14 research outputs found
Is Quantization of QCD Unique at the Non-Perturbative Level ?
We find that QCD in covariant gauge yields zero for the topological
susceptibility, even at the nonperturbative level. The result is derived in two
ways, one using translational invariance, and the other using the BRST
Hamiltonian. Comparison with the canonical formalism suggests that QCD is not
uniquely defined at the nonperturbative level. Supporting evidence is also
provided in 1+1 dimensions. Our results imply that the strong CP problem admits
a trivial resolution in covariant gauge, but obstacles remain for the U(1)
problem.Comment: 5 pages, Previous version updated and an example in 1+1 dimensions
supplie
A MASTER FORMULA FOR CHIRAL SYMMETRY BREAKING
We derive a master formula for chiral breaking, based on
the Veltman-Bell equations and the Peierls-Dyson relation. Our approach does
not rely on the use of the soft pion limit or an expansion around the chiral
limit, and yields exact results for on-shell pions. Threshold theorems for , , ,
, and are recovered, and corrections to them are given. The
reactions , ,
and are also
discussed. A general formula for scattering and a new one loop
effective action are obtained. The new effective action reproduces the KSFR
relation, and yields specific estimates for the pion polarisabilities. A
detailed comparison with baryon-free chiral perturbation theory to one loop is
made. An extension of our effective action to two loops is outlined.Comment: 119 pages + 7 Figures available from (I.Zahed
Electromagnetic Emission Rates and Spectral Sum Rules
The electromagnetic emission rates at SPS energies satisfy spectral
constraints in leading order in the pion and nucleon densities. These
constraints follow from the strictures of broken chiral symmetry. We saturate
these constraints using available data, leading to model independent emission
rates from a hadronic gas. With a simple fire-ball scenario, only large nucleon
densities may account for the present CERES data.Comment: 4 pages (Latex), 2 embedded ps figures, espcrc1 style, talk given at
Quark Matter 97, December 97, Tsukuba, Japa
Anterior and Posterior Corneal Astigmatism after Refractive Lenticule Extraction for Myopic Astigmatism
Purpose. To assess the amount and the axis orientation of anterior and posterior corneal astigmatism after refractive lenticule extraction (ReLEx) for myopic astigmatism. Methods. We retrospectively examined 53 eyes of 53 consecutive patients (mean age ± standard deviation, 33.2 ± 6.5 years) undergoing ReLEx to correct myopic astigmatism (manifest cylinder = 0.5 diopters (D)). Power vector analysis was performed with anterior and posterior corneal astigmatism measured with a rotating Scheimpflug system (Pentacam HR, Oculus) and refractive astigmatism preoperatively and 3 months postoperatively. Results. Anterior corneal astigmatism was significantly decreased, measuring 1.42 ± 0.73 diopters (D) preoperatively and 1.11 ± 0.53 D postoperatively (p<0.001, Wilcoxon signed-rank test). Posterior corneal astigmatism showed no significant change, falling from 0.44 ± 0.12 D preoperatively to 0.42 ± 0.13 D postoperatively (p=0.18). Refractive astigmatism decreased significantly, from 0.92 ± 0.51 D preoperatively to 0.27 ± 0.44 D postoperatively (p<0.001). The anterior surface showed with-the-rule astigmatism in 51 eyes (96%) preoperatively and 48 eyes (91%) postoperatively. By contrast, the posterior surface showed against-the-rule astigmatism in all eyes preoperatively and postoperatively. Conclusions. The surgical effects were largely attributed to the astigmatic correction of the anterior corneal surface. Posterior corneal astigmatism remained unchanged even after ReLEx for myopic astigmatism
Master Formula Approach to Chiral Symmetry Breaking: Pi-Pi scattering
The master formula approach to chiral symmetry breaking is used to analyze
the phase shifts for scattering in the elastic region. The results are
in excellent agreement with the data for the phase shifts up to the K-K bar
threshold. Our analysis shows that the pi-pi data near threshold in the scalar
channel favors a large quark condensate in the vacuum, i.e. \sim
-(240 MeV)^3.Comment: 17 pages, LaTeX, 1 postscript file of 12 figures in addition.
Equation 2 is changed, the rest is the sam