Chapter 15: Problem 9
Derive the indicial equation for the Riemann DE.
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Chapter 15: Problem 9
Derive the indicial equation for the Riemann DE.
These are the key concepts you need to understand to accurately answer the question.
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Verify the following relations: (a) \(\quad Y_{n+1 / 2}(z)=(-1)^{n+1} J_{-n-1 / 2}(z), \quad Y_{-n-1 / 2}(z)=(-1)^{n} J_{n+1 / 2}(z)\), (b) \(Y_{-v}(z)=\sin v \pi J_{v}(z)+\cos v \pi Y_{v}(z)=\frac{J_{v}(z)-\cos v \pi J_{-v}(z)}{\sin v \pi}\), (c) \(Y_{-n}(z)=(-1)^{n} Y_{n}(z)\) in the limit \(v \rightarrow n\) in part (b).
The linear combination $$ \begin{aligned} \Psi(\alpha, \gamma ; z) \equiv & \frac{\Gamma(1-\gamma)}{\Gamma(\alpha-\gamma+1)} \Phi(\alpha, \gamma ; z) \\ &+\frac{\Gamma(\gamma-1)}{\Gamma(\alpha)} z^{1-\gamma} \Phi(\alpha-\gamma+1,2-\gamma ; z) \end{aligned} $$ is also a solution of the CHGDE. Show that the Hermite polynomials can be Written as $$ H_{n}\left(\frac{z}{\sqrt{2}}\right)=2^{n} \Psi\left(-\frac{n}{2}, \frac{1}{2} ; \frac{z^{2}}{2}\right) $$.
Obtain the following integral identities: $$ \begin{array}{l} \text { (a) } \int z^{v+1} J_{v}(z) d z=z^{v+1} J_{v+1}(z) \\ \text { (b) } \int z^{-v+1} J_{v}(z) d z=-z^{-v+1} J_{v-1}(z) \\ \text { (c) } \int z^{\mu+1} J_{v}(z) d z=z^{\mu+1} J_{v+1}(z)+(\mu-v) z^{\mu} J_{v}(z) \\ \quad-\left(\mu^{2}-v^{2}\right) \int z^{\mu-1} J_{v}(z) d z \end{array} $$ and evaluate $$ \text { (d) } \int z^{3} J_{0}(z) d z \text { . } $$ Hint: For (c) write \(z^{\mu+1}=z^{\mu-v} z^{v+1}\) and use integration by parts.
Show that the Jacobi functions are related to the hypergeometric functions.
Theorem \(15.2 .6\) states that under certain conditions, linearly independent solutions of SOLDE at regular singular points exist even though the difference between the characteristic exponents is an integer. An example is the case of Bessel functions of half-odd-integer orders. Evaluate the Wronskian of the two linearly independent solutions, \(J_{v}\) and \(J_{-v}\), of the Bessel equation and show that it vanishes only if \(v\) is an integer. This shows, in particular, that \(J_{n+1 / 2}\) and \(J_{-n-1 / 2}\) are linearly independent. Hint: Consider the value of the Wronskian at \(z=0\), and use the formula \(\Gamma(v) \Gamma(1-v)=\pi / \sin v \pi\).
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