2,472 research outputs found

    Radial coordinates for defect CFTs

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    We study the two-point function of local operators in the presence of a defect in a generic conformal field theory. We define two pairs of cross ratios, which are convenient in the analysis of the OPE in the bulk and defect channel respectively. The new coordinates have a simple geometric interpretation, which can be exploited to efficiently compute conformal blocks in a power expansion. We illustrate this fact in the case of scalar external operators. We also elucidate the convergence properties of the bulk and defect OPE decompositions of the two-point function. In particular, we remark that the expansion of the two-point function in powers of the new cross ratios converges everywhere, a property not shared by the cross ratios customarily used in defect CFT. We comment on the crucial relevance of this fact for the numerical bootstrap.Comment: Matches journal version; the attached mathematica file (Bulk CB.nb + rec.txt) computes the conformal blocks in the bulk channe

    Random Field Ising Model and Parisi-Sourlas Supersymmetry I. Supersymmetric CFT

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    Quenched disorder is very important but notoriously hard. In 1979, Parisi and Sourlas proposed an interesting and powerful conjecture about the infrared fixed points with random field type of disorder: such fixed points should possess an unusual supersymmetry, by which they reduce in two less spatial dimensions to usual non-supersymmetric non-disordered fixed points. This conjecture however is known to fail in some simple cases, but there is no consensus on why this happens. In this paper we give new non-perturbative arguments for dimensional reduction. We recast the problem in the language of Conformal Field Theory (CFT). We then exhibit a map of operators and correlation functions from Parisi-Sourlas supersymmetric CFT in dd dimensions to a (d2)(d-2)-dimensional ordinary CFT. The reduced theory is local, i.e. it has a local conserved stress tensor operator. As required by reduction, we show a perfect match between superconformal blocks and the usual conformal blocks in two dimensions lower. This also leads to a new relation between conformal blocks across dimensions. This paper concerns the second half of the Parisi-Sourlas conjecture, while the first half (existence of a supersymmetric fixed point) will be examined in a companion work.Comment: 36 pages, 2 figures. Minor corrections, new references, some comments and clarifications in section 4, a new appendix on "Supersymmetry in the problem of critical dynamics" are added. To appear in JHE

    Recursion Relations for Conformal Blocks

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    In the context of conformal field theories in general space-time dimension, we find all the possible singularities of the conformal blocks as functions of the scaling dimension Δ\Delta of the exchanged operator. In particular, we argue, using representation theory of parabolic Verma modules, that in odd spacetime dimension the singularities are only simple poles. We discuss how to use this information to write recursion relations that determine the conformal blocks. We first recover the recursion relation introduced in 1307.6856 for conformal blocks of external scalar operators. We then generalize this recursion relation for the conformal blocks associated to the four point function of three scalar and one vector operator. Finally we specialize to the case in which the vector operator is a conserved current.Comment: 55 pages, 12 figures; v2 Typos corrected, conclusions changed, reference adde

    Projectors and seed conformal blocks for traceless mixed-symmetry tensors

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    In this paper we derive the projectors to all irreducible SO(d) representations (traceless mixed-symmetry tensors) that appear in the partial wave decomposition of a conformal correlator of four stress-tensors in d dimensions. These projectors are given in a closed form for arbitrary length l1l_1 of the first row of the Young diagram. The appearance of Gegenbauer polynomials leads directly to recursion relations in l1l_1 for seed conformal blocks. Further results include a differential operator that generates the projectors to traceless mixed-symmetry tensors and the general normalization constant of the shadow operator.Comment: 49 pages, 1 Mathematica notebook, many figures, v2: add reference

    Radial expansion for spinning conformal blocks

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    This paper develops a method to compute any bosonic conformal block as a series expansion in the optimal radial coordinate introduced by Hogervorst and Rychkov. The method reduces to the known result when the external operators are all the same scalar operator, but it allows to compute conformal blocks for external operators with spin. Moreover, we explain how to write closed form recursion relations for the coefficients of the expansions. We study three examples of four point functions in detail: one vector and three scalars; two vectors and two scalars; two spin 2 tensors and two scalars. Finally, for the case of two external vectors, we also provide a more efficient way to generate the series expansion using the analytic structure of the blocks as a function of the scaling dimension of the exchanged operator.Comment: 42 pages, 17 figures, 7 Mathematica files, v2: minor changes in the text, typos correcte

    The Parisi-Sourlas Uplift and Infinitely Many Solvable 4d CFTs

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    Parisi-Sourlas (PS) supersymmetry is known to emerge in some models with random field type of disorder. When PS SUSY is present the dd-dimensional theory allows for a d2d-2-dimensional description. In this paper we investigate the reversed question and we provide new indications that any given CFTd2_{d-2} can be uplifted to a PS SUSY CFTd_{d}. We show that any scalar four-point function of a CFTd2_{d-2} is mapped to a set of 43 four-point functions of the uplifted CFTd_{d} which are related to each other by SUSY and satisfy all necessary bootstrap axioms. As a byproduct we find 43 non trivial relations between conformal blocks across dimensions. We test the uplift in generalized free field theory (GFF) and find that PS SUSY is a powerful tool to bootstrap an infinite class of previously unknown GFF observables. Some of this power is shown to persist in perturbation theory around GFF. We explain why all diagonal minimal models admit an uplift and we show exact results for correlators and CFT data of the 4d4d uplift of the Ising model. Despite being strongly coupled 4d4d CFTs, the uplifted minimal models contain infinitely many conserved currents and are expected to be integrable.Comment: 50 pages + 15 pages of appendices, 3 figures, Mathematica notebook in the ancillary file

    Random Field Ising Model and Parisi-Sourlas Supersymmetry II. Renormalization Group

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    We revisit perturbative RG analysis in the replicated Landau-Ginzburg description of the Random Field Ising Model near the upper critical dimension 6. Working in a field basis with manifest vicinity to a weakly-coupled Parisi-Sourlas supersymmetric fixed point (Cardy, 1985), we look for interactions which may destabilize the SUSY RG flow and lead to the loss of dimensional reduction. This problem is reduced to studying the anomalous dimensions of "leaders" -- lowest dimension parts of SnS_n-invariant perturbations in the Cardy basis. Leader operators are classified as non-susy-writable, susy-writable or susy-null depending on their symmetry. Susy-writable leaders are additionally classified as belonging to superprimary multiplets transforming in particular OSp(d2)\textrm{OSp}(d | 2) representations. We enumerate all leaders up to 6d dimension Δ=12\Delta = 12, and compute their perturbative anomalous dimensions (up to two loops). We thus identify two perturbations (with susy-null and non-susy-writable leaders) becoming relevant below a critical dimension dc4.2d_c \approx 4.2 - 4.74.7. This supports the scenario that the SUSY fixed point exists for all 3<d63 < d \leq 6, but becomes unstable for d<dcd < d_c.Comment: 103 pages, 15 figures. v2: susy-null leader discussion modified (Sec. 8.5 and App. A.6), and other tweaks. v3: version accepted by JHEP, added executive summary in Sec. 1.1, discussion in Sec 11.1.1 and Sec. 11.2.1, corrected typos. Conclusions unchange
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