Hadronic spectroscopy at a ≈ 0.15 fm.
Nuclear Physics B (Proceedings Supplements) 20:C (1991) 362-369
Abstract:
We discuss some aspects of the hadron spectrum with two flavors of Kogut-Susskind dynamical quarks at 6/g2 = 5.6 and amq = 0.01 and 0.025, using both Kogut-Susskind and Wilson valence quarks. Our high statistics simulations allow us to study systematic errors. Among the problematic features of our results are a dip in the pion effective mass which we ascribe to replicating the lattice in the time direction and large finite size effects in the baryon masses. We also compare the full QCD results to a quenched simulation at similar lattice spacing and quark masses to test whether the effects of dynamical fermions can be absorbed into renormalization of the lattice parameters. © 1991.Pure gauge theories
Nuclear Physics B (Proceedings Supplements) 20:C (1991) 159-172
Abstract:
I focus on three topics in my review of pure gauge theories. Firstly, how close are we to solving the continuum theory. Secondly, cooling and confinement. Thirdly, the status of lattice topology. © 1991.QCD thermodynamics with Wilson quarks
Nuclear Physics B (Proceedings Supplements) 20:C (1991) 272-275
Abstract:
We present results from a study of hadron thermodynamics with Wilson quarks. The crossover curve between the high and low temperature phases is determined as a function of the gauge coupling and hopping parameter on 83 × 4 lattices. Meson masses are calculated along the crossover curve, and screening lengths are determined in the vicinity of it on 83 × 16 and 82 × 16 × 4 lattices, respectively. © 1991.On the implications of a 17 keV neutrino
Physics Letters B 260:3-4 (1991) 381-388
Abstract:
We discuss the implications of the recent measurement of a 17 keV mass component in the electron neutrino sector. Such a heavy state must decay in order to be compatible with cosmology; this requires states additional to those of the standard model. The most likely candidates are either majorons, allowing the decay into massless weakly interacting scalars, or single neutrinos, allowing the decay via the Z into light neutrinos. We show that in the latter case there is a lower bound on the lifetime in conflict with the cosmological constraints on this decay channel and on the photon plus neutrino decay channel which is also present. The extensions of the standard model needed to reduce the lifetime are considered. We analyze the mass matrix, playing particular regard to the singlet neutrino case, and discuss how it might be extended to explain the solar neutrino deficit. © 1991.Topological fluctuations in SU(2) gauge theory with staggered fermions: An explotary study
Nuclear Physics, Section B 348:1 (1991) 178-209