516 research outputs found

    Spatial Geometry of the Electric Field Representation of Non-Abelian Gauge Theories

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    A unitary transformation \Ps [E]=\exp (i\O [E]/g) F[E] is used to simplify the Gauss law constraint of non-abelian gauge theories in the electric field representation. This leads to an unexpected geometrization because \o^a_i\equiv -\d\O [E]/\d E^{ai} transforms as a (composite) connection. The geometric information in \o^a_i is transferred to a gauge invariant spatial connection \G^i_{jk} and torsion by a suitable choice of basis vectors for the adjoint representation which are constructed from the electric field EaiE^{ai}. A metric is also constructed from EaiE^{ai}. For gauge group SU(2)SU(2), the spatial geometry is the standard Riemannian geometry of a 3-manifold, and for SU(3)SU(3) it is a metric preserving geometry with both conventional and unconventional torsion. The transformed Hamiltonian is local. For a broad class of physical states, it can be expressed entirely in terms of spatial geometric, gauge invariant variables.Comment: 16pp., REVTeX, CERN-TH.7238/94 (Some revision on Secs.3 and 5; one reference added

    Lebed' and Rodionov: Views on Russia's Security

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    Reformulating Yang-Mills theory in terms of local gauge invariant variables

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    An explicit canonical transformation is constructed to relate the physical subspace of Yang-Mills theory to the phase space of the ADM variables of general relativity. This maps 3+1 dimensional Yang-Mills theory to local evolution of metrics on 3 manifolds.Comment: Lattice 2000 (Gravity and Matrix Models) 3 pages, espcrc2.st

    Yang--Mills Configurations from 3D Riemann--Cartan Geometry

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    Recently, the {\it spacelike} part of the SU(2)SU(2) Yang--Mills equations has been identified with geometrical objects of a three--dimensional space of constant Riemann--Cartan curvature. We give a concise derivation of this Ashtekar type (``inverse Kaluza--Klein") {\it mapping} by employing a (3+1)(3+1)--decomposition of {\it Clifford algebra}--valued torsion and curvature two--forms. In the subcase of a mapping to purely axial 3D torsion, the corresponding Lagrangian consists of the translational and Lorentz {\it Chern--Simons term} plus cosmological term and is therefore of purely topological origin.Comment: 14 pages, preprint Cologne-thp-1994-h1

    Russia-India relations: the significance of subjective factors

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    Sergei Lunev argues that Russia should pursue improved political and economic relations with India, despite the many setbacks in the partnership. This is the second of two posts examining parallels and bilateral relations between India and Russia. Click here for a post titled ‘Globalisation: Many Indias, many Russias’

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