1964
DOI: 10.1007/bf02734585
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Lagrangian theory for neutral massive spin-2 fields

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Cited by 108 publications
(98 citation statements)
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“…In the calculation of the inverse kinetic operator, necessary to determine the graviton propagator, we employ an algorithm based on the Barnes-Rivers rank-two spin projectors [86][87][88][89][90][91], given by P (1) µν,κλ = 1 2 (θ µκ ω νλ + θ µλ ω νκ + θ νκ ω µλ + θ νλ ω µκ ) , P (2) µν,κλ = 1 2 (θ µκ θ νλ + θ µλ θ νκ ) − 1 3 θ µν θ κλ ,…”
Section: Remarks and Conclusionmentioning
confidence: 99%
“…In the calculation of the inverse kinetic operator, necessary to determine the graviton propagator, we employ an algorithm based on the Barnes-Rivers rank-two spin projectors [86][87][88][89][90][91], given by P (1) µν,κλ = 1 2 (θ µκ ω νλ + θ µλ ω νκ + θ νκ ω µλ + θ νλ ω µκ ) , P (2) µν,κλ = 1 2 (θ µκ θ νλ + θ µλ θ νκ ) − 1 3 θ µν θ κλ ,…”
Section: Remarks and Conclusionmentioning
confidence: 99%
“…They confirm the results of Refs. [14][15][16] regarding the existence of other ghost-free second-order models different from the FP theory, contrary to early works [9][10][11][12][13].…”
Section: Discussionmentioning
confidence: 66%
“…The general case of a second-order (in derivatives) Lagrangian for an arbitrary rank-2 tensor e has been investigated in the past in Refs. [9][10][11][12][13]. They concluded that the massive FP theory is the only possibility which avoids ghosts.…”
Section: Introductionmentioning
confidence: 99%
“…Using these operators, we may write the complete set of the D-dimensional Barnes-Rivers operators [1,16] as…”
Section: Appendix A: Barnes-rivers Operatorsmentioning
confidence: 99%