310 research outputs found

    Exact Half-BPS Flux Solutions in M-theory III: Existence and rigidity of global solutions asymptotic to AdS4 x S7

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    The BPS equations in M-theory for solutions with 16 residual supersymmetries, SO(2,2)×SO(4)×SO(4)SO(2,2)\times SO(4)\times SO(4) symmetry, and AdS4×S7AdS_4 \times S^7 asymptotics, were reduced in [arXiv:0806.0605] to a linear first order partial differential equation on a Riemann surface with boundary, subject to a non-trivial quadratic constraint. In the present paper, suitable regularity and boundary conditions are imposed for the existence of global solutions. We seek regular solutions with multiple distinct asymptotic AdS4×S7AdS_4 \times S^7 regions, but find that, remarkably, such solutions invariably reduce to multiple covers of the M-Janus solution found by the authors in [arXiv:0904.3313], suggesting rigidity of the half-BPS M-Janus solution. In particular, we prove analytically that no other smooth deformations away from the M-Janus solution exist, as such deformations invariably violate the quadratic constraint. These rigidity results are contrasted to the existence of half-BPS solutions with non-trivial 4-form fluxes and charges asymptotic to AdS7×S4AdS_7 \times S^4. The results are related to the possibility of M2-branes to end on M5-branes, but the impossibility of M5-branes to end on M2-branes, and to the non-existence of half-BPS solutions with simultaneous AdS4×S7AdS_4 \times S^7 and AdS7×S4AdS_7 \times S^4 asymptotic regions.Comment: 52 pages, 2 figures, pdf-latex. Minor change

    Screening in (2+1)D pure gauge theory at high temperatures

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    We compute heavy quark potentials in pure gauge SU(3)SU(3) at high temperatures in 2+12+1 dimensions and confront them with expectations emerging from perturbative calculations.Comment: 3 pages, latex, 4 figures, uu, Contribution to LATTICE 9

    Near-Extremal Correlators and Generalized Consistent Truncation for AdS_{4|7}\times S^{7|4}

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    We present conjectures for the space-time form and leading large N dependence of extremal and near-extremal correlation functions in the \N=8 superconformal Yang-Mills theory in d=3 as well as in the (0,2) superconformal theory in d=6, using their gravity duals with M-theory on AdS4ק7AdS_4\times \S^7 and AdS7ק4AdS_7 \times \S^4 respectively. As a key part of the conjectures, we argue that the bulk couplings associated with extremal and near-extremal field configurations in the corresponding AdS4AdS_4 and AdS7AdS_7 gauged supergravities vanish. The vanishing of these couplings constitutes a generalization of the property of consistent truncation of the Kaluza-Klein modes.Comment: 22 pages, 2 figure

    Nonperturbative Matching for Field Theories with Heavy Fermions

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    We examine a paradox, suggested by Banks and Dabholkar, concerning nonperturbative effects in an effective field theory which is obtained by integrating out a generation of heavy fermions, where the heavy fermion masses arise from Yukawa couplings. They argue that light fermions in the effective theory appear to decay via instanton processes, whereas their decay is forbidden in the full theory. We resolve this paradox by showing that such processes in fact do not occur in the effective theory, due to matching corrections which cause the relevant light field configurations to have infinite action.Comment: 10 pages, no figures, uses harvmac, Harvard University Preprint HUTP-93/A03

    Gravity duals of half-BPS Wilson loops

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    We explicitly construct the fully back-reacted half-BPS solutions in Type IIB supergravity which are dual to Wilson loops with 16 supersymmetries in N=4\mathcal{N}=4 super Yang-Mills. In a first part, we use the methods of a companion paper to derive the exact general solution of the half-BPS equations on the space AdS2×S2×S4×ΣAdS_2 \times S^2 \times S^4 \times \Sigma, with isometry group SO(2,1)×SO(3)×SO(5)SO(2,1)\times SO(3) \times SO(5) in terms of two locally harmonic functions on a Riemann surface Σ\Sigma with boundary. These solutions, generally, have varying dilaton and axion, and non-vanishing 3-form fluxes. In a second part, we impose regularity and topology conditions. These non-singular solutions may be parametrized by a genus g≥0g \geq 0 hyperelliptic surface Σ\Sigma, all of whose branch points lie on the real line. Each genus gg solution has only a single asymptotic AdS5×S5AdS_5 \times S^5 region, but exhibits gg homology 3-spheres, and an extra gg homology 5-spheres, carrying respectively RR 3-form and RR 5-form charges. For genus 0, we recover AdS5×S5AdS_5 \times S^5 with 3 free parameters, while for genus g≥1g \geq 1, the solution has 2g+52g+5 free parameters. The genus 1 case is studied in detail. Numerical analysis is used to show that the solutions are regular throughout the g=1g=1 parameter space. Collapse of a branch cut on Σ\Sigma subtending either a homology 3-sphere or a homology 5-sphere is non-singular and yields the genus g−1g-1 solution. This behavior is precisely expected of a proper dual to a Wilson loop in gauge theory.Comment: 62 pages, LaTeX, 6 figures, v2: minor change

    Dispersion Relations in String Theory

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    We analyze the analytic continuation of the formally divergent one-loop amplitude for scattering of the graviton multiplet in the Type II Superstring. In particular we obtain explicit double and single dispersion relations, formulas for all the successive branch cuts extending out to plus infinity, as well as for the decay rate of a massive string state of arbitrary mass 2N into two string states of lower mass. We compare our results with the box diagram in a superposition of Ï•3\phi^3-like field theories. The stringy effects are traced to a convergence problem in this superposition.Comment: 17 pages, COLUMBIA-YITP-UCLA/93/TEP/45 (figures fixed up

    An Example of Poincare Symmetry with a Central Charge

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    We discuss a simple system which has a central charge in its Poincare algebra. We show that this system is exactly solvable after quantization and that the algebra holds without anomalies.Comment: 11 pages, Revte
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