Is QCD free from all divergences?

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Solution 1

What Gross means is that QCD is well defined in the ultraviolet, so that if you take a lattice version and send the lattice spacing to zero, there is no divergence in the coupling as you take the lattice spacing small. Instead, the coupling goes to zero as the inverse logarithm of the lattice spacing, so very slowly.

This doesn't mean that QCD perturbation theory doesn't have ultraviolet divergences, it has those like any other unitary interacting field theory in 4d. These ultraviolet divergences though are not a sign of a problem with the theory, since the lattice definition works fine. This is in contrast to, say, QED, where the short lattice spacing limit requires the bare coupling to blow up, and it is likely that the theory blows up to infinite coupling at some small but finite distance. This is certainly what happens in the simplest interacting field theory, the quartically self-interacting scalar.

There is no proof that the limit of small lattice spacing gives a proper continuum limit for QCD, but the difficulties are of a stupid technical nature--- there is absolutely no doubt that it is true. The full proof will require a better handle on the best way to define continuum limits for statistical fluctuating fields within mathematics.

Solution 2

After renormalization (with infinite counterterms), QCD is utraviolet finite, which means that it has a sensible renormalized perturbation theory at sufficiently high energies = small distances.

The vanishing bare coupling referred to by David Gross means that there are divergences at finite coupling, but the true coupling is infinitesimal (i.e., vanishes in the limit of no regularization) and the renormalization technology extracts finite contributions in the limit of inifinitesimal coupling.

However, QCD still has severe infrared divergences (at small energies = large distances, which are not cured by renormalization. Because of confinement of quarks, these IR divergences are much more severe than in QED (where they can be resolved using coherent states), and techniques for handling these are not well developed.

In addition, QCD has - like all field theories - only an asymptotic perturbation series, which means that the series itself will also diverge if all terms are summed.

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Updated on July 20, 2020

Comments

  • DJBunk
    DJBunk over 3 years

    On page 8 in The Triumph And Limitations Of Quantum Field Theory David Gross makes the following comment:

    "This theory [QCD] has no ultraviolet divergences at all. The local (bare) coupling vanishes, and the only infinities that appear are due to the fact that one sometimes expresses observables measured at finite distances in terms of those measured at infinitely small distances. "

    1. First of all, is this statement even correct?

    2. Now my main question is: certainly, a naive application of the Feynman rules and regularization leads to non zero counterterms. (See chap 16 of Peskin). So what scheme could one work in such that the counterterms vanish?

    • stupidity
      stupidity over 11 years
      I don't undersand this too!! I learned all this divergence/regularization/renormalization stuff from calculating the QCD $\beta$-function which amounts to calculating a number of ultraviolet divergent integrals!!
    • Qmechanic
      Qmechanic almost 10 years
      Minor comment to the post (v1): In the future please link to abstract pages rather than pdf files, e.g., arxiv.org/abs/hep-th/9704139
  • Ron Maimon
    Ron Maimon over 11 years
    Yes, but all these questions are moot, since the theory is well defined on a lattice, where you don't need perturbations.
  • Arnold Neumaier
    Arnold Neumaier over 11 years
    @RonMaimon: The lattice itself is a regularization, not the full theory. And on an infinite lattice, the IR problems are fully present. Working in the approximation but claiming its results for the exact theory without qualification is poor scientific style.
  • user1504
    user1504 over 11 years
    @ArnoldNeumaier: I think Ron's point is that the QFT we call QCD is defined to be a continuum limit of lattice regularizations. This does not involve any UV divergences; the only UV divergences which appear result from the degenerate nature of continuum perturbation theory.
  • Arnold Neumaier
    Arnold Neumaier over 11 years
    @user1504: QCD is defined by its action, not by a quaetionable contimuum limit of lattice regularizations. (If the limiting process were understood, the confinement problem would have been solved.) Indeed, different workers on QCD use (and need) quite different regularizations, depending on what they want to compute.
  • user1504
    user1504 over 11 years
    @ArnoldNeumaier: I take issue with the assertion that the short distance perturbation theory defines QCD. First, to make a definition with perturbation theory, you have to choose a renormalization scheme; the action alone isn't sufficient. So you're defining the theory via its effective approximations in any case. And the lattice definition generalizes the perturbation theory for the short distance degrees of freedom; this is why perturbation-improved lattice gauge theory works.
  • Arnold Neumaier
    Arnold Neumaier over 11 years
    @user1504: What is taken as definition depends on the author. It was defined by the action at the time QCD was established, and however it is defined by anyone, it must give the same perturbative series as the definition at that time. The lattice regularization is derived from the action, hence secondary. None of the current limiting definitions is mathematically sound. Thus people define it by what they like best, and this differs among those working in QCD. - In any case, the large-distance behavior on a lattice is not under control, so infrared divergences have no real cure yet.
  • Jose Javier Garcia
    Jose Javier Garcia over 10 years
    in any case aren't IR divergences 'artificial' ? i mean IR divergences are for $ p \to 0 $ or $ \lambda \to \infty $ but how can the wavelenght of a particle be bigger that the size of the universo shouldn't we have a IR cut-off so $ \lambda _{max =size-of-the-universe $
  • Arnold Neumaier
    Arnold Neumaier about 10 years
    @JoseJavierGarcia: The standard model is an idealization in which the universe is an unbounded Minkowski space. My remarks refer to this theory. At present there is no more comprehensive theory that would indicate how QCD would have to be modified in a finite universe.
  • Turgon
    Turgon about 5 years
    @JoseJavierGarcia I think you misunderstood what IR divergence is. It appears when particles are soft or/and collinear, and while it has something to do with large length scale, there's hardly any direct correspondence. The problem with QCD is actually a problem of confinement, because if you have unbound quark, by KLN theorem there's no IR divergence. However it's neither possible or practical to sum over all final states involving hadrons, thus KLN theorem is not applied.