O(2) CHERN–SIMONS GAUGE THEORY AND Z2 ORBIFOLDS

1992 ◽  
Vol 07 (05) ◽  
pp. 1007-1023 ◽  
Author(s):  
KAORU AMANO ◽  
HIROSHI SHIROKURA

We quantize the three-dimensional O(2) pure Chern–Simons gauge field theory in a functional coherent-state representation. Both trivial and nontrivial flat O(2) bundles admit physical states. An explicit calculation relates the state functionals to the rational Z2-orbifold models.

1990 ◽  
Vol 05 (05) ◽  
pp. 959-988 ◽  
Author(s):  
MICHIEL BOS ◽  
V.P. NAIR

Three-dimensional Chern-Simons gauge theories are quantized in a functional coherent state formalism. The connection with two-dimensional conformal field theory is found to emerge naturally. The normalized wave functionals are identified as generating functionals for the chiral blocks of two-dimensional current algebra.


1994 ◽  
Vol 09 (26) ◽  
pp. 2399-2410
Author(s):  
M. LAGRAA

We consider pure 2−d supergravity as a flat OSp (1,2/2) superconnection of a super-gauge field theory on a (2, 2)−d supermanifold. From an appropriate Wigner-Inonu contraction of the OSp (1,2/2) algebra, we show that the superzweibein [Formula: see text] and the U(1) superconnection ΩM of 2−d supergravity transmute into BRST multiplets composed of the fields, their ghosts and the auxiliary fields of gauge theory of topological 2−d gravity. These fields and their topological BRST transformations can be recast in this geometric formalism where the “gravitino” now plays the role of ghost related to the zweibein shift of topological 2−d gravity. We close this paper by constructing a gauge fixed term of the quantum action in terms of superfield.


1993 ◽  
Vol 48 (21) ◽  
pp. 15787-15791 ◽  
Author(s):  
L. Martina ◽  
O. K. Pashaev ◽  
G. Soliani

2002 ◽  
Vol 16 (20n22) ◽  
pp. 3199-3202
Author(s):  
P. A. MARCHETTI ◽  
Z.-B. SU ◽  
L. YU

The U(1)×SU(2) Chern-Simons gauge field theory, proposed by the authors to explain in a unified fashion the metal-insulator crossover of the in-plane resistivity upon temperature decrease in heavily underdoped cuprates without magnetic field and a similar phenomenon, observed in several classes of superconducting cuprates, when a strong magnetic field suppresses the superconductivity, is briefly outlined and confronted with recent experiments.


1996 ◽  
Vol 11 (21) ◽  
pp. 1713-1728 ◽  
Author(s):  
O.K. PASHAEV

The classical spin model in planar condensed media is represented as the U(1) Chern-Simons gauge field theory. When the vorticity of the continuous flow of the media coincides with the statistical magnetic field, which is necessary for the model’s integrability, the theory admits zero curvature connection. This allows us to formulate the model in terms of gauge-invariant fields whose evolution is described by the Davey-Stewartson (DS) equations. The Self-dual Chern-Simons solitons described by the Liouville equation are subjected to the corresponding integrable dynamics. As a by-product the (2+1)-dimensional zero-curvature representation for the DS equation is obtained as well as the new reduction conditions related to the DS-I case. The physical interpretation of the Bäcklund transformations in terms of the Chern-Simons gauge theory is given. Some possible applications for the statistical transmutation in the anyon superfluid and TQFT are briefly discussed.


2007 ◽  
Vol 22 (29) ◽  
pp. 2201-2208 ◽  
Author(s):  
YISHI DUAN ◽  
XINHUI ZHANG ◽  
LI ZHAO

Based on the decomposition of U(1) gauge potential theory and the ϕ-mapping topological current theory, the three-dimensional knot invariant and a four-dimensional new topological invariant are discussed in the U(1) gauge field.


Sign in / Sign up

Export Citation Format

Share Document