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16 votes
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Why do we need the Condon-Shortley phase in spherical harmonics?

You don't need it: it's a sign convention and the only thing you need to do with it is to be consistent. (In particular, this means always checking that the sign and normalization conventions for $Y_{...
Emilio Pisanty's user avatar
10 votes
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Why in QM the solution to Laguerre equations are ONLY Laguerre polynomials?

This is related to the fact that the solutions in the textbook are written only for the discrete spectrum of energies. We are interested in the normalized solutions, i.e. such that \begin{equation*} \...
OON's user avatar
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5 votes
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Green Function expressed in terms of Hankel function (of the second kind)

There is a useful class of dummy integration variable trick, which applies also later when calculating Feynman diagrams. You can make the following observation: $$ \frac{1}{x} = \int_0^{+\infty}dt e^{-...
LPZ's user avatar
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3 votes
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Spherical Bessel Equation has different forms?

To arrive at this, I begin manipulating the Radial equation: $$\frac{d}{dr}\left(r^2\frac{dR}{dr}\right)-\frac{2mr^2}{\hbar^2}(V(r)-E)R=l(l+1)R$$ You forgot some factors of $r$ while manipulating ...
Lucky Charms's user avatar
3 votes

What does it mean that Zernike's polynomials form a orthogonal basis on the unit disk?

It means that any function (sensible) $f(\rho, \phi)$ defined on the unit circle can be expanded into a linear combination of Zernike polynomials: $$ f(\rho, \phi) = \sum_{m,n}{a_{m,n}R_n^m(\rho)\cos{...
JEB's user avatar
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3 votes

Addition theorem for Spherical Bessel function

The identity you seek is $$j_0(|\vec{p}-\vec{p}\,'|r)=\sum_{n=0}^{\infty}(2n+1)j_n(pr)j_n(p'r)P_n(\cos\theta).$$ It follows from (10.60.2) here.
G. Smith's user avatar
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3 votes
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Spherical Harmonics Sum Identity

In the process of proving the sum rule \begin{equation} \sum_{m=-l}^l |Y_l^m(\theta,\phi)|^2 = \frac{2l+1}{4\pi} \, , \end{equation} you often start from the more general addition theorem for the ...
secavara's user avatar
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3 votes
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References regarding Green's function on a square domain in 2D

Thanks to @Nephente advice, I'm now able to answer my question. Finding the Green's function for the Laplacian in a 2D square can be considered as a particular case of the more general problem of ...
3 votes

What physically determines Bessel functions' orders?

The "$n$" in the $J_n(\kappa r)$ refers to the number of nodes in the angular direction. A complete set of eigenfunctions of $-\nabla^2$ in ${\mathbb R}^2$ are $$ \psi_{n,\kappa}(r,\theta)= e^{in\...
mike stone's user avatar
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2 votes

Is there a generating function for Hermite polynomials of 2n?

Of course. Parity. Recall $$ H_{2n+1}(x) + H_{2n+1}(-x)=0, \qquad H_{2n}(x) + H_{2n}(-x)= 2 H_{2n}(x), $$ so that $$ e^{2xt -t^2} + e^{-2xt -t^2} = \sum_{n=0}^{\infty} (H_{n}(x)+H_n(-x) ) \frac{...
Cosmas Zachos's user avatar
2 votes
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Why are some associated Legendre functions not orthogonal to each other?

Because the orthogonality is supplied by the azimuthal direction when the two $z$-components of the angular momentum differ. This is why we usually bundle them together into the spherical harmonics ...
Sean E. Lake's user avatar
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2 votes
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How fast should you rotate a chain hoop so that it doesn't tilt?

Segments of chain in the loop are subject to tension forces from each side. The resultant of these must have a radial component which provides the centripetal acceleration, and a vertical component ...
R.W. Bird's user avatar
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2 votes
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Deriving recurrence of the Hermite polynomials

$$ g(0,t)= e^{-t^2}= \sum_m {(-t^2)^m \over m!}= \sum_n H_n(0) {t^n\over n!} \leadsto \\ H_n(0) = \begin{cases} 0 & \text{for odd }n, \\ (-2)^\frac{n}{2} (n-1)!! & \text{for even }n. \...
Cosmas Zachos's user avatar
2 votes

Manipulating Hypergeometric functions

I think you want the connection formulae that link solutions about the three regular singular points to each other. There is a brief discussion starting on page 408 of my lecture notes: http://...
mike stone's user avatar
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2 votes

Commutator of raising operator in angular momentum with partial derivative wrt z

You are aiming to show $$ [p_z,L_x+iL_y]= p_x+ip_y. $$ Have set $\hbar=1$ for simplicity. This near duplicate answer works out $$ [p_i, L_j] = i \epsilon_{ijm}p_m, $$ yielding your answer. As @...
Cosmas Zachos's user avatar
1 vote

What is the form of general expression (one expression) for the eigenfunctions of discrete and continuous spectra of motion in the Coulomb potential?

