- The variegated mud-loving beetles (Coleoptera: Heteroceridae) of Mississippi and Alabama, with discussion and keys to the species occurring in the southeastern United States (2012)
- We review the variegated mud-loving beetle fauna of the southeastern United States (Coleoptera: Heteroceridae), with an emphasis on Mississippi and Alabama. A key is presented to all species known to occur in the southeastern US, and includes several extra-limital species. Descriptions, illustrations and distribution maps are presented for each species. One new species, Tropicus nigrellus, is described and a lectotype is designated for Heterocerus schwarzi Horn. Our molecular data suggest that many previously recognized generic concepts are unnatural. As a result, the following generic synonymies are proposed: Culmus Pacheco 1964, Damfius Pacheco 1964, Efflagitatus Pacheco 1964, Erus Pacheco 1964, Filiolus Pacheco 1964, Gradus Pacheco 1964, Lanternarius Pacheco 1964, Lapsus Pacheco 1964, Neoheterocerus Pacheco 1964, Olmedous Pacheco 1964 and Peditatus Pacheco 1964 are synonyms of Heterocerus Fabricius; the genera Centariatus Pacheco 1964, Explorator Pacheco 1964, and Microaugyles Pacheco 1964 are synonyms of Augyles Schiödte. New combinations proposed and used in this paper include: Augyles auromicans (Kiesenwetter 1851, Heterocerus), Heterocerus parrotus (Pacheco 1964, Lanternarius), Heterocerus sandersoni (Pacheco 1964, Neoheterocerus) and Heterocerus selanderi (Pacheco 1964, Efflagitatus), Heterocerus texanus (Pacheco 1964, Peditatus). Other new combinations for North American species formed as a result of these generic reconfigurations, but not used in this paper, include: Heterocerus inciertus (Pacheco 1964, Damfius), Heterocerus longilobulus (Pacheco 1964, Neoheterocerus), Heterocerus sinuosus (Pacheco 1964, Lanternarius), Augyles canadensis (Fall 1920, Heterocerus), Augyles compactus (Fall 1937, Heterocerus), Augyles moleculus (Fall 1920, Heterocerus) and Augyles mundulus (Fall 1920, Heterocerus). New combinations for South American species suggested by molecular data, all originally described in the genus Efflagitatus, include: Heterocerus boliviensis (Pacheco 1964), Heterocerus freudei (Pacheco 1973), Heterocerus furmidus (Pacheco 1964), Heterocerus ingeniosus (Pacheco 1964), Heterocerus meridianus (Pacheco 1975), Heterocerus reticulatus (Pacheco 1964), Heterocerus solitarius (Pacheco 1973), Heterocerus splendidus (Pacheco 1964), Heterocerus tortuosus (Pacheco 1973), Heterocerus woodruffi (Pacheco 1975). No new combinations involving synonymy within the genera Culmus, Erus, Filiolus, Gradus, Lapsus, and Olmedous were proposed because all included species were originally described as Heterocerus. Introduction
- Emission patterns in central and peripheral relativistic heavy-ion collisions (1980)
- Proton emission in relativistic nuclear collisions is examined for events of low and high multiplicity, corresponding to large and small impact parameters. Peripheral reactions exhibit distributions of protons in agreement with spectator-participant decay modes. Central collisions of equal-size nuclei are dominated by the formation and decay of a fireball system. Central collisions of light projectiles with heavy targets exhibit an enhancement in sideward emission which is predicted by recent hydrodynamical calculations.
