Integration involving spherical harmonics

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Homework Help Overview

The discussion revolves around evaluating the integral ∫∫dΩ V(Ω)Yml(Ω) where V(Ω) takes different values based on the angle θ. The context involves spherical harmonics and their properties, particularly in relation to integration over specified regions of a sphere.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss splitting the integral into two parts corresponding to different regions of the sphere and question the application of orthonormality properties of spherical harmonics. There is also mention of rewriting V(Ω) to utilize these properties. Some participants explore the implications of integrating over φ and the resulting expressions involving Legendre polynomials.

Discussion Status

The discussion is active with various approaches being considered. Some participants suggest that the integral should be straightforward while others express uncertainty about the implications of the spherical harmonics' properties. There is no explicit consensus on the best approach, but multiple interpretations and methods are being explored.

Contextual Notes

Participants are navigating the complexities introduced by the integral's limits and the nature of the functions involved. The discussion reflects a focus on the mathematical properties of spherical harmonics and their integration rather than providing a direct solution.

lordkelvin
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Homework Statement



Evaluate the integral ∫∫dΩ V(Ω)Yml(Ω) for V(Ω) = +V0 for 0<θ<π/2 ; -V0 for π/2<θ<π


Homework Equations


I was hoping to apply the orthonormality properties of the spherical harmonics but this is a little more difficult since the integral breaks into two integrals over half spheres instead of one integral over a full sphere.

I guess it may be useful to rewrite the V(Ω) as ±√(4π)Y00(Ω)V0 in order to invoke the orthogonality properties of the spherical harmonics when integrated on a sphere.


The Attempt at a Solution



Basically I've split the integral into two integrals over the upper and lower halves of the sphere. Now what? Surely I'm not to use the definition of the spherical harmonics; there must be a cleaner way to do this by invoking the properties of Ylm(omega). There is nothing I can say about ∫∫half of spheredΩYlm(Y00)* as far as I know. Is there some way to combine the two integrals again so that I can use the orthonormality property?
 
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Orthonormality won't really help here because you're not integrating the product of two spherical harmonics. The integral should be pretty straightforward though. Start by integrating φ out first. Then you'll be left with an integral involving a Legendre polynomial.
 
I get zero. I think this is so since Ylm(θ,\phi) = const* e^(i*\phi)*Plm(cos(\theta) and so the integral over phi yields zero.
 
It's e^{im\phi}, not e^{i\phi}. It makes a difference.
 
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