Reciprocal lattice and Fourier series

touqra
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First off, this is not a homework problem. I was reading Charles Kittel solid states book on Chapter 2, equation 3:

electron number density, n(x), expanded in a Fourier series:

n(x) = n_0 + \sum_{p} [C_p cos(\frac{2\pi p x}{a}) + S_p sin(\frac{2\pi p x}{a})]

From this expansion, wouldn't the density n(x = 0) be infinity ? since C_p shouldn't be zero for the Fourier expansion to make sense.
 
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Why shouldn't C_p be zero for it to make sense? You realize that the value of C_p depends on p, right? So there could be C_p values which are non-zero and others which are zero.
 
Basically Fourier series repersentation is applied to functions which are bounded.The next thing is that you have to check for appropriate Dirichlet's conditions.

Thus at the very beginning, a peassumption for applying Fourier series expansion is that the function it represents is always finite.
More simply speaking, kanato is right.
O.K.?
 
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