What is the coinciding point limit of these two parametrized terms?

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SUMMARY

The discussion focuses on evaluating the coinciding point limit of two parametrized terms involving integrals and series in the context of quantum mechanics. The terms include exponential functions and oscillatory integrals, specifically using parameters such as mass (m), charge (e), electric field strength (E), and length of the box (L). The participant has utilized Mathematica to analyze the behavior of the integrals, noting that one integral decays like 1/n for large n, leading to expectations of a logarithmic form in the sum. The main inquiry is whether there exists an analytic method to expand the integral dependent on n into a series format.

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Homework Statement


The story is that I would like to evaluate the coinciding point limit (when ## (x^0, x^1)→(y^0,y^1)##) of these two terms:

\begin{eqnarray*}
&&\frac{1}{2L}e^{\frac{i}{2}eE\left((x ^1)^2-(y^1)^2\right)}\left( im\left( x^0-y^0+ x^1-y^1\right) \right) \sum_{n=0}^{\infty}e^{-ik_n( x^0-y^0+x^1-y^1)}\\
&&\times \frac{1}{L}\int_{-L/2}^{L/2}dx\left( -1\right)^{n}\cos \left( eE\left(\frac{L^2}{4} -x^2\right) +\left( 2n+1\right) \pi \frac{x}{L}\right) \\
&&+\frac{1}{2L}e^{\frac{i}{2}eE\left((x ^1)^2-(y^1)^2\right)}m \sum_{n=0}^{\infty} e^{-ik_n( x^0-y^0+x^1-y^1)}\\
&&\times \frac{1}{L}\int_{-L/2}^{L/2}dx\left(-1 \right)^{n}\left(2x-L \right)\sin\left( eE\left(\frac{L^2}{4}-x^2 \right)+\left(2n+1\right)\pi \frac{x}{L} \right)
\end{eqnarray*}

m, e, E, L are respectively the mass, charge, electric field strength, length of the box, and are constant. The energy levels ##k_n##'s are given by ##k_n=(n+1/2)\frac{\pi}{L}##.

Homework Equations

& 3. The Attempt at a Solution [/B]

1. There will be no singularities since another calculation of mine has shown that.

2. When I put ## \frac{1}{L}\int_{-L/2}^{L/2}dx\left( -1\right)^{n}\cos \left( eE\left(\frac{L^2}{4} -x^2\right) +\left( 2n+1\right) \pi \frac{x}{L}\right) ## in Mathematica, I got something that decays like ##\frac{1}{n}##, when ##n## is large.

So I expect the sum will give me ##\log (1-exp...)## (appropriate dissipative term ##\pm i \epsilon## may be needed); of course there will be some residue.

3. My burning question is: is there an analytic way to expand the integral which depends on ##n## as ##\frac{C}{n}+D+...##, for some constant ##C, D##, which are to be found?

Thanks!
 
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The limit for the first term should be obvious from inspection.

The limit for the second term has a divergent series ##\sum_{n=0}^{\infty} 1##.

The integrals look like monsters to do analytically (although it appears possible), why not just observe the behaviour of the other terms and use some simple limit laws?
 

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