Solution to Laplace's equation in spherical co-ordinates

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The general solution to Laplace's equation in spherical coordinates involves a linear combination of spherical harmonics. When solving for potential within two concentric spherical shells, the coefficients B_{lm} do not vanish in the outer volume, which does not include the origin. Conversely, in the inner volume that contains the origin, the coefficients B_{lm} do vanish. Between the two spheres, both coefficients A and B remain non-zero. This understanding is crucial for accurately determining the potential in such geometries.
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I have a question about the general solution to Laplace's equation in spherical co-ordinates, which takes the form of a linear combination of the spherical harmonics. In my problem, I am solving for the potential within two concentric spherical shells, each with its own conductivity. Now, since the outer volume does not contain the origin, am I right to assume that the coefficients B_{lm} do not vanish? For the inner volume, which does contain the origin, am I right in assuming that the coefficients B_{lm} do vanish?
 
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Yes. In between the spheres, neither A nor B vanishes.
 
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