arXiv:1607.01784v2 [hep-th] 19 Sep 2016 July 2016 MIT-CTP-4815 On the curious spectrum of duality invariant higher-derivative gravity Olaf Hohm,1Usman Naseer,2and Barton Zwiebach2 1Simons Center for Geometry and Physics, Stony Brook University, Stony Brook, NY 11794-3636, USA 2Center for Theoretical Physics, Massachusetts Institute of Technology Cambridge, MA 02139, USA ohohm@scgp.stonybrook.edu,unaseer@mit.edu,zwiebach@mit.edu Abstract We analyze the spectrum of the exactly duality and gauge invariant higher-derivative double field theory. While this theory is based on a chiral CFT and does not correspond to a standard string theory, our analysis illuminates a number of issues central in string theory.The full quadratic action is rewritten as a two-derivative theory with additional fields. This allows for a simple analysis of the spectrum, which contains two massive spin-2 ghosts and massive scalars, in addition to the massless fields.Moreover, in this formulation, the massless or tensionless limitα′→ ∞is non-singular and leads to an enhanced gauge symmetry.We show that the massive modes can be integrated out exactly at the quadratic level, leading to an infinite series of higher-derivative corrections. Finally, we present a ghost-free massive extension of linearized double field theory, which employs a novel mass term for the dilaton and metric.
Contents 1Introduction1 2Full quadratic theory and non-derivative terms4 2.1Full quadratic Lagrangian. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .5 2.2Full non-derivative Lagrangian and vacua. . . . . . . . . . . . . . . . . . . . . . . . .6 3Spectrum of the quadratic theory7 3.1Spectrum of the two-derivative quadratic theory. . . . . . . . . . . . . . . . . . . . .8 3.2Spectrum of the full six-derivative quadratic theory . . . . . . . . . . . . . . . . . . . .8 4Massive linearized DFT11 5Tensionless limit and degrees of freedom14 5.1Tensionless limit, enhanced gauge symmetry, and Bianchi identities. . . . . . . . . .14 5.2Higher derivatives that reduce the number of degrees of freedom. . . . . . . . . . . .15 6Eliminating the massive fields17 ADegrees of freedom21 A.1Degrees of freedom of two-derivative HSZ theory. . . . . . . . . . . . . . . . . . . . .22 A.2Degrees of freedom of full quadratic HSZ theory . . . . . . . . . . . . . . . . . . . . . .23 A.3Degrees of freedom of massive DFT . . . . . . . . . . . . . . . . . . . . . . . . . . . . .24 1Introduction Some of the salient characteristics of string theory are the presence of higher-derivativeα′corrections, massive modes of higher spin, and duality invariance, such as T-duality.In this paper we aim to illuminate the interplay between these aspects by analyzing the quadratic approximation to theα′- deformed double field theory (DFT) constructed by Siegel and two of the authors in [1] (generalizing [2–6] and further investigated in [7–15]). This theory, henceforth called HSZ theory, contains higher- derivative corrections and is exactly duality1and gauge invariant and hence well-suited for this purpose. 1In the following we refer to the globalO(d, d,R) invariance emerging upon dimensional reduction on a torus, which is made manifest in DFT, for brevity simply as ‘duality invariance’. 1
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