/ 93 02 04 5 v 1 9 F eb 1 99 3 Poincare invariance in temporal gauge canonical quantization and θ - vacua

نویسنده

  • Hisashi Kikuchi
چکیده

The Poincare invariance in the temporal gauge canonical quantization of QCD is shown manifestly by verifying the energy-momentumvector and angular-momentum-tensor satisfy the Poincare algebra in the physical Hilbert space. Two different values of θ for the θ-term in QCD lagrangian lead to different representations of the Poincare group, which are, however, connected by an unitary transformation. Thus the parameter θ becomes physically irrelevant unless we can further restrict the physical Hilbert space. 1

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

ar X iv : h ep - t h / 99 02 02 7 v 1 3 F eb 1 99 9 INFRARED REGION OF QCD AND CONFINEMENT

Gauge field configurations appropriate for the infrared region of QCD is proposed. Using the usual QCD action, confinement is realized as in the London theory of Meissner effect.

متن کامل

ar X iv : h ep - t h / 01 02 19 1 v 2 1 F eb 2 00 2 Wigner ’ s Little Group , Gauge Transformations and Dimensional Descent

Wigner’s little group[1], which is a subgroup of the Poincare group that leaves the fourmomentum invariant, is of fundamental importance for both massive and massless particles. In the latter case this group is E(2), which is a semi-direct product of T (2) (the group of translations in the plane) and SO(2). Each of these subgroups has its own role, but here we are concerned with T (2) which act...

متن کامل

ar X iv : h ep - t h / 96 02 01 3 v 1 3 F eb 1 99 6 Laughlin States on the Poincare half - plane and its quantum group symmetry

We find the Laughlin states of the electrons on the Poincare half-plane in different representations. In each case we show that there exist a quantum group su q (2) symmetry such that the Laughlin states are a representation of it. We calculate the corresponding filling factor by using the plasma analogy of the FQHE.

متن کامل

99 02 02 9 v 1 3 F eb 1 99 9 Vacuum structure in supersymmetric

Vacuum structure in supersymmetric Yang–Mills theories with any gauge group. Abstract We consider the pure supersymmetric Yang–Mills theories placed on a small 3-dimensional spatial torus with higher orthogonal and exceptional gauge groups. The problem of constructing the quantum vacuum states is reduced to a pure mathematical problem of classifying the flat connections on T 3 which is solved i...

متن کامل

ar X iv : h ep - p h / 94 02 30 1 v 1 1 6 Fe b 19 94 VPI - IHEP - 93 - 13 Inconsistency of QED in the Presence of Dirac Monopoles II

We enlarge the local gauge invariance of QED from U(1)A to U(1)A × U(1)Θ by introducing another unphysical pure gauge field Θ with an independent, unphysical gauge coupling ẽ . This pure gauge field can be gauge-transformed away and the resulting theory is identical to standard QED. We then re-examine the Dirac quantization condition (DQC) for point monopoles and find that two essentially diffe...

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 1993