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Sokhatsky-Weierstrass theorem
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The Sokhatsky-Weierstrass theorem (also spelled Sokhotsky-Weierstrass theorem, and also called the Weierstrass theorem, although the latter term has several, more common, alternate meanings) is a theorem in complex analysis, which helps in evaluating certain Cauchy-type integrals, among many other applications. It is often used in physics, although rarely referred to by name. The theorem is named after Yulian Sokhotski and Karl Weierstrass.
Proof of the theorem A simple proof is as follows.
For the first term, we note that is an approximate identity, and therefore approaches a Dirac delta function in the limit. Therefore, the first term equals .
For the second term, we note that the factor approaches 1 for |x| >> e, approaches 0 for |x| << e, and is exactly symmetric about 0. Therefore, in the limit, it turns the integral into a Cauchy principal value integral.
Physics application In quantum mechanics and quantum field theory, one often has to evaluate integrals of the form
where E is some energy and t is time. This expression, as written, is undefined (since the time integral does not converge), so it is typically modified by adding a negative real coefficient to t in the exponential, and then taking that to zero, i.e.:
where the latter step uses this theorem.
uses this theorem.
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