- Pion production and charged-particle multiplicity selection in relativistic nuclear collisions (1982)
- Spectra of positive pions with energies of 15-95 MeV were measured for high energy proton, 4He, 20Ne, and 40Ar bombardments of targets of 27Al, 40Ca, 107,109Ag, 197Au, and 238U. A Si-Ge telescope was used to identify charged pions by dE / dx-E and, in addition, stopped pi + were tagged by the subsequent muon decay. In all, results for 14 target-projectile combinations are presented to study the dependence of pion emission patterns on the bombarding energy (from E / A=0.25 to 2.1 GeV) and on the target and the projectile masses. In addition, associated charged-particle multiplicities were measured in an 80-paddle array of plastic scintillators, and used to make impact parameter selections on the pion-inclusive data. NUCLEAR REACTIONS U(20Ne, pi +), E / A=250 MeV; U(40Ar, pi +), Ca(40Ar, pi +), U(20Ne, pi +), Au(20Ne, pi +), Ag(20Ne, pi +), Al(20Ne, pi +), U(4He, pi +), Al(4He, pi +). E / A=400 MeV; Ca(40Ar, pi +), U(20Ne, pi +), U(4He, pi +), U(p, pi +), E / A=1.05), GeV; U(20Ne, pi +), E / A=2.1 GeV; measured sigma (E, theta ), inclusive and selected on associated charged-particle multiplicity.
- Spectra of p, d, and t from relativistic nuclear collisions (1980)
- Inclusive energy spectra of protons, deuterons, and tritons were measured with a telescope of silicon and germanium detectors with a detection range for proton energies up to 200 MeV. Fifteen sets of data were taken using projectiles ranging from protons to 40Ar on targets from 27Al to 238U at bombarding energies from 240 MeV/nucleon to 2.1 GeV/nucleon. Particular attention was paid to the absolute normalization of the cross sections. For three previously reported reactions, He fragment cross sections have been corrected and are presented. To facilitate a comparison with theory the sum of nucleonic charges emitted as protons plus composite particles was estimated and is presented as a function of fragment energy per nucleon in the interval from 15 to 200 MeV/nucleon. For low-energy fragments at forward angles the protons account for only 25% of the nucleonic charges. The equal mass 40Ar plus Ca systems were examined in the center of mass. Here at 0.4 GeV/nucleon 40Ar plus Ca the proton spectra appear to be nearly isotropic in the center of mass over the region measured. Comparisons of some data with firestreak, cascade, and fluid dynamics models indicate a failure of the first and a fair agreement with the latter two. In addition, associated fast charged particle multiplicities (where the particles had energies larger than 25 MeV/nucleon) and azimuthal correlations were measured with an 80 counter array of plastic scintillators. It was found that the associated multiplicities were a smooth function of the total kinetic energy of the projectile. NUCLEAR REACTIONS U(20Ne,X), E / A=240 MeV/nucleon; U(40Ar,X), Ca(40Ar,X), U(20Ne,X), Au(20Ne,X), Ag(20Ne,X), Al(20Ne,X), U(4He,X), Al(4He,X), E / A=390 MeV/nucleon; U(40Ar,X), Ca(40Ar,X), U(20Ne,X), U(4He,X), U(p,X), E / A=1.04 GeV/nucleon; U(20Ne,X), E / A=2.1 GeV/nucleon; measured sigma (E, theta ), X=p,d,t.
- Pion Production in the 40Ar+40Ca Reaction at 1.05 GeV/Nucleon (1979)
- Pion-production cross sections have been measured for the reaction 40Ar+40Ca--> pi ++X at a laboratory energy of 1.05 GeV/nucleon. A maximum in the pi + cross section occurs at mid-rapidity, which is anomalous relative to p+p and p+nucleus reactions and compared to many other heavy-ion reactions. Calculations based on cascade and thermal models fail to fit the data.
- Monetary discretion, pricing complementarity and dynamic multiple equilibria (2004)
- In a plain-vanilla New Keynesian model with two-period staggered price-setting, discretionary monetary policy leads to multiple equilibria. Complementarity between the pricing decisions of forward-looking firms underlies the multiplicity, which is intrinsically dynamic in nature. At each point in time, the discretionary monetary authority optimally accommodates the level of predetermined prices when setting the money supply because it is concerned solely about real activity. Hence, if other firms set a high price in the current period, an individual firm will optimally choose a high price because it knows that the monetary authority next period will accommodate with a high money supply. Under commitment, the mechanism generating complementarity is absent: the monetary authority commits not to respond to future predetermined prices. Multiple equilibria also arise in other similar contexts where (i) a policymaker cannot commit, and (ii) forward-looking agents determine a state variable to which future policy respond. Klassifikation: E5, E61, D78. March 2004