Square root of volume in fourier expansion of the vector potential

In summary, the use of 1/\sqrt{V} in the Fourier expansion of the vector potential is just a convention that is sometimes used in quantum theory of radiation to avoid the appearance of V in the expression of the Poynting energy. It does not affect the dimension of the vector potential itself, but introduces a different dimension for \vec A_{0\vec k}.
  • #1
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Hi. I just wondered why we use a [itex] 1/\sqrt{V}[/itex] in the Fourier expansion of the vector potential. A regular 3 dimensional Fourier expansion is just

[tex] f(\vec r) = \sum_{\vec k} c_\vec{k} e^{i \vec k \cdot \vec r}[/tex]

but as the solution to the equation

[tex] (\frac{\partial ^2}{\partial t^2} - \nabla^2 ) \vec A(\vec r,t) = 0[/tex]

one usually writes

[tex] \vec A(\vec r,t) = \frac{1}{\sqrt{V}}\sum_{\vec k} \vec A_{0 \vec{k}}(t) e^{i \vec k \cdot \vec r}.[/tex]

What is the reason for this? Doesn't this also screw up the dimension of the euation when [itex]\vec A_{0 \vec k}[/itex] already has the same dimension as the vector potential since the plane wave solutions are

[tex] \vec A_{0 \vec k}(t) e^{i \vec k \cdot \vec r}?[/tex]
 
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  • #2
why we use a 1/V−−√ in the Fourier expansion of the vector potential

It is just a convention. Perhaps you came across it in a book on quantum theory of radiation, where it is sometimes used because it leads to expression of the Poynting energy of the field in the box V in which V does not appear.

If we used the standard convention

[tex]
\vec A(\vec r,t) = \sum_{\vec k} \vec A_{0 \vec{k}}(t) e^{i \vec k \cdot \vec r},
[/tex]

the integration over volume would introduce the prefactor V in the total Poynting energy.

...Doesn't this also screw up the dimension of the euation when A⃗ 0k⃗ already has the same dimension as the vector potential...

The dimension of [itex]\vec A(\vec r,t)[/itex] stays the same as in the standard convention, but the dimension of [itex]\vec A_{0\vec k}[/itex] is [itex][ A(\vec r,t) ] \mathrm{m}^{3/2} [/itex].
 

1. What is the concept of "square root of volume" in Fourier expansion of the vector potential?

The square root of volume in Fourier expansion of the vector potential refers to the normalization factor used in the Fourier transform to ensure that the transformed function has the same units as the original function. In the case of the vector potential, this factor is the square root of the volume in which the function is defined.

2. How is the square root of volume calculated in Fourier expansion?

The square root of volume is calculated by taking the square root of the product of the dimensions of the volume in which the function is defined. For example, if the function is defined in a three-dimensional volume with dimensions of length, width, and height, the square root of volume would be the square root of (length x width x height).

3. Why is the square root of volume important in Fourier expansion?

The square root of volume is important in Fourier expansion because it normalizes the transformed function and ensures that the units of the original function and the transformed function are consistent. This is crucial in mathematical and scientific applications where precise units and measurements are necessary.

4. How does the square root of volume affect the Fourier transform of a function?

The square root of volume does not affect the actual transformation of the function, but it is used to scale the transformed function to have the same units as the original function. In other words, it ensures that the transformed function is a true representation of the original function.

5. Can the square root of volume be applied to other types of functions besides the vector potential?

Yes, the concept of the square root of volume can be applied to any function that is being transformed using Fourier expansion. It is a general normalization factor used to ensure consistency between the original and transformed functions.

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