439 research outputs found

    Parity Conservation and Bootstraps

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    Symmetry Breaking in the Schr\"odinger Representation for Chern-Simons Theories

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    This paper discusses the phenomenon of spontaneous symmetry breaking in the Schr\"odinger representation formulation of quantum field theory. The analysis is presented for three-dimensional space-time abelian gauge theories with either Maxwell, Maxwell-Chern-Simons, or pure Chern-Simons terms as the gauge field contribution to the action, each of which leads to a different form of mass generation for the gauge fields.Comment: 16pp, LaTeX , UCONN-94-

    Remark on charge conjugation in the non relativistic limit

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    We study the non relativistic limit of the charge conjugation operation C\cal C in the context of the Dirac equation coupled to an electromagnetic field. The limit is well defined and, as in the relativistic case, C\cal C, P\cal P (parity) and T\cal T (time reversal) are the generators of a matrix group isomorphic to a semidirect sum of the dihedral group of eight elements and Z2\Z_2. The existence of the limit is supported by an argument based in quantum field theory. Also, and most important, the limit exists in the context of galilean relativity. Finally, if one complexifies the Lorentz group and therefore the galilean spacetime xμx_\mu, then the explicit form of the matrix for C\cal C allows to interpret it, in this context, as the complex conjugation of the spatial coordinates: xx\vec{x} \to \vec{x}^*. This result is natural in a fiber bundle description.Comment: 8 page

    Gluon Condensates, Chiral Symmetry Breaking and Pion Wave Function

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    We consider here chiral symmetry breaking in quantum chromodynamics arising from gluon condensates in vacuum. Through coherent states of gluons simulating a mean field type of approximation, we show that the off-shell gluon condensates of vacuum generate a mass-like contribution for the quarks, giving rise to chiral symmetry breaking. We next note that spontaneous breaking of global chiral symmetry links the four component quark field operator to the pion wave function. This in turn yields many hadronic properties in the light quark sector in agreement with experiments, leading to the conclusion that low energy hadron properties are primarily driven by the vacuum structure of quantum chromodynamics.Comment: 25 pages, IP/BBSR/92-76, revte

    Bose-Einstein condensation for interacting scalar fields in curved spacetime

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    We consider the model of self-interacting complex scalar fields with a rigid gauge invariance under an arbitrary gauge group GG. In order to analyze the phenomenon of Bose-Einstein condensation finite temperature and the possibility of a finite background charge is included. Different approaches to derive the relevant high-temperature behaviour of the theory are presented.Comment: 28 pages, LaTe

    Slavnov-Taylor identities in Coulomb gauge Yang-Mills theory

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    The Slavnov-Taylor identities of Coulomb gauge Yang-Mills theory are derived from the (standard, second order) functional formalism. It is shown how these identities form closed sets from which one can in principle fully determine the Green's functions involving the temporal component of the gauge field without approximation, given appropriate input.Comment: 20 pages, no figure

    Action Principle and Algebraic Approach to Gauge Transformations in Gauge Theories

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    The action principle is used to derive, by an entirely algebraic approach, gauge transformations of the full vacuum-to-vacuum transition amplitude (generating functional) from the Coulomb gauge to arbitrary covariant gauges and in turn to the celebrated Fock-Schwinger (FS) gauge for the abelian (QED) gauge theory without recourse to path integrals or to commutation rules and without making use of delta functionals. The interest in the FS gauge, in particular, is that it leads to Faddeev-Popov ghosts-free non-abelian gauge theories. This method is expected to be applicable to non-abelian gauge theories including supersymmetric ones.Comment: LaTeX, 12 pages, Corrected typo

    A Finite Quantum Gravity Field Theory Model

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    We discuss the quantization of Delta gravity, a two symmetric tensors model of gravity. This model, in Cosmology, shows accelerated expansion without a cosmological constant. We present the δ~\tilde{\delta} transformation which defines the geometry of the model. Then we show that all delta type models live at one loop only. We apply this to General Relativity and we calculate the one loop divergent part of the Effective Action showing its null contribution in vacuum, implying a finite model. Then we proceed to study the existence of ghosts in the model. Finally, we study the form of the finite quantum corrections to the classical action of the model.Comment: Latex, 33 page
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