2014
DOI: 10.1088/0264-9381/31/15/159501
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Corrigendum: Generalized ghost-free quadratic curvature gravity (2014 Class. Quantum Grav. 31 015022)

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Cited by 78 publications
(76 citation statements)
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“…8 This point has been stressed repeatedly by Tomboulis [16,27], and also by Biswas [28]. 9 If I were working with Weyl term instead of Riemann, the constraint a(−k 2 ) = c(−k 2 ) would lead to following constraint: 6F 1 (¯ ) + 3F 2 (¯ ) + 2F 3 (¯ ) = 0, see [19]. Now, along with Eqs.…”
Section: Graviton Propagator and Ghost Free Actionmentioning
confidence: 89%
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“…8 This point has been stressed repeatedly by Tomboulis [16,27], and also by Biswas [28]. 9 If I were working with Weyl term instead of Riemann, the constraint a(−k 2 ) = c(−k 2 ) would lead to following constraint: 6F 1 (¯ ) + 3F 2 (¯ ) + 2F 3 (¯ ) = 0, see [19]. Now, along with Eqs.…”
Section: Graviton Propagator and Ghost Free Actionmentioning
confidence: 89%
“…The only difference will be and addition contribution from cosmological constant ±Λ. One can also recast the action in terms of S µν = R µν − (1/4)g µν R and the Weyl C µνλ σ instead of R µνλ σ , see [19].…”
Section: Infinite Derivative Gravity (Idg)mentioning
confidence: 99%
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“…The most general torsion-free, parity-invariant and quadratic covariant action that contains an infinite number of derivatives has been constructed around constant curvature backgrounds, and reads [5,[21][22][23]:…”
Section: Infinite Derivative Ghost-free and Singularity-free Gravitymentioning
confidence: 99%