2019
DOI: 10.1103/physrevd.100.086006
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Breakdown of the classical double copy for the effective action of dilaton-gravity at NNLO

Abstract: We demonstrate that a recently proposed classical double copy procedure to construct the effective action of two massive particles in dilaton-gravity from the analogous problem of two color charged particles in Yang-Mills gauge theory fails at next-to-next-to-leading orders in the post-Minkowskian (3PM) or post-Newtonian (2PN) expansions.

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Cited by 60 publications
(46 citation statements)
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“…This connection comes about from an effective field theory perspective where spinless blackholes may be modeled by massive scalar particles in the classical and large mass limit (for introductory reviews see [41][42][43]). While the double copy procedure could be efficiently applied up to the 1PN and 2PM level [18,[20][21][22][23][24]26] a recent double-copy construction at the 2PN and 3PM level of the present authors and Steinhoff revealed a disagreement with the known 2PN result in dilatongravity [44].…”
Section: Introductionmentioning
confidence: 97%
“…This connection comes about from an effective field theory perspective where spinless blackholes may be modeled by massive scalar particles in the classical and large mass limit (for introductory reviews see [41][42][43]). While the double copy procedure could be efficiently applied up to the 1PN and 2PM level [18,[20][21][22][23][24]26] a recent double-copy construction at the 2PN and 3PM level of the present authors and Steinhoff revealed a disagreement with the known 2PN result in dilatongravity [44].…”
Section: Introductionmentioning
confidence: 97%
“…In ref. [66] a first attempt was made to find a gauge-invariant double copy, where a general formula applicable for QCD amplitudes was given in terms of an unknown KLT-like 1 Curiously, a recent classical double-copy calculation of the effective action of two massive spinless particles failed to match the known next-to-next-to-leading order result [63]. It remains to be seen if this is because of some inherent problem, or simply due to the ambiguities present in off-shell unphysical quantities.…”
Section: Introductionmentioning
confidence: 99%
“…(3.9), the width of the slit around the bisecting line T = T ′ defined by the partie-finie procedure is dT = f (T )ǫ where ǫ is initially considered as being infinitesimal, before replacing it by the finite value 2s/c at the end. This leads to the following partie-finie integral 29) the above expression can be rewritten as 30) where ǫ = 2s/c. Note that q(T, T ′ ) is not (contrary to G(T, T ′ )) a symmetric function of T and T ′ .…”
mentioning
confidence: 99%