Renormalization and divergent integrals.

In summary, the issue with renormalization is that there are divergent integrals for x-->oo. One possible solution could be to make a change by using rectangles with a small base 'j' and approximating the divergent integral with a divergent series, then using Borel or other types of resummation. However, this approach may not work for all field theories and there are obstructions to Borel resummation.
  • #1
Klaus_Hoffmann
86
1
If the problem of renormalization is that there are divergent integrals for x-->oo couldn't we make the change.

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

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 [tex] f(x)= \frac{C}{x^{n}} [/tex] n >0 we could apply some kind of 'Hadamard finite-part integral' or Cauchy Principal Value to get finite results
 
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  • #2
Klaus_Hoffmann said:
If the problem of renormalization is that there are divergent integrals for x-->oo couldn't we make the change.

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

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.
 
  • #3
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.
 
  • #4
Why not 'Haelfix' ?? if a integral is divergent a series is also divergent.

the easiest example is the finite value attached to divergent integral

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

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

[tex] \sum_{n=-\infty}^{\infty}a_{n}z^{n} [/tex]

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...
 
  • #5
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)
 
  • #6
You mean that the integrals are not Borel summable or that you can't find the Borel transform of the sequence a(n) mainly:

[tex] \sum_{n=0}^{\infty}\frac{a_{n}}{n!}x^{n} [/tex]

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

1. What is renormalization and why is it important in scientific research?

Renormalization is a mathematical technique used to eliminate divergences (infinities) in physical theories, particularly in quantum field theory. It allows for the calculation of meaningful and finite physical quantities, making it an essential tool in understanding the behavior of particles at very small scales.

2. How does renormalization work?

Renormalization involves rescaling certain parameters in a theory to account for the effects of virtual particles, which are constantly being created and destroyed. These virtual particles contribute to the overall energy of the system, causing divergences in calculations. By adjusting the parameters, renormalization allows for the removal of these infinities.

3. Are all divergent integrals eliminated through renormalization?

No, not all divergent integrals can be removed through renormalization. Some may still persist, but they can often be interpreted as physical effects, such as the mass or charge of particles. Others may require further theoretical developments to be understood.

4. Can renormalization be applied to any physical theory?

Renormalization is primarily used in quantum field theory, but it can also be applied to other areas of physics, such as statistical mechanics and condensed matter physics. However, it may not be applicable in all cases, and alternative methods may need to be used.

5. What are the limitations of renormalization?

Renormalization is a powerful tool, but it is not a complete solution to all problems in physics. It relies on certain assumptions and approximations, and its results may not always be physically meaningful. Additionally, the technique can become increasingly complex and difficult to apply in more complicated physical systems.

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