Abstract
A reduction of degrees of freedom at large N is performed by representing space-time translations in the internal symmetry group. The reduced model for the U(∞) gauge theory is constructed in a translation invariant gauge. The rule is U(x, x+μ)→Dk(x)VμDk+(x) where Vμ belong to the coset U(N) U(1)N and Dk(x) is a diagonal plane-wave matrix representing translations. We show that at large N, the planar perturbation expansion of the gauge theory is identical to that of the reduced model.
Original language | English |
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Pages (from-to) | 228-232 |
Number of pages | 5 |
Journal | Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics |
Volume | 117 |
Issue number | 3-4 |
DOIs | |
State | Published - Nov 11 1982 |
Bibliographical note
Funding Information:'~ Work supported in part by the DOE: AE-AC02-81ER 10957A; and by the NSF: PHY79-23669. z Permanent address after October 1, 1982: Theoretical Phys-ics Group, Tata Institute of Fundamental Research, Homi Bhabha Road, Bombay-400005, India.
Funding
'~ Work supported in part by the DOE: AE-AC02-81ER 10957A; and by the NSF: PHY79-23669. z Permanent address after October 1, 1982: Theoretical Phys-ics Group, Tata Institute of Fundamental Research, Homi Bhabha Road, Bombay-400005, India.
Funders | Funder number |
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National Science Foundation (NSF) | PHY79-23669 |
Michigan State University-U.S. Department of Energy (MSU-DOE) Plant Research Laboratory | AE-AC02-81ER 10957A |
ASJC Scopus subject areas
- Nuclear and High Energy Physics