1 3 Ju l 1 99 9 1 What QCD Tells Us About Nature – and Why We Should Listen ∗

نویسنده

  • Frank Wilczek
چکیده

1.1. It embodies deep and beautiful principles. These are, first of all, the general principles of quantum mechanics, special relativity, and locality, that lead one to relativistic quantum field theory [1]. In addition, we require invariance under the nonabelian gauge symmetry SU(3), the specific matter content of quarks – six spin 1/2 Dirac fermions which are color triplets – and renormalizability. These requirements determine the theory completely, up to a very small number of continuous parameters as discussed below. Deeper consideration reduces the axioms further. Theoretical physicists have learned the hard way that consistent, non-trivial relativistic quantum field theories are difficult to construct, due to the infinite number of degrees of freedom (per unit volume) needed to construct local fields, which tends to bring in ultraviolet divergences. To construct a relativistic quantum theory, one typically introduces at intermediate stages a cutoff, which spoils the locality or relativistic invariance of the theory. Then one attempts to remove the cutoff, while adjusting the defining parameters, to achieve a finite, cutoff-independent limiting theory. Renormalizable theories are those for which this can be done, order by order in a perturbation expansion around free field theory. This formulation, while convenient for mathematical analysis, obviously begs the question whether the perturbation theory converges (and in practice it never does). A more straightforward procedure, conceptually, is to regulate the theory as a whole by discretizing it, approximating space-time by a lattice [2]. This spoils the continuous space-time symmetries of the theory. Then one attempts to remove dependence on the discretization by refining it, while if necessary adjusting the defining parameters, to achieve a finite limiting theory that does not depend on the discretization, and does respect the space-time symmetries. The redefinition of parameters is necessary, because in refining

برای دانلود متن کامل این مقاله و بیش از 32 میلیون مقاله دیگر ابتدا ثبت نام کنید

ثبت نام

اگر عضو سایت هستید لطفا وارد حساب کاربری خود شوید

منابع مشابه

X iv : h ep - p h / 99 07 34 0 v 2 1 5 Ju l 1 99 9 1 What QCD Tells Us About Nature – and Why We Should

1.1. It embodies deep and beautiful principles. These are, first of all, the general principles of quantum mechanics, special relativity, and locality, that lead one to relativistic quantum field theory [1]. In addition, we require invariance under the nonabelian gauge symmetry SU(3), the specific matter content of quarks – six spin 1/2 Dirac fermions which are color triplets – and renormalizab...

متن کامل

ar X iv : h ep - t h / 99 07 03 4 v 2 1 1 Ju l 1 99 9 Nature : ” I have Two Times ”

This is a slightly extended version of a seminar given the 8th of June at the TASI 99 at Colorado University in Boulder. The motivations behind two time theory are explained and the theory is introduced via one of the theory’s easier gauges of a particle on a black hole background. Important results that should be interesting as well in the light of the recent AdS mania will be summarized. 1 Mo...

متن کامل

ar X iv : h ep - l at / 9 60 70 86 v 1 3 1 Ju l 1 99 6 1 Random matrix model approach to chiral symmetry

We review the application of random matrix theory (RMT) to chiral symmetry in QCD. Starting from the general philosophy of RMT we introduce a chiral random matrix model with the global symmetries of QCD. Exact results are obtained for universal properties of the Dirac spectrum: i) finite volume corrections to valence quark mass dependence of the chiral condensate, and ii) microscopic fluctuatio...

متن کامل

SU(2)L × SU(2)R and U(1)A restorations high in the hadron spectrum and what it tells us about.

SU (2) L × SU (2) R and U (1) A restorations high in the hadron spectrum and what it tells us about. Abstract Recent data for highly excited mesons suggest that not only the chiral SU (2) L × SU (2) R symmetry of QCD is restored high in the spectrum but also the U (1) A symmetry. This means that it is not a confining interaction in QCD which triggers the spontaneous breaking of chiral symmetry....

متن کامل

ذخیره در منابع من


  با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید

برای دانلود متن کامل این مقاله و بیش از 32 میلیون مقاله دیگر ابتدا ثبت نام کنید

ثبت نام

اگر عضو سایت هستید لطفا وارد حساب کاربری خود شوید

عنوان ژورنال:

دوره   شماره 

صفحات  -

تاریخ انتشار 1999