325 research outputs found

    The fossil record of early tetrapods: worker effort and the end-Permian mass extinction

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    It is important to understand the quality of the fossil record of early tetrapods (Tetrapoda, minus Lissamphibia and Amniota) because of their key role in the transition of vertebrates from water to land, their dominance of terrestrial faunas for over 100 million years of the late Palaeozoic and earlyMesozoic, and their variable fates during the end−Permian mass extinction. The first description of an early tetrapod dates back to 1824, and since then discoveries have occurred at a rather irregular pace, with peaks and troughs corresponding to some of the vicissitudes of human history through the past two centuries. As expected, the record is dominated by the well−sampled sedimentary basins of Europe and North America, but finds from other continents are increasing rapidly. Comparisons of snapshots of knowledge in 1900, 1950, and 2000 show that discovery of new species has changed the shape of the species−level diversification curve, contrary to earlier studies of family−level taxa. There is, however, little evidence that taxon counts relate to research effort (as counted by numbers of publications), and there are no biasing effects associated with differential study of different time intervals through the late Palaeozoic and Mesozoic. In fact, levels of effort are apparently not related to geological time, with no evidence that workers have spent more time on more recent parts of the record. In particular, the end−Permian mass extinction was investigated to determine whether diversity changes through that interval might reflect worker effort: it turns out that most records of early tetrapod taxa (when corrected for duration of geological series) occur in the Lower Triassic

    A Relation Between Approaches to Integrability in Superconformal Yang-Mills Theory

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    We make contact between the infinite-dimensional non-local symmetry of the typeIIB superstring on AdS5xS5 worldsheet theory and a non-abelian infinite-dimensional symmetry algebra for the weakly coupled superconformal gauge theory. We explain why the planar limit of the one-loop dilatation operator is the Hamiltonian of a spin chain, and show that it commutes with the g*2 N = 0 limit of the non-abelian charges.Comment: 19 pages, harvma

    Freezing transitions and the density of states of 2D random Dirac Hamiltonians

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    Using an exact mapping to disordered Coulomb gases, we introduce a novel method to study two dimensional Dirac fermions with quenched disorder in two dimensions which allows to treat non perturbative freezing phenomena. For purely random gauge disorder it is known that the exact zero energy eigenstate exhibits a freezing-like transition at a threshold value of disorder σ=σth=2\sigma=\sigma_{th}=2. Here we compute the dynamical exponent zz which characterizes the critical behaviour of the density of states around zero energy, and find that it also exhibits a phase transition. Specifically, we find that ρ(E=0+iÏ”)∌ϔ2/z−1\rho(E=0 + i \epsilon) \sim \epsilon^{2/z-1} (and ρ(E)∌E2/z−1\rho(E) \sim E^{2/z-1}) with z=1+σz=1 + \sigma for σ<2\sigma < 2 and z=8σ−1z=\sqrt{8 \sigma} - 1 for σ>2\sigma > 2. For a finite system size L<ϔ−1/zL<\epsilon^{-1/z} we find large sample to sample fluctuations with a typical ρϔ(0)∌Lz−2\rho_{\epsilon}(0) \sim L^{z-2}. Adding a scalar random potential of small variance ÎŽ\delta, as in the corresponding quantum Hall system, yields a finite noncritical ρ(0)∌Ύα\rho(0) \sim \delta^{\alpha} whose scaling exponent α\alpha exhibits two transitions, one at σth/4\sigma_{th}/4 and the other at σth\sigma_{th}. These transitions are shown to be related to the one of a directed polymer on a Cayley tree with random signs (or complex) Boltzmann weights. Some observations are made for the strong disorder regime relevant to describe transport in the quantum Hall system

    Destabilization of dark states and optical spectroscopy in Zeeman-degenerate atomic systems

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    We present a general discussion of the techniques of destabilizing dark states in laser-driven atoms with either a magnetic field or modulated laser polarization. We show that the photon scattering rate is maximized at a particular evolution rate of the dark state. We also find that the atomic resonance curve is significantly broadened when the evolution rate is far from this optimum value. These results are illustrated with detailed examples of destabilizing dark states in some commonly-trapped ions and supported by insights derived from numerical calculations and simple theoretical models.Comment: 14 pages, 10 figure
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