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Perturbative RG flows in AdS: an \'etude

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arxiv 2309.10031 v3 pith:W5CHWZYV submitted 2023-09-18 hep-th cond-mat.str-el

classification hep-thcond-mat.str-el
keywords boundarygeneralflowsbcftscorrelationdiscussflat-spaceflow
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

We discuss general properties of perturbative RG flows in AdS with a focus on the treatment of boundary conditions and infrared divergences. In contrast with flat-space boundary QFT, general covariance in AdS implies the absence of independent boundary flows. We illustrate how boundary correlation functions remain conformally covariant even if the bulk QFT has a scale. We apply our general discussion to the RG flow between consecutive unitary diagonal minimal models which is triggered by the $\phi_{(1,3)}$ operator. For these theories we conjecture a flow diagram whose form is significantly simpler than that in flat-space boundary QFT. In several stand-alone appendices we discuss two-dimensional BCFTs in general and the minimal model BCFTs in particular. These include both an extensive review as well as the computation of several new BCFT correlation functions.

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Cited by 4 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. QFT as a set of ODEs: higher dimensions

    hep-th 2026-06 unverdicted novelty 7.0 of 10

    The authors generalize the AdS₂ flow equations for QFT data to AdS₃ and AdS₄, add crossing-based closure and Padé-accelerated sums, and verify them in free theories.

  2. $\mathcal{N}=2$ Super Yang-Mills in AdS$_4$ and $F_{\text{AdS}}$-maximization

    hep-th 2025-06 conditional novelty 7.0 of 10

    A new maximization principle, F_AdS-maximization, selects boundary conditions for N=2 SYM in AdS4 and predicts a transition to a U(1)-Higgsed phase at strong coupling.

  3. Conformal QED in AdS as a BCFT

    hep-th 2026-07 conditional novelty 6.0 of 10

    In conformal QED on AdS_d, the Dirichlet boundary condition's second lightest scalar becomes marginal for 3<d<4, indicating the Dirichlet BCFT is unstable at d=3, whereas the Neumann BCFT remains stable.

  4. Neumann scalars in AdS: partition functions and phases

    hep-th 2026-07 conditional novelty 6.0 of 10

    Neumann scalars in AdS admit one-loop partition functions obtained by contour deformation from the Dirichlet result; the stricter unitarity bound then yields qualitatively different phase diagrams that are corroborate...

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