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Category Archives: Differential Equations
SelfAdjoint Differential Equations III: Real Eigenvalues, GramSchmidt Orthogonalization
In here, I mentioned that the eigenvalues of a Hermitian operator are real and that the eigenfunctions of a Hermitian operator are orthogonal. Let $\mathcal{L}$ be a Hermitian operator and let $u_i$, $u_j$ be eigenfunctions of $\mathcal{L}$ with eigenvalues $\lambda_i$, … Continue reading
SelfAdjoint Differential Equations II: Hermitian Operators
Let $\mathcal{L}$ be a secondorder selfadjoint differential operator. Then $\mathcal{L}u(x)$ may be written as $$\mathcal{L}u(x)=\frac{d}{dx}\left[p(x)\frac{du(x)}{dx}\right]+q(x)u(x)\ \ \ \ \ (1)$$ as we discussed here. Multiply (1) by $v^\ast$ ($v^\ast$ is the complex conjugate of $v$) and integrate \begin{align*} \int_a^bv^\ast\mathcal{L}udx&=\int_a^bv^\ast\frac{d}{dx}\left[p(x)\frac{du(x)}{dx}\right]dx+\int_a^bv^\ast qudx\\ … Continue reading
Posted in Differential Equations, Mathematical Physics
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SelfAdjoint Differential Equations I
Let $\mathcal{L}$ be the secondorder linear differential operator $$\mathcal{L}=p_0(x)\frac{d^2}{dx^2}+p_1(x)\frac{d}{dx}+p_2(x)$$ which acts on a function $u(x)$ as $$\mathcal{L}u(x)=p_0(x)\frac{d^2u(x)}{dx^2}+p_1(x)\frac{du(x)}{dx}+p_2(x)u(x).\ \ \ \ \ (1)$$ Define an adjoint operator $\bar{\mathcal{L}}$ by \begin{align*} \bar{\mathcal{L}}&:=\frac{d^2}{dx^2}[p_0u]\frac{d}{dx}[p_1u]+p_2u\\ &=p_0\frac{d^2u}{dx^2}+(2p_0^\primep_1)\frac{du}{dx}+(p_0^{\prime\prime}p_1+p_2)u. \end{align*} If $\mathcal{L}=\bar{\mathcal{L}}$, $\mathcal{L}$ is said to be selfadjoint. … Continue reading
Posted in Differential Equations, Mathematical Physics
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Legendre Functions II: Recurrence Relations and Special Properties
In this lecture, we derive some important recurrence relations of Legendre functions and use them to show that Legendre functions are indeed solutions of a differential equation, called Legendre’s differential equation. Differentiating the generating function $$g(x,t)=(12xt+t^2)^{1/2}=\sum_{n=0}^\infty P_n(x)t^n,\ t<1\ \ \ … Continue reading