1,695 research outputs found
Harish-Chandra integrals as nilpotent integrals
Recently the correlation functions of the so-called
Itzykson-Zuber/Harish-Chandra integrals were computed (by one of the authors
and collaborators) for all classical groups using an integration formula that
relates integrals over compact groups with respect to the Haar measure and
Gaussian integrals over a maximal nilpotent Lie subalgebra of their
complexification. Since the integration formula a posteriori had the same form
for the classical series, a conjecture was formulated that such a formula
should hold for arbitrary semisimple Lie groups. We prove this conjecture using
an abstract Lie-theoretic approach.Comment: 10 page
Universality in the profile of the semiclassical limit solutions to the focusing Nonlinear Schroedinger equation at the first breaking curve
We consider the semiclassical (zero-dispersion) limit of the one-dimensional
focusing Nonlinear Schroedinger equation (NLS) with decaying potentials. If a
potential is a simple rapidly oscillating wave (the period has the order of the
semiclassical parameter epsilon) with modulated amplitude and phase, the
space-time plane subdivides into regions of qualitatively different behavior,
with the boundary between them consisting typically of collection of piecewise
smooth arcs (breaking curve(s)). In the first region the evolution of the
potential is ruled by modulation equations (Whitham equations), but for every
value of the space variable x there is a moment of transition (breaking), where
the solution develops fast, quasi-periodic behavior, i.e., the amplitude
becomes also fastly oscillating at scales of order epsilon. The very first
point of such transition is called the point of gradient catastrophe. We study
the detailed asymptotic behavior of the left and right edges of the interface
between these two regions at any time after the gradient catastrophe. The main
finding is that the first oscillations in the amplitude are of nonzero
asymptotic size even as epsilon tends to zero, and they display two separate
natural scales; of order epsilon in the parallel direction to the breaking
curve in the (x,t)-plane, and of order epsilon ln(epsilon) in a transversal
direction. The study is based upon the inverse-scattering method and the
nonlinear steepest descent method.Comment: 40 pages, 10 figure
The PDEs of biorthogonal polynomials arising in the two-matrix model
The two-matrix model can be solved by introducing bi-orthogonal polynomials.
In the case the potentials in the measure are polynomials, finite sequences of
bi-orthogonal polynomials (called
"windows") satisfy polynomial ODEs as well as deformation equations (PDEs)
and finite difference equations (Delta-E) which are all Frobenius compatible
and define discrete and continuous isomonodromic deformations for the irregular
ODE, as shown in previous works of ours.
In the one matrix model an explicit and concise expression for the
coefficients of these systems is known and it allows to relate the partition
function with the isomonodromic tau-function of the overdetermined system.
Here, we provide the generalization of those expressions to the case of
bi-orthogonal polynomials, which enables us to compute the determinant of the
fundamental solution of the overdetermined system of ODE+PDEs+Delta-E.Comment: 20 pages v1 18 Nov 2003; v2 9 Jan 2004: trivial Latex mistake
correcte
On the location of poles for the Ablowitz-Segur family of solutions to the second Painlev\'e equation
Using a simple operator-norm estimate we show that the solution to the second
Painlev\'e equation within the Ablowitz-Segur family is pole-free in a well
defined region of the complex plane of the independent variable. The result is
illustrated with several numerical examples.Comment: 8 pages, to appear in Nonlinearit
Mixed Correlation Functions of the Two-Matrix Model
We compute the correlation functions mixing the powers of two non-commuting
random matrices within the same trace. The angular part of the integration was
partially known in the literature: we pursue the calculation and carry out the
eigenvalue integration reducing the problem to the construction of the
associated biorthogonal polynomials. The generating function of these
correlations becomes then a determinant involving the recursion coefficients of
the biorthogonal polynomials.Comment: 16 page
Moment determinants as isomonodromic tau functions
We consider a wide class of determinants whose entries are moments of the
so-called semiclassical functionals and we show that they are tau functions for
an appropriate isomonodromic family which depends on the parameters of the
symbols for the functionals. This shows that the vanishing of the tau-function
for those systems is the obstruction to the solvability of a Riemann-Hilbert
problem associated to certain classes of (multiple) orthogonal polynomials. The
determinants include Haenkel, Toeplitz and shifted-Toeplitz determinants as
well as determinants of bimoment functionals and the determinants arising in
the study of multiple orthogonality. Some of these determinants appear also as
partition functions of random matrix models, including an instance of a
two-matrix model.Comment: 24 page
The Cauchy two-matrix model
We introduce a new class of two(multi)-matrix models of positive Hermitean
matrices coupled in a chain; the coupling is related to the Cauchy kernel and
differs from the exponential coupling more commonly used in similar models. The
correlation functions are expressed entirely in terms of certain biorthogonal
polynomials and solutions of appropriate Riemann-Hilbert problems, thus paving
the way to a steepest descent analysis and universality results. The
interpretation of the formal expansion of the partition function in terms of
multicolored ribbon-graphs is provided and a connection to the O(1) model. A
steepest descent analysis of the partition function reveals that the model is
related to a trigonal curve (three-sheeted covering of the plane) much in the
same way as the Hermitean matrix model is related to a hyperelliptic curve.Comment: 34 pages, 2 figures. V2: changes only to metadat
The Orthogonal Gaseous Kinematical Decoupling in the Sa Spiral NGC 2855
We present major and minor-axis kinematics of stars and ionized gas as well
as narrow and broad-band surface photometry of the Sa spiral NGC 2855. In the
nuclear regions of this unbarred and apparently undisturbed spiral galaxy the
gas is rotating perpendicularly to the galaxy disk. We suggest that this
kinematically-decoupled component is the signature of an acquisition process in
the history of this galaxy.Comment: 7 pages, 4 PostScript figures. Accepted for pubblication in A&A.
Figs. 1 and 3 at lower resolution. Data tables will be available at CD
Second and Third Order Observables of the Two-Matrix Model
In this paper we complement our recent result on the explicit formula for the
planar limit of the free energy of the two-matrix model by computing the second
and third order observables of the model in terms of canonical structures of
the underlying genus g spectral curve. In particular we provide explicit
formulas for any three-loop correlator of the model. Some explicit examples are
worked out.Comment: 22 pages, v2 with added references and minor correction
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