Physics Asked on July 30, 2021
In the book by Prof Nagaosa, the Lagrange density was given by Eq. (1)
(1)
Then, according to the Euler-Lagrange equation (Eq.(2)), we can do the derivatives of Lagrange density (e.g., Eq. (1)) with respect to .
By doing so, the Book by Prof Nagaosa indicates the following result:
(3)
Why the factor $1/2$ in front of the integral (over r‘) disappear?
This can be understood from the definition of functional variation, together with v(r-r')==v(r'-r) of Coulomb potential.
First of all, the functional derivative can be found here: https://en.wikipedia.org/wiki/Functional_derivative where you can find this: Clearly, this gives the derivative of the Lagrange equation:
Next, let me define functional J as a function of function L:
If we follow the definition of the functional derivative by taking
we should have (v(|r-r'|) is used; the derivative is exactly a mimic of fig.1 if you read the wiki carefully)
One interesting fact is that the 1/2 comes from the double-counting, and gets omitted by switching of r and r'.
Correct answer by Paul Chern on July 30, 2021
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