Massive gravity as a quantum gauge theory |
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Authors: | Grigore D. R. Scharf G. |
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Affiliation: | (1) Department of Theor. Phys., Inst. Atomic Phys., Bucharest-Mgurele, P.O. Box MG 6, ROMâNIA;(2) Institute of Theor. Phys., Univ Zürich, Winterthurerstr 190, 8057 Zürich, SWITZERLAND |
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Abstract: | We present a new point of view on the quantization of the massive gravitational field, namely we use exclusively the quantum framework of the second quantization. The Hilbert space of the many-gravitons system is a Fock space F+ (Hgraviton) where the one-particle Hilbert space Hgraviton carries the direct sum of two unitary irreducible representations of the Poincaré group corresponding to two particles of mass m > 0 and spins 2 and 0, respectively. This Hilbert space is canonically isomorphic to a space of the type Ker(Q)/Im(Q) where Q is a gauge charge defined in an extension of the Hilbert space Hgraviton generated by the gravitational field h and some ghosts fields u, (which are vector Fermi fields) and v (which is a vector Bose field).Then we study the self interaction of massive gravity in the causal framework. We obtain a solution which goes smoothly to the zero-mass solution of linear quantum gravity up to a term depending on the bosonic ghost field. This solution depends on two real constants as it should be; these constants are related to the gravitational constant and the cosmological constant. In the second order of the perturbation theory we do not need a Higgs field, in sharp contrast to Yang-Mills theory. |
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Keywords: | Gravitational field Quantum gravity Gauge field theories |
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