Renormalization and divergent integrals.

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Discussion Overview

The discussion revolves around the concept of renormalization in quantum field theory, specifically addressing the challenges posed by divergent integrals and the potential methods for handling them, such as Borel resummation and other mathematical techniques. Participants explore theoretical implications and practical applications related to divergent series and integrals.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • Some participants propose approximating divergent integrals using a series representation and suggest methods like Borel resummation to address the divergences.
  • Others argue that if an integral is divergent, it remains divergent, and no resummation can change that, indicating a fundamental issue with the original Hamiltonian in quantum electrodynamics (QED).
  • A participant mentions that while Borel resummation can work for certain field theories, it does not apply universally, and there are examples where it fails.
  • Another participant highlights the use of the Hurwitz zeta function in approximating divergent integrals and suggests that finding the Borel sum for power-law divergent integrals is a straightforward task.
  • There is a discussion about the conditions under which integrals or series may not be Borel summable, questioning the existence of the Borel transform for specific sequences.

Areas of Agreement / Disagreement

Participants express differing views on the effectiveness of Borel resummation for divergent integrals, with some asserting its utility in specific cases while others maintain that it does not resolve the underlying issues of divergence. The discussion remains unresolved regarding the general applicability of these methods.

Contextual Notes

Limitations include the dependency on specific definitions of divergence and the conditions under which Borel resummation is applicable. The discussion does not reach a consensus on the validity or utility of the proposed methods across all scenarios.

Klaus_Hoffmann
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If the problem of renormalization is that there are divergent integrals for x-->oo couldn't we make the change.

\int_{0}^{\infty}dx f(x) \approx \sum_{n=0}^{\infty}f(nj)

using rectangles with base 'j' small , and approximating the divergent integral by a divergent series and 'summing' by Borel or other kind of resummation, to solve the problem

for Infrared divergences f(x)= \frac{C}{x^{n}} n >0 we could apply some kind of 'Hadamard finite-part integral' or Cauchy Principal Value to get finite results
 
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Klaus_Hoffmann said:
If the problem of renormalization is that there are divergent integrals for x-->oo couldn't we make the change.

\int_{0}^{\infty}dx f(x) \approx \sum_{n=0}^{\infty}f(nj)

using rectangles with base 'j' small , and approximating the divergent integral by a divergent series and 'summing' by Borel or other kind of resummation, to solve the problem

If the integral is divergent, it is divergent. Period. No "resummation" can change that. Divergent integrals in QED are signs of a serious problem. The problem is that the original Hamiltonian is wrong and cannot be used beyond the first non-vanishing order. Tomonaga-Schwinger-Feynman renormalization theory corrects this problem: (infinite) counterterms are added to the Hamiltonian. Then all infinities in S-matrix elements cancel out, and very accurate results are obtained.

Eugene.
 
Sometimes you can borel resum the integral in that way, there are examples of field theories like that (typically in d = 3). Unfortunately it doesn't work in the general case.
 
Why not 'Haelfix' ?? if a integral is divergent a series is also divergent.

the easiest example is the finite value attached to divergent integral

\int_{0}^{\infty}dp(1+ p)^{n} \approx h^{n+1} \zeta(1/h,-n)

where 'h' is the step and we have used the 'Hurwitz zeta function' since for a function we can make the expansion (Laurent series)

\sum_{n=-\infty}^{\infty}a_{n}z^{n}

the rest of the problem should be a trivial question, for a power-law divergent integral you must find the Borel sum of a certain sequence...
 
Eh? I never said the contrary.

Borel resummation is precisely the process whereby you try to make sense of certain classes of divergent series (or integrals, its a straightforward generalization).

Like I said, it works for some field theories, but not all of them (most do not). Actually, when you can find such an example, you tend to become rather famous, there are preciously few analytic results in QFT.

Try to Borel resum some of the textbook cases of field theories as an exercise, you will find there are obstructions to doing this. (In fact a lot was learned about general nonperturbative contributions by comparing perturbation theory and the analytic results in the few cases where we could resum)
 
You mean that the integrals are not Borel summable or that you can't find the Borel transform of the sequence a(n) mainly:

\sum_{n=0}^{\infty}\frac{a_{n}}{n!}x^{n}

or that there is a theorem that says ..that series with factor e^{iax} are not Borel summable.
 

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