There is no unified expression, because we simply have two different ordinary differential equations, each with its own set of solutions, according to whether a certain parameter (eventually found to ...
DanielC's user avatar
  • 4,421
1 vote

What does a star on a spherical harmonic mean?

It has nothing to do with spherical harmonics in particular, an asterisk is one of the common notations for the complex conjugate.
ACuriousMind's user avatar
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1 vote
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Orthonormalization condition for $L^2$ operator

The differential solid angle (in spherical polar coordinate ) is $$d\Omega=\sin\theta \ d\theta \ d\phi$$ $$\int_0^{2\pi}\int_0^\pi d\Omega \ Y^*_{l'm'}(\theta,\phi) \ Y_{lm}(\theta,\phi)=\int_0^{2\...
Himanshu's user avatar
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1 vote

What is the general solution of the Associated Legendre differential equation when $A$ does not equal $\ell(\ell+1)$?

What is the general solution of the Associated Legendre differential equation when $A$ does not equal $\ell(\ell+1)$? When you allow $\ell$ and $m$ to be arbitrary complex numbers $\lambda$ and $\mu$,...
G. Smith's user avatar
  • 52.2k
1 vote

To what extent can one recover plane waves from the Airy eigenfunctions of a linear potential as the field is turned off?

Let me add a few aspects being somewhat complementary to the already existing answers. The crucial point of your interesting problem is the fact that the spectrum $\sigma(H_{F_0})$ of the operator $$...
Hyperon's user avatar
  • 7,298
1 vote

Integral of Hermite functions

I found in the work of Groenwold, 1946, a closed form for the solution of \begin{equation} k_{mn}(\zeta_1,\zeta_2)=\frac{1}{\sqrt{\pi 2^{m+n} m!n!}}\int_{\mathbb R} \mathrm d \zeta \; e^{-\zeta^2} H_{...
Graz's user avatar
  • 385
1 vote
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Integral of Hermite functions

By experimenting in Mathematica I found that $$\int_{-\infty}^\infty d\zeta e^{-\zeta^2}H_n(\zeta+\zeta_1)H_{n-1}(\zeta+\zeta_2)= \sqrt{\pi}2^n(n-1)!\zeta_1L_{n-1}^1(-2\zeta_1\zeta_2)$$ holds for $n=...
G. Smith's user avatar
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1 vote

Is there a generating function for Hermite polynomials of 2n?

....A far more convenient formulation is actually available, which expresses the $\,H_n\,$ in terms of a generating function $\,S\left(\xi,s\right)$. \begin{equation} S\left(\xi,s\right)\...
Voulkos's user avatar
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1 vote

Different levels of physical model solvability and why reality doesn't care

If reality follows the same rules, why is it so "easy" for her to move the planets in the solar system according to GR and produce atoms with many electrons, hyperfine structure and whatnot, while we ...
Mitchell Porter's user avatar
1 vote

Expanding the Green's function in spherical harmonics

It is both the symmetry and the reality of the Green's function that implies this. For example, if I know $A\left(\theta\right)Y\left(\theta^{\prime}\right)$ is both symmetric and real, then \begin{...
Andrew's user avatar
  • 263
1 vote
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On fusion transformation in Liouville CFT

First of all let me point out that Ponsot-Teschner has been superseded by Teschner-Vartanov https://arxiv.org/abs/1202.4698 , whose formulas are more symmetric (although not less complicated). Then ...
Sylvain Ribault's user avatar
1 vote

Resources for special functions

I absolutely recommend the text by James Seaborn Hypergeometric functions and their applications. This text is completely approachable and contains all the special functions required at the ...
1 vote
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Manipulating Hypergeometric functions

With a substitution $x\equiv r/R$ one can transform the ODE into a hypergeometric equation: $$x(1-x)\phi''(x)-\phi'(x)+l(l+1)\phi(x)=0.$$ This corresponds to $(a,b,c)=(-1-l,l,-1)$ or equivalently $(l,-...
N0va's user avatar
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