62,339 research outputs found
On two geometric constructions of U(sl_n) and its representations
Ginzburg and Nakajima have given two different geometric constructions of
quotients of the universal enveloping algebra of sl_n and its irreducible
finite-dimensional highest weight representations using the convolution product
in the Borel-Moore homology of flag varieties and quiver varieties
respectively. The purpose of this paper is to explain the precise relationship
between the two constructions. In particular, we show that while the two yield
different quotients of the universal enveloping algebra, they produce the same
representations and the natural bases which arise in both constructions are the
same. We also examine how this relationship can be used to translate the
crystal structure on irreducible components of quiver varieties, defined by
Kashiwara and Saito, to a crystal structure on the varieties appearing in
Ginzburg's construction, thus recovering results of Malkin.Comment: 20 pages, 1 figure; v2: Minor changes to match published versio
The Landau gauge lattice QCD simulation and the gluon propagator
The gluon propagator in the Landau gauge lattice QCD simulation of quenched
8^3 x 16 lattice is measured. The data suggests the confinement mechanism of
the Gribov-Zwanziger theory.Comment: LATTICE98(confine), 3 pages, 3 eps figure
Numerical studies of confinement in the lattice Landau gauge
Critical conjectures on confinement in the Landau gauge is numerically tested
in focus to Gribov copy effects. One of the subjects is of the Kugo-Ojima
confinement criterion and the other is of various viewpoints in the
Gribov-Zwanziger theory. We use the smearing gauge as a reference gauge free of
Gribov copy, and performed three types of simulations, log U, U-linear and log
U in the smearing gauge. It is found that Gribov copy effect on the Kugo-Ojima
parameter is small. log U and U-linear simulations yield only global scale
factor difference in gluon propagator and in ghost propagator, and about 10%
difference in Kugo-Ojima parameter. The horizon function defined by Zwanziger
is evaluated in three types of gauge field and compared. All data show the
negative horizon function as expected.Comment: 4 pages, 2 eps figures, espcrc2.sty included, Lattice 2000
contribution(Confinement and Strings
Existence of random gradient states
We consider two versions of random gradient models. In model A the interface
feels a bulk term of random fields while in model B the disorder enters through
the potential acting on the gradients. It is well known that for gradient
models without disorder there are no Gibbs measures in infinite-volume in
dimension d=2, while there are "gradient Gibbs measures" describing an
infinite-volume distribution for the gradients of the field, as was shown by
Funaki and Spohn. Van Enter and K\"{u}lske proved that adding a disorder term
as in model A prohibits the existence of such gradient Gibbs measures for
general interaction potentials in . In the present paper we prove the
existence of shift-covariant gradient Gibbs measures with a given tilt for model A when and the disorder has mean zero, and for
model B when . When the disorder has nonzero mean in model A, there are
no shift-covariant gradient Gibbs measures for . We also prove similar
results of existence/nonexistence of the surface tension for the two models and
give the characteristic properties of the respective surface tensions.Comment: Published in at http://dx.doi.org/10.1214/11-AAP808 the Annals of
Applied Probability (http://www.imstat.org/aap/) by the Institute of
Mathematical Statistics (http://www.imstat.org
Quiver varieties and fusion products for sl_2
We construct the fusion product of finite-dimensional sl_2-modules in the
homology of (or in the space of constructible functions on) a certain
subvariety L_l(w_1, ..., w_r) of Nakajima's tensor product variety L(w_1,...,
w_r). We also give a combinatorial description of the irreducible components of
this subvariety using the notions of graphical calculus and crossingless
matches for sl_2.Comment: 11 pages, Latex. v2: Some minor typos correcte
Test of the Kugo-Ojima Confinement Criterion in the Lattice Landau Gauge
We present the first results of numerical test of the Kugo-Ojima confinement
criterion in the lattice Landau gauge. The Kugo-Ojima criterion of colour
confinement in the BRS formulation of the continuum gauge theory is given by
, where is defined by the two point function of
the Faddeev-Popov ghost fields and the gauge field . We
measured the lattice version of in use of where
is a lattice covariant derivative in the new definition of the gauge
fields as . We obtained that is consistent with
in SU(3) quenched simulation data of on
and . We report the dependence and finite-size effect of c.Comment: 3 pages Latex, 2 eps figures, Talk given at Lattice99(confine), Pisa,
Ital
A new algorithm of Langevin simulation and its application to the SU(2) and SU(3) lattice gauge
The 2nd order Runge-Kutta scheme Langevin simulation of unquenched QCD in
pseudofermion method derived from our general theory shows a behaviour as a
function of the Langevin step t better than the Fukugita,Oyanagi,Ukawa's
scheme.Comment: Talk given at the ``XVth International Symposium on Lattice Field
Theory'', Edinburgh (UK), July 22nd-26th 1997 (LATTICE 97); 3 pages, LaTeX
file, one Latex picture, uses espcrc2.st
Dual F-signature of special Cohen-Macaulay modules over cyclic quotient surface singularities
The notion of -signature is defined by C. Huneke and G. Leuschke and this
numerical invariant characterizes some singularities. This notion is extended
to finitely generated modules and called dual -signature. In this paper, we
determine the dual -signature of a certain class of Cohen-Macaulay modules
(so-called "special") over cyclic quotient surface singularities. Also, we
compare the dual -signature of a special Cohen-Macaulay module with that of
its Auslander-Reiten translation. This gives a new characterization of the
Gorensteiness.Comment: 14 pages, to appear in J. Commut. Algebra, v3: improved proofs of
theorems, v2: minor change
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