5,359 research outputs found

    Duality for Legendrian contact homology

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    The main result of this paper is that, off of a `fundamental class' in degree 1, the linearized Legendrian contact homology obeys a version of Poincare duality between homology groups in degrees k and -k. Not only does the result itself simplify calculations, but its proof also establishes a framework for analyzing cohomology operations on the linearized Legendrian contact homology.Comment: This is the version published by Geometry & Topology on 8 December 200

    Duality between Lagrangian and Legendrian invariants

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    Consider a pair (X,L)(X,L), of a Weinstein manifold XX with an exact Lagrangian submanifold LL, with ideal contact boundary (Y,Ξ›)(Y,\Lambda), where YY is a contact manifold and Ξ›βŠ‚Y\Lambda\subset Y is a Legendrian submanifold. We introduce the Chekanov-Eliashberg DG-algebra, CEβˆ—(Ξ›)CE^{\ast}(\Lambda), with coefficients in chains of the based loop space of Ξ›\Lambda and study its relation to the Floer cohomology CFβˆ—(L)CF^{\ast}(L) of LL. Using the augmentation induced by LL, CEβˆ—(Ξ›)CE^{\ast}(\Lambda) can be expressed as the Adams cobar construction Ξ©\Omega applied to a Legendrian coalgebra, LCβˆ—(Ξ›)LC_{\ast}(\Lambda). We define a twisting cochain:t ⁣:LCβˆ—(Ξ›)β†’B(CFβˆ—(L))#\mathfrak{t} \colon LC_{\ast}(\Lambda) \to \mathrm{B} (CF^*(L))^\#via holomorphic curve counts, where B\mathrm{B} denotes the bar construction and #\# the graded linear dual. We show under simply-connectedness assumptions that the corresponding Koszul complex is acyclic which then implies that CEβˆ—(Ξ›)CE^*(\Lambda) and CFβˆ—(L)CF^{\ast}(L) are Koszul dual. In particular, t\mathfrak{t} induces a quasi-isomorphism between CEβˆ—(Ξ›)CE^*(\Lambda) and the cobar of the Floer homology of LL, Ξ©CFβˆ—(L)\Omega CF_*(L). We use the duality result to show that under certain connectivity and locally finiteness assumptions, CEβˆ—(Ξ›)CE^*(\Lambda) is quasi-isomorphic to Cβˆ’βˆ—(Ξ©L)C_{-*}(\Omega L) for any Lagrangian filling LL of Ξ›\Lambda. Our constructions have interpretations in terms of wrapped Floer cohomology after versions of Lagrangian handle attachments. In particular, we outline a proof that CEβˆ—(Ξ›)CE^{\ast}(\Lambda) is quasi-isomorphic to the wrapped Floer cohomology of a fiber disk CC in the Weinstein domain obtained by attaching Tβˆ—(Λ×[0,∞))T^{\ast}(\Lambda\times[0,\infty)) to XX along Ξ›\Lambda (or, in the terminology of arXiv:1604.02540 the wrapped Floer cohomology of CC in XX with wrapping stopped by Ξ›\Lambda). Along the way, we give a definition of wrapped Floer cohomology without Hamiltonian perturbations.Comment: 126 pages, 20 figures. Substantial overall revision based on referee's comments. The main results remain the same but the exposition has been improve

    Augmented Superfield Approach to Nilpotent Symmetries in the Modified Version of 2D Proca Theory

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    We derive the complete set of off-shell nilpotent and absolutely anticommuting Becchi-Rouet-Stora-Tyutin (BRST), anti-BRST and (anti-)co-BRST symmetry transformations for all the fields of the modified version of two (1+1)-dimensional (2D) Proca theory by exploiting the "augmented" superfield formalism where the (dual-)horizontality conditions and (dual-)gauge-invariant restrictions are exploited together. We capture the (anti-)BRST and (anti-)co-BRST invariance of the Lagrangian density in the language of superfield formalism. We also express the nilpotency and absolute anticommutativity of the (anti-)BRST and (anti-)co-BRST charges within the framework of augmented superfield formalism. This exercise leads to some novel observations which have, hitherto, not been pointed out in the literature within the framework of superfield approach to BRST formalism. For the sake of completeness, we also mention, very briefly, a unique bosonic symmetry, the ghost-scale symmetry and discrete symmetries of the theory and show that the algebra of conserved charges captures the cohomological aspects of differential geometry. Thus, our present modified 2D Proca theory is a model for the Hodge Theory.Comment: LaTeX file, 32 pages, journal reference give

    Lagrange optimality system for a class of nonsmooth convex optimization

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    In this paper, we revisit the augmented Lagrangian method for a class of nonsmooth convex optimization. We present the Lagrange optimality system of the augmented Lagrangian associated with the problems, and establish its connections with the standard optimality condition and the saddle point condition of the augmented Lagrangian, which provides a powerful tool for developing numerical algorithms. We apply a linear Newton method to the Lagrange optimality system to obtain a novel algorithm applicable to a variety of nonsmooth convex optimization problems arising in practical applications. Under suitable conditions, we prove the nonsingularity of the Newton system and the local convergence of the algorithm.Comment: 19 page

    On barrier and modified barrier multigrid methods for 3d topology optimization

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    One of the challenges encountered in optimization of mechanical structures, in particular in what is known as topology optimization, is the size of the problems, which can easily involve millions of variables. A basic example is the minimum compliance formulation of the variable thickness sheet (VTS) problem, which is equivalent to a convex problem. We propose to solve the VTS problem by the Penalty-Barrier Multiplier (PBM) method, introduced by R.\ Polyak and later studied by Ben-Tal and Zibulevsky and others. The most computationally expensive part of the algorithm is the solution of linear systems arising from the Newton method used to minimize a generalized augmented Lagrangian. We use a special structure of the Hessian of this Lagrangian to reduce the size of the linear system and to convert it to a form suitable for a standard multigrid method. This converted system is solved approximately by a multigrid preconditioned MINRES method. The proposed PBM algorithm is compared with the optimality criteria (OC) method and an interior point (IP) method, both using a similar iterative solver setup. We apply all three methods to different loading scenarios. In our experiments, the PBM method clearly outperforms the other methods in terms of computation time required to achieve a certain degree of accuracy
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