1,164 research outputs found
Asymptotically free theories based on discrete subgroups
We study the critical behavior of discrete spin models related to the 2d O(3)
non-linear sigma model. Precise numerical results suggest that models with
sufficiently large discrete subgroups are in the same universality class as the
original sigma model. We observe that at least up to correlation lengths
the cut-off effects follow effectively an
behaviour both in the O(3) and in the dodecahedron model.Comment: 4 pages, 3 figures, Lattice 2000 (Spin Models
The SU(3) deconfining phase transition with Symanzik action
We report on the determination of the deconfining temperature in SU(3) pure
gauge theory, using the Symanzik tree level improved action, on lattices of
size 3 x 12^3, 4 x 16^3, 5 x 20^3, 6 x24^3. We find that the asymptotic scaling
violation pattern is similar to the one observed using the Wilson action. We
conclude that the irrelevant operators do not affect, in the range of couplings
considered, the lattice beta function. An analysis based on an effective
coupling formulation shows an apparent improvement.Comment: 8 pages, report IFUP-TH 12/9
Gauge invariant extremization on the lattice
Recently, a method was proposed and tested to find saddle points of the
action in simulations of non-abelian lattice gauge theory. The idea, called
`extremization', is to minimize \int(\dl S/\dl A_\mu)^2. The method was
implemented in an explicitly gauge variant way, however, and gauge dependence
showed up in the results.
Here we show how extremization can be formulated in a way that preserves
gauge invariance on the lattice. The method applies to any gauge group and any
lattice action. The procedure is worked out in detail for the standard
plaquette action with gauge groups U(1) and SU(N).Comment: 7 pages, LaTeX, Oxford preprint OUTP-92-16
Verification of O(a) improvement
The status of simulations using the non-perturbatively O(a) improved Wilson
action in the quenched approximation is reviewed. The impact of
non-perturbative improvement on the hadronic mass spectrum and the size of
residual lattice artefacts in spectral quantities and decay constants are
assessed.Comment: Plenary talk presented at LATTICE '97, 6 pages, LaTeX, espcrc2.sty, 6
postscript files, to be included with eps
Classical improvement of lattice actions and quantum effects: a unified view
The possibility of removing the one-loop perturbative effects of lattice
artifacts by a proper choice of the lattice action is explored, and found to
depend crucially on the properties of the physical quantity considered. In this
respect the finite-space-volume mass gap m(L) is an improved observable. We
find an explicit momentum space representation of the one-loop contribution to
m(L) for arbitrary lattice actions in the case of two-dimensional O(N) sigma
models. We define a ``tree perfect'' Symanzik action and find that it formally
removes all one-loop lattice artifacts in m(L). On-shell improved actions do
not share this property.Comment: 10 pages, revte
Improved actions of the staggered fermion
We have studied improved lattice QCD with the staggered fermion by
using Symanzik's program. We find that there are 5 dimension-6 fermion
bilinears and gauge operators. In addition, there are 10 four-fermion operators
which are absent at the tree-level and tadpole-improved tree-level.Comment: 3 pages, Latex, talk presented at LATTICE''97(Improvement
Unexpected results in asymptotically free quantum field theories
We study the behavior of asymptotically free (AF) spin and gauge models when
their continuous symmetry group is replaced by different discrete non-Abelian
subgroups. Precise numerical results with relative errors down to O(0.1%)
suggest that the models with large subgroups are in the universality class of
the underlying original models. We argue that such a scenario is consistent
with the known properties of AF theories. The small statistical errors allow a
detailed investigation of the cut-off effects also. At least up to correlation
lengths ~300 they follow effectively an O(a) rather than the expected O(a^2)
form both in the O(3) and in the dodecahedron model.Comment: 16 pages, 7 figures, some omissions corrected, a reference adde
Predicting the Aoki Phase using the Chiral Lagrangian
This work is concerned with the phase diagram of Wilson fermions in the mass
and coupling constant plane for two-flavor (unquenched) QCD. We show that as
the continuum limit is approached, one can study the lattice theory using the
continuum chiral Lagrangian, supplemented by additional terms proportional to
powers of the lattice spacing. We find two possible phase structures at
non-zero lattice spacing: (1) There is an Aoki phase of spontaneously broken
flavor and parity, with two massless Goldstone-pions, and a width ; (2) There is no spontaneous symmetry breaking, and all three pions
have equal mass of order . Present numerical simulations suggest that the
former option is realized.Comment: LATTICE98(spectrum), 3 pages, 2 figures, LaTex, uses espcrc2.st
Determining Lines of Constant Physics in the Confinement Phase of the SU(2) Higgs Model
We present a method for finding lines of constant physics in the confinement
phase of the SU(2) Higgs model on the lattice. The model is considered at
finite values of the cut-off where it behaves like an effective field theory
with three independent couplings. In particular, a renormalised quantity
sensitive to a variation of the bare Higgs quartic self-coupling is constructed
from generalised Binder cumulants. Numerical results for the non-perturbative
matching of the bare parameters of the model between beta=2.2 and beta=2.4 are
presented.Comment: 10 pages, 4 figures, small changes in the introductio
Non-perturbative O(a) improvement of the vector current
We discuss non-perturbative improvement of the vector current, using the
Schroedinger Functional formalism. By considering a suitable Ward identity, we
compute the improvement coefficient which gives the O(a) mixing of the tensor
current with the vector one.Comment: 3 pages (LaTeX, 2 ps figures, styles), talk presented at Lattice 9
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