1,295 research outputs found
Symplectic Geometry of Supersymmetry and Nonlinear Sigma Model
Recently it has been argued, that Poincar\'{e} supersymmetric field theories
admit an underlying loop space hamiltonian (symplectic) structure. Here shall
establish this at the level of a general supermultiplet. In particular,
we advocate the use of a superloop space and explain the necessity of using
nonconventional auxiliary fields. As an example we consider the nonlinear
-model. Due to the quartic fermionic term, we conclude that the use of
superloop space variables is necessary for the action to have a hamiltonian
loop space interpretation.Comment: 9 pages, UU-ITP 30/9
Competition in European Telecom Markets
In recent years, the European telecommunications market has witnessed major developments, with rapid expansion in access to telecommunications networks and a surge in the number of available services and applications. While many factors have contributed to the transformation of the telecommunications industry, competition has played a key role in driving telecom players to invest in new technologies, to innovate and to offer new services. Increased competitive pressure is being felt across all market segments, even though significant differences remain across services and countries. Broadband roll-out has allowed operators to offer multiple-play services, thereby transforming traditional segment boundaries and competitive market structures.competition; access; convergence; multiple-play; fixed telephony; mobile services; broadband; VoIP; MVNO
The B model as a twisted spinning particle
The B-twisted topological sigma model coupled to topological gravity is
supposed to be described by an ordinary field theory: a type of holomorphic
Chern-Simons theory for the open string, and the Kodaira-Spencer theory for the
closed string. We show that the B model can be represented as a PARTICLE
theory, obtained by reducing the sigma model to one dimension, and replacing
the coupling to topological gravity by a coupling to a twisted one-dimensional
supergravity. The particle can be defined on ANY Kahler manifold--it does not
require the Calabi-Yau condition--so it may provide a more generalized setting
for the B model than the topological sigma model. The one-loop partition
function of the particle can be written in terms of the Ray-Singer torsion of
the manifold, and agrees with that of the original B model. After showing how
to deform the Kahler and complex structures in the particle, we prove the
independence of this partition function on the Kahler structure, and
investigate the origin of the holomorphic anomaly. To define other amplitudes,
one needs to introduce interactions into the particle. The particle will then
define a field theory, which may or may not be the Chern-Simons or
Kodaira-Spencer theories.Comment: 25/17 Pages big/little (LaTeX), TAUP-2192-94, CERN-TH.7402/9
Determinant bundles, boundaries, and surgery
In this note we specialize and illustrate the ideas developed in the paper
math.DG/0201112 of the first author ("Index theory, eta forms, and Deligne
cohomology ") in the case of the determinant line bundle. We discuss the
surgery formula in the adiabatic limit using the adiabatic decomposition
formula of the zeta regularized determinant of the Dirac Laplacian obtained by
the second author and K. Wojciechowski.Comment: 23 page
Cohomological Partition Functions for a Class of Bosonic Theories
We argue, that for a general class of nontrivial bosonic theories the path
integral can be related to an equivariant generalization of conventional
characteristic classes.Comment: 9 pages; standard LATEX fil
Equivariant Kaehler Geometry and Localization in the G/G Model
We analyze in detail the equivariant supersymmetry of the model. In
spite of the fact that this supersymmetry does not model the infinitesimal
action of the group of gauge transformations, localization can be established
by standard arguments. The theory localizes onto reducible connections and a
careful evaluation of the fixed point contributions leads to an alternative
derivation of the Verlinde formula for the WZW model. We show that the
supersymmetry of the model can be regarded as an infinite dimensional
realization of Bismut's theory of equivariant Bott-Chern currents on K\"ahler
manifolds, thus providing a convenient cohomological setting for understanding
the Verlinde formula. We also show that the supersymmetry is related to a
non-linear generalization (q-deformation) of the ordinary moment map of
symplectic geometry in which a representation of the Lie algebra of a group
is replaced by a representation of its group algebra with commutator . In the large limit it reduces to the ordinary moment map of
two-dimensional gauge theories.Comment: LaTex file, 40 A4 pages, IC/94/108 and ENSLAPP-L-469/9
A new short proof of the local index formula and some of its applications
We give a new short proof of the index formula of Atiyah and Singer based on
combining Getzler's rescaling with Greiner's approach of the heat kernel
asymptotics. As application we can easily compute the Connes-Moscovici cyclic
cocycle of even and odd Dirac spectral triples, and then recover the
Atiyah-Singer index formula (even case) and the Atiyah-Patodi-Singer spectral
flow formula (odd case).Comment: v5: more typos fixed; 19 page
Abelian Yang-Mills theory on Real tori and Theta divisors of Klein surfaces
The purpose of this paper is to compute determinant index bundles of certain
families of Real Dirac type operators on Klein surfaces as elements in the
corresponding Grothendieck group of Real line bundles in the sense of Atiyah.
On a Klein surface these determinant index bundles have a natural holomorphic
description as theta line bundles. In particular we compute the first
Stiefel-Whitney classes of the corresponding fixed point bundles on the real
part of the Picard torus. The computation of these classes is important,
because they control to a large extent the orientability of certain moduli
spaces in Real gauge theory and Real algebraic geometry.Comment: LaTeX, 44 pages, to appear in Comm. Math. Phy
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