Can zeta regularization provide FINITENESS to quantum field theory ?

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Discussion Overview

The discussion revolves around the potential of zeta regularization to provide finiteness in quantum field theory (QFT). Participants explore the implications of zeta regularization and its relationship to other regularization methods, as well as its application in specific contexts like the Casimir effect and string theory.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • One participant questions whether zeta regularization can provide finiteness in QFT, referencing papers that claim it can yield finite results for divergences.
  • Another participant asserts that while dimensional regularization is related, no regularization scheme can prove finiteness; they argue that these schemes merely rewrite infinite results in a way that allows for consistent calculations.
  • A participant mentions that zeta regularization yields correct results for the Casimir effect, suggesting that similar procedures could yield finite answers in other contexts.
  • One participant draws an analogy between zeta regularization and geometric series, suggesting that the existence of finite expressions may be obscured by the infinities encountered in QFT.
  • A question is raised about whether all logarithmic divergences can be expressed in a specific integral form, and whether changes of variables in integrals are permissible from a renormalization perspective.
  • Concerns are expressed about the understanding of mass in QFT, with references to the vagueness of particles being point-like and the implications for computational approaches.
  • Another participant notes that a referenced paper may not be directly related to zeta-function regularization, despite discussing concepts of renormalization.

Areas of Agreement / Disagreement

Participants express differing views on the effectiveness of zeta regularization in providing finiteness in QFT. There is no consensus on whether zeta regularization can definitively yield finite results, and multiple competing perspectives remain regarding the nature of divergences and regularization methods.

Contextual Notes

Some participants highlight the limitations of current understanding in QFT, particularly regarding the treatment of infinities and the mathematical expressions used. The discussion reflects ongoing uncertainties and challenges in the field.

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Yes. It's called dimensional regularization in this context. Nobel prize of '99 is based on this.
 


zetafunction said:
can zeta regularization provide FINITENESS to quantum field theory ??
No, strictly speaking not.

All regularization schemes simply re-write the infinite result for an amplitude or a Green's function as an infinite term + a finite term. The regularization expresses the infinite term as a regulated expression which, when the regulator is removed, becomes infinite again. The regularization scheme allows you to drop the infinities in a consistent manner for all amplitudes you want to calculate. The remaining finite terms contain the physical information.

So no regularization scheme (zeta-function, dim. reg., Pauli-Villars, ...) provides a proof of finiteness; they simply manage to "hide" the infinities in a consistent manner. The expressions are still divergent, or - mathematically speaking - do not exist.
 


however for Casimir effect the zeta regularization gives the CORRECT answer \sum_{n=1}^{\infty}n^{3} = \zeta (-3)
http://en.wikipedia.org/wiki/Casimir_effect#Casimir.27s_calculation

shouldn't we expect the same for similar procedures involving zeta regularization ? , the idea si that perhaps the REGULARIZATION procedures 'hide' the infinities away to get FINITE answers that can be contrasted by experiments is somehow as it nature 'sees analytic continuation' and in the end you get finite answers.

Also in string theory the zeta regularized value 1+2+3+4+5+...= -1/12 appears to be consistent with the fact that bosoinc string is only valid for 23 dimensions.
 


Yes, it is something like this.

Compare it to the geometric series. You have f(q) = 1+q+q²+q³+ ... and you know that you can rewrite the series as f(q) = (1-q)-1. You know that the series converges for |q| < 1. Once you have the expression f(q) = (1-q)-1 for some q with |q| > 1 it would be silly to write it as a series as that would mean to throw away a finite expression and replace it by something that diverges; nobody would do that ...

But in QFT, especially in a perturbative approach, all you have is the diverging expression. You can't re-sum it explicitly to get the finite expression, you have to live with the infinities that are created by such a stupid approach. Of course you would be happy to be able to use finite expressions only, but unfortunately nobody is able to derive them. Therefore you have to live with the infinities.

[Attention: don't get me wrong, my example with the geometric series is not in one-to-one correspondence with QFT; it is not the re-summation of the power series in the coupling constant, but applies to every individual term in the perturbation expansion; it is only an example where you replace a finite expression by something infinite]

So my guess is that the reason why regularization and hiding of infinities works is a hint that there is an underlying finite expression which is still to be discovered. The infinities arise simply because we have not yet managed to express QFT correctly, that means based on finite quantities only. The point where everything gets "wrong" is when you start to use perturbation theory. Perhaps the problem arises even earlier when you take a classical action integral and use it as a starting point for the construction of a quantum field theory.Perhaps already the replacement of fields with field operators is the wrong turn, I am not so sure about that. But it definitely becomes "wrong" when you use perturbation theory.

So we believe that there is something like f(q) = (1-q)-1 but unfortunately we only know f(q) = 1+q+q²+q³+ ... .

[Remark: there are hints that non-perturbative calculations or new theories like SUGRA or strings may cure this mess. As far as I understood the latest ideas rearding finiteness in SUGRA there could be a different turn where it usually gets wrong in QFT. It could very well be that it is not allowed to use Green's functions G(Q²) off-shell. As far as I understood the approaches to prove finiteness of SUGRA, they rely on on-shell symmetries of G(Q²). Nevertheless it means that we use the wrong expressions and that the correct ones are still to be discovered]
 
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thanks Tom a last question regarding this paper, can ALL logarithmic divergences be re-written as \int_{0}^{\infty}dx \frac{log^{k}(x)}{x+a} for some constants (positive) a and k ?

and from the renormalization point of view .. would it be licit to make a change of variable ? for example

\int_{0}^{\infty}dx \frac{1}{x} becomes under the change of variable e^{u}=x the logarithmic divergent integral becomes the UV divergent integral \int_{-\infty}^{\infty}du
 


zetafunction said:
... can ALL logarithmic divergences be re-written as \int_{0}^{\infty}dx \frac{log^{k}(x)}{x+a} for some constants (positive) a and k ?
I am sorry, I don't know.
 


The problem is with the mass, it is still not well understood. The particle being a point and having properties is very vague. We all know the work around, anybody who works with software knows how that works.
 


qsa said:
The problem is with the mass, it is still not well understood. The particle being a point and having properties is very vague. We all know the work around, anybody who works with software knows how that works.


Please check this post #240 for more info


https://www.physicsforums.com/showthread.php?p=2665832#post2665832

What do you think, Tom?

Zeta look up the paper in the link you will see a new kind of regularizaion/renormalization.
 
  • #10


Interesting, but it has not really much to do with zeta-function regularization.
 
  • #11


tom.stoer said:
Interesting, but it has not really much to do with zeta-function regularization.

You are right Tom, I just ment this section on page 5, as a general concept.


V RENORMALIZATION BY GRAVITY AND
REGULARIZATION OF SELF-ENERGY


Of course After reading more carefully, I found out that the theory is a branch of Twister theory.
 

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