4,205 research outputs found
Solutions of Word Equations over Partially Commutative Structures
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
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
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 where is the
curvature 2-form and is an invariant scalar
product on the corresponding Lie algebra . The descent for
gives rise to an element of
mixed degree. The 3-form part is the Chern-Simons form. The 2-form
part is known as the Wess-Zumino action in physics. The 1-form
component is related to the canonical central extension of the loop
group .
In this paper, we give a new interpretation of the low degree components
and . 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 . In more
detail, we define a 1-cocycle which maps automorphisms of the free Lie
algebra to one forms. A solution of the Kashiwara-Vergne equation is mapped
to . Furthermore, the component is related to the
associator corresponding to . It is surprising that while and
satisfy the highly non-linear twist and pentagon equations, the elements
and solve the linear descent equation
Lectures on mathematical aspects of (twisted) supersymmetric gauge theories
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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