Abstract
The geometric properties of string worldsheets embedded in a higher-dimensional space-time, and of linearized perturbations above them, have been object of various studies since the seminal observation on the relevance of quantizing string models [1]. In the framework of the AdS/CFT correspondence, a particularly important setting where these analyses have been performed is the non-linear sigma-model on the curved \(AdS_5\times S^5\).
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Notes
- 1.
- 2.
The AdS/CFT correspondence prescribes a conformal compactification of \(AdS_5\times S^5\) and the dual \(\mathbb {R}^{1,3}\) space, as explained in the review [8]. We thank Hagen Münkler for pointing out to us the reference [9] where such construction for \(\mathbb {R}^{p,q}\) is rigorously spelt out.
- 3.
Note that the “shape” of a minimal surface is deeply influenced by the signature of the 10d \(G_{MN}\) and 2d metric \(h_{ij}\). This also implies that a rigorous mathematical treatment of the differential equations (3.10)—e.g. existence and uniqueness theorems of its solutions—is substantially different in a Riemannian or pseudo-Riemannian ambient space. We acknowledge an elucidating discussion with Thomas Klose about this point.
- 4.
If we reintroduce the string tension T / 2 in the Polyakov action, then we need to rescale \(\delta X^M\rightarrow \sqrt{\frac{2}{T}}\delta X^M\) and the effective expansion parameter \(\sqrt{\frac{2}{T}}\zeta ^M\) is small in semiclassical approximation \(T\rightarrow \infty \).
- 5.
This corresponds to the absence of non-trivial Beltrami differentials at genus 0.
- 6.
This follows from the fact that we have just two independent components of the extrinsic curvature (e.g. \(K^M_{11}\) and \(K^M_{12}\)). Alternatively, we can argue this result, in a covariant way, from the following matrix relation \( \mathcal{F}^4=\frac{1}{2}\mathrm {tr}(\mathcal {F}^2) \mathcal{F}^2 \) satisfied by \(\mathcal F\).
- 7.
The matrix elements are labelled by \(\underline{i},\underline{j}=2,\dots 9\) in our index conventions.
- 8.
- 9.
A widely used alternative to (3.78) is the light-cone gauge-fixing \(\Gamma ^+\Psi ^I=0\), where the light-cone might lie entirely in \(S^5\) [27, 28] or being shared between \(AdS_5\) and \(S^5\) [29] (and [30] for further references therein). One of the obvious advantages of the “covariant” gauge-fixing (3.78) is preservation of global bosonic symmetries of the action. A more general choice is \(\Psi _1=k\,\Psi _2\equiv k \, \Psi \) where k is a real parameter whose dependence is expected to cancel in the effective action, see discussion in [31]. Yet another \(\kappa \)-symmetry gauge-fixing, albeit equivalent to (3.78) [3], has been used for studying stringy fluctuations in \(AdS_5\times S^5\) in [32].
- 10.
- 11.
- 12.
At variance with the notation in [6], from \(a^{(F)}_2\) we stripped off a minus sign and the factor of 1 / 2 of the Majorana condition. We also included the integration in the SDW coefficients as it is common in literature.
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Vescovi, E. (2017). Geometric Properties of Semiclassically Quantized Strings. In: Perturbative and Non-perturbative Approaches to String Sigma-Models in AdS/CFT. Springer Theses. Springer, Cham. https://doi.org/10.1007/978-3-319-63420-3_3
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