4,205 research outputs found

    Solutions of Word Equations over Partially Commutative Structures

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    We give NSPACE(n log n) algorithms solving the following decision problems. Satisfiability: Is the given equation over a free partially commutative monoid with involution (resp. a free partially commutative group) solvable? Finiteness: Are there only finitely many solutions of such an equation? PSPACE algorithms with worse complexities for the first problem are known, but so far, a PSPACE algorithm for the second problem was out of reach. Our results are much stronger: Given such an equation, its solutions form an EDT0L language effectively representable in NSPACE(n log n). In particular, we give an effective description of the set of all solutions for equations with constraints in free partially commutative monoids and groups

    Cumulants, free cumulants and half-shuffles

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    Free cumulants were introduced as the proper analog of classical cumulants in the theory of free probability. There is a mix of similarities and differences, when one considers the two families of cumulants. Whereas the combinatorics of classical cumulants is well expressed in terms of set partitions, the one of free cumulants is described, and often introduced in terms of non-crossing set partitions. The formal series approach to classical and free cumulants also largely differ. It is the purpose of the present article to put forward a different approach to these phenomena. Namely, we show that cumulants, whether classical or free, can be understood in terms of the algebra and combinatorics underlying commutative as well as non-commutative (half-)shuffles and (half-)unshuffles. As a corollary, cumulants and free cumulants can be characterized through linear fixed point equations. We study the exponential solutions of these linear fixed point equations, which display well the commutative, respectively non-commutative, character of classical, respectively free, cumulants.Comment: updated and revised version; accepted for publication in PRS

    Chern-Simons, Wess-Zumino and other cocycles from Kashiwara-Vergne and associators

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    Descent equations play an important role in the theory of characteristic classes and find applications in theoretical physics, e.g. in the Chern-Simons field theory and in the theory of anomalies. The second Chern class (the first Pontrjagin class) is defined as p=⟨F,F⟩p= \langle F, F\rangle where FF is the curvature 2-form and ⟨⋅,⋅⟩\langle \cdot, \cdot\rangle is an invariant scalar product on the corresponding Lie algebra g\mathfrak{g}. The descent for pp gives rise to an element ω=ω3+ω2+ω1+ω0\omega=\omega_3 + \omega_2 + \omega_1 + \omega_0 of mixed degree. The 3-form part ω3\omega_3 is the Chern-Simons form. The 2-form part ω2\omega_2 is known as the Wess-Zumino action in physics. The 1-form component ω1\omega_1 is related to the canonical central extension of the loop group LGLG. In this paper, we give a new interpretation of the low degree components ω1\omega_1 and ω0\omega_0. Our main tool is the universal differential calculus on free Lie algebras due to Kontsevich. We establish a correspondence between solutions of the first Kashiwara-Vergne equation in Lie theory and universal solutions of the descent equation for the second Chern class pp. In more detail, we define a 1-cocycle CC which maps automorphisms of the free Lie algebra to one forms. A solution of the Kashiwara-Vergne equation FF is mapped to ω1=C(F)\omega_1=C(F). Furthermore, the component ω0\omega_0 is related to the associator corresponding to FF. It is surprising that while FF and Φ\Phi satisfy the highly non-linear twist and pentagon equations, the elements ω1\omega_1 and ω0\omega_0 solve the linear descent equation

    Lectures on mathematical aspects of (twisted) supersymmetric gauge theories

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    Supersymmetric gauge theories have played a central role in applications of quantum field theory to mathematics. Topologically twisted supersymmetric gauge theories often admit a rigorous mathematical description: for example, the Donaldson invariants of a 4-manifold can be interpreted as the correlation functions of a topologically twisted N=2 gauge theory. The aim of these lectures is to describe a mathematical formulation of partially-twisted supersymmetric gauge theories (in perturbation theory). These partially twisted theories are intermediate in complexity between the physical theory and the topologically twisted theories. Moreover, we will sketch how the operators of such a theory form a two complex dimensional analog of a vertex algebra. Finally, we will consider a deformation of the N=1 theory and discuss its relation to the Yangian, as explained in arXiv:1308.0370 and arXiv:1303.2632.Comment: Notes from a lecture series by the first author at the Les Houches Winter School on Mathematical Physics in 2012. To appear in the proceedings of this conference. Related to papers arXiv:1308.0370, arXiv:1303.2632, and arXiv:1111.423
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