Rightarrow v(b)=A v(a)+B v'(a) \text{ and } v'(b)=C v(a)+D v'(a)$$

The complex conjugate of $v(b)=A v(a)+B v'(a)$ is $v^*(b)=A v^*(a)+B v^{*'}(a)$ and of $ v'(b)=C v(a)+D v'(a)$ it's $v^{*'}(b)=C v^*(a)+D v^{*'}(a)$, isn't it? (Wondering) (If we suppose that $A,B,C,D$ are real numbers)
 
  • #14
mathmari said:
Let's suppose that $v$ is a solution.
So, $$\begin{pmatrix}
v(b)\\
v'(b)
\end{pmatrix}=\begin{pmatrix}
A & B\\
C & D
\end{pmatrix} \begin{pmatrix}
v(a)\\
v'(a)
\end{pmatrix} \Rightarrow v(b)=A v(a)+B v'(a) \text{ and } v'(b)=C v(a)+D v'(a)$$

The complex conjugate of $v(b)=A v(a)+B v'(a)$ is $v^*(b)=A v^*(a)+B v^{*'}(a)$ and of $ v'(b)=C v(a)+D v'(a)$ it's $v^{*'}(b)=C v^*(a)+D v^{*'}(a)$, isn't it? (Wondering) (If we suppose that $A,B,C,D$ are real numbers)

Yes.
But indeed only if we suppose that $A,B,C,D$ are real numbers.
Can it be that there is some more context to your problem that specifies this? (Wondering)
Because it seems to me this is necessary information to solve the problem.
 

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