Abstract
Modern theoretical physics has been written in the language of two major scientific paradigms.
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Notes
- 1.
In principle, one can also consider the instanton angle \(\theta \) which combines with the YM coupling constant into a complex coupling \(\tau =\frac{\theta }{2\pi }+\frac{4\pi i}{g_\mathrm{YM}^2}\). Through the AdS/CFT correspondence (Sect. 1.1), the angle \(\theta \) equals the expectation value of the axion field in the spectrum of the dual Type IIB superstring, e.g. [19].
- 2.
Twist-two (Wilson) operators play an important role in deep inelastic scattering in QCD as much as in \(\mathcal {N}=4\). Their anomalous dimension for large spin is governed by the so-called scaling function of the theory in question, see Sect. 7.1. The maximal transcendentality principle conjectured in [27] states that the \(\mathcal {N}=4\) SYM scaling function has uniform degree of transcendentality \(2l-2\) at loop order l and can be extracted from the QCD expression by removing the terms that are not of maximal transcendentality. A brief account of the subject and references are in [28, 29].
- 3.
- 4.
We will make clear the distinction between the ’t Hooft parameter \(\lambda _\mathrm{YM}\) of \(\mathcal {N}=4\) SYM and the one \(\lambda _\mathrm{ABJM}\) of ABJM when necessary, namely in Chap. 6.
- 5.
- 6.
- 7.
- 8.
Higher point functions decompose into these elementary constituents [9].
- 9.
The integrability of the string in the \(AdS_5\times S^5\) background has been mostly studied in the supercoset description [70] (e.g. in [77]) than in the pure spinor version. Some integrable properties in the former formalism will be discussed to some extent in Sects. 2.1.1, 2.1.2 and 2.1.3, while we refer the reader to a non-exhaustive selection of relevant references in the latter formalism in [78, 79] and in the reviews [80, 81]. Arguments that support the quantum integrability of the pure spinor action were given in [82].
- 10.
This is a function undetermined by the symmetries of the theory, but constrained by physical requirements such as crossing symmetry and unitarity, see [92] for a short review.
- 11.
More references on the subject are below (2.35) in Sect. 2.2.
- 12.
We will test the strong-coupling expansion of the interpolating function in Chap. 6.
- 13.
For a general curved target space, the string equations of motion are nonlinear and the right and left oscillator modes of the string interact with themselves and with each other [155], see also [156] for further issues. As for the quantization of a generic field theory in curved spacetime, a good initial reference is the textbook [157].
- 14.
The string sigma-model of [70] is nonlinear because the curvature of the target space brings field-dependent coefficients of the kinetic terms. Expanding the path-integral around a classical solution generates standard quadratic kinetic terms (and interaction terms) for the fluctuation fields that make the sigma-model tractable.
- 15.
- 16.
- 17.
- 18.
The net contribution comes only from the kinetic operators \(\mathcal {O}_B\) and \(\mathcal {O}_F\) because we suppose that the determinant of the diffeomorphism ghosts cancels the one of the “unphysical” (longitudinal) bosons, see comments below (3.46) and (3.98), and we also ignore the caveats in footnote 15.
- 19.
The three spaces listed here are maximally symmetric because their metrics possess the maximal number \(d(d+1)/2\) of Killing vectors in d dimensions.
- 20.
- 21.
This geometrically manifests as an axial symmetry of the minimal surface (5.25) in Fig. 5.3.
- 22.
- 23.
This is of course just one possible route. It is a well-known result [221] that the logarithm of the determinant is equivalently computed by the on-shell vacuum energy, as obtained by summing over the frequency spectrum of the operator, e.g. [198], under certain assumptions. Alternatively, one can also employ the phaseshift method [222,223,224], see [225] for a recent application. We are grateful to Xinyi Chen-Lin and Daniel Medina Rincón for long discussions about this point.
- 24.
We thank Amit Dekel for informing us about this reference.
- 25.
In the first two-loop calculation of [238] the conformal gauge was used, in which propagators are non-diagonal, implying the evaluation of a larger number of two-loop diagrams.
- 26.
In regularizing our integrals all manipulations of tensor structures in the Feynman integrands are however carried out strictly in two dimensions.
- 27.
In literature scaling function and cusp anomalous dimension are essentially synonyms, as we will explain in Sect. 7.1.
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Vescovi, E. (2017). Introduction. 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_1
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