2006
DOI: 10.1103/physrevd.74.124014
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Conformally invariant wave equations and massless fields in de Sitter spacetime

Abstract: Conformally invariant wave equations in de Sitter space, for scalar and vector fields, are introduced in the present paper. Solutions of their wave equations and the related two-point functions, in the ambient space notation, have been calculated. The "Hilbert" space structure and the field operator, in terms of coordinate independent de Sitter plane waves, have been defined. The construction of the paper is based on the analyticity in the complexified pseudo-Riemanian manifold, presented first by Bros et al..… Show more

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Cited by 49 publications
(57 citation statements)
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“…This CI equation is similar to the gauge-fixed wave equation for the vector field∂ · K α [6,24]. We are now in a position to write CI system for dS field K αβ .…”
Section: Dirac's Six-cone Conformally Invariant Equationsmentioning
confidence: 99%
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“…This CI equation is similar to the gauge-fixed wave equation for the vector field∂ · K α [6,24]. We are now in a position to write CI system for dS field K αβ .…”
Section: Dirac's Six-cone Conformally Invariant Equationsmentioning
confidence: 99%
“…Wave equations, subsidiary conditions, etc., must be expressed in terms of operators that are defined intrinsically on the cone. These are well-defined operators that map tensor fields on tensor fields with the same rank on cone u 2 = 0 [6,21]. It is important to note that on the cone u 2 = 0, the second order Casimir operator of conformal group, Q 2 , is not a suitable operator to obtain CI wave equations.…”
Section: Dirac's Six-cone Conformally Invariant Equationsmentioning
confidence: 99%
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