Abstract

The O(D,D) covariant generalized metric, postulated as a truly fundamental variable, can describe novel geometries where the notion of Riemannian metric ceases to exist. Here we quantize a closed string upon such backgrounds and identify flat, anomaly free, non-Riemannian string vacua in the familiar critical dimension, D=26 (or D=10). Remarkably, the whole Becchi-Rouet-Stora-Tyutin closed string spectrum is restricted to just one level with no tachyon, and matches the linearized equations of motion of double field theory. Taken as an internal space, our non-Riemannian vacua may open up novel avenues alternative to traditional string compactification.

Highlights

  • We quantize a closed string upon such backgrounds and identify flat, anomaly free, non-Riemannian string vacua in the familiar critical dimension, D 1⁄4 26

  • The whole Becchi-Rouet-Stora-Tyutin closed string spectrum is restricted to just one level with no tachyon, and matches the linearized equations of motion of double field theory

  • The types of ðD; 0Þ or ð0; DÞ are worthy of note. They are uniquely given by HMN 1⁄4 ÆJ MN, and correspond to the most symmetric vacua of double field theory (DFT) with no moduli [24]

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Summary

Here d is the conventional

OðD; DÞ singlet dilaton through eD−2FdT1⁄4diplaffi−tffioffiffigffinffie−re2φla,teadndto the Sð0Þ. Postulating fJ MN; HMN; dg as the only geometric quantities, one can uniquely identify a covariant derivative, ∇M [41,42], and construct the scalar curvature, Sð0Þ, as well as “Einstein” tensor, GMN, which is off-shell conserved, ∇MGMN 1⁄4 0 [43]. This is all analogous to general relativity, though there seems no four-index Riemann tensor [44].

TMN ðJ
The is its inverse satisfying underlying coset is
Vαμ ÞðAβν
Riemannian geometries are consistent superstring vacua in
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