447 research outputs found

    Gear and behaviour committee 1971

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    Supermembrane dynamics from multiple interacting strings

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    The supermembrane theory on R10xS1R^{10}x S^1 is investigated, for membranes that wrap once around the compact dimension. The Hamiltonian can be organized as describing NsN_s interacting strings, the exact supermembrane corresponding to Ns→∞N_s\to \infty. The zero-mode part of Ns−1N_s-1 strings turn out to be precisely the modes which are responsible of instabilities. For sufficiently large compactification radius R0R_0, interactions are negligible and the lowest-energy excitations are described by a set of harmonic oscillators. We compute the physical spectrum to leading order, which becomes exact in the limit g2→∞ g^2 \to \infty , where g2≡4π2T3R03g^2\equiv 4\pi^2 T_3 R_0^3 and T3T_3 is the membrane tension. As the radius is decreased, more strings become strongly interacting and their oscillation modes get frozen. In the zero-radius limit, the spectrum is constituted of the type IIA superstring spectrum, plus an infinite number of extra states associated with flat directions of the quartic potential.Comment: Small corrections. 21 page

    Stability of the quantum supermembrane in a manifold with boundary

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    We point out an effect which may stabilize a supersymmetric membrane moving on a manifold with boundary, and lead to a light-cone Hamiltonian with a discrete spectrum of eigenvalues. The analysis is carried out explicitly for a closed supermembrane in the regularized SU(N)SU(N) matrix model version.Comment: 10 pages, harvmac (references added, minor changes

    T-duality in M-theory and supermembranes

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    The (q_1,q_2) SL(2,Z) string bound states of type IIB superstring theory admit two inequivalent (T-dual) representations in eleven dimensions in terms of a fundamental 2-brane. In both cases, the spectrum of membrane oscillations can be determined exactly in the limit g2→∞g^2\to \infty , where g2g^2 is the type IIA string coupling. We find that the BPS mass formulas agree, and reproduce the BPS mass spectrum of the (q1,q2)(q_1,q_2) string bound state. In the non-BPS sector, the respective mass formulas apply in different corners of the moduli space. The axiomatic requirement of T-duality in M-theory permits to derive a discrete mass spectrum in a (thin torus) region where standard supermembrane theory undergoes instabilities.Comment: harvmac, 9 page
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