Error in Modern Theory of Critical Phenomena by Shang-Keng Ma

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The discussion centers on the mathematical expressions presented in Shang-Keng Ma's book, "Modern Theory of Critical Phenomena," specifically on page 17, which detail the relationship between continuous and discrete Fourier transforms. The equations provided illustrate the transformation of a function in real space, σ(x), into its Fourier space representation, σ(k), and vice versa. The participants clarify that when the x-domain is bounded, the k-domain becomes discrete, akin to the behavior of Fourier series for periodic functions. This confirms the validity of the inversion process between continuous and discrete Fourier transforms under specific conditions.

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In book Modern theory of critical phenomena author Shang - Keng Ma in page 17.

[tex]\sigma_{\vec{k}}=V^{-\frac{1}{2}}\int d^3\vec{x}e^{-i\vec{k}\cdot\vec{x}}\sigma(\vec{x})[/tex]

[tex]\sigma(\vec{x})=V^{-\frac{1}{2}}\sum_{\vec{k}}e^{i\vec{k}\cdot \vec{x}}\sigma_{\vec{k}}[/tex]

Is this correct? How can inversion of continual FT be discrete FT? Thanks for your answer.
 
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The sum is to be understood as an integral over a comb of very narrow functions which approach delta functions in the limit V to infinity, i.e. think of the FT of a product of a periodic function with a rectangle of width V.
The integral over the delta functions is then equivalent to a sum over their locations.
 
matematikuvol said:
In book Modern theory of critical phenomena author Shang - Keng Ma in page 17.

[tex]\sigma_{\vec{k}}=V^{-\frac{1}{2}}\int d^3\vec{x}e^{-i\vec{k}\cdot\vec{x}}\sigma(\vec{x})[/tex]

[tex]\sigma(\vec{x})=V^{-\frac{1}{2}}\sum_{\vec{k}}e^{i\vec{k}\cdot \vec{x}}\sigma_{\vec{k}}[/tex]

Is this correct? How can inversion of continual FT be discrete FT? Thanks for your answer.

If the x-domain is bounded, the k-domain will be discrete. This is what happens for an ordinary Fourier series for functions on a bounded domain, or periodic:

http://en.wikipedia.org/wiki/Fourier_series
 

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