419 research outputs found

    Ohio SB5 and the Attempt to “Yeshiva” Public University Faculty

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    In 2011, the introduction of Ohio Senate Bill 5 (SB5) attempted to drastically curtail public sector collective bargaining in Ohio. The bill included a proposed amendment designed by the Inter-University Council of Ohio, an organization of the top administrators of the state universities in Ohio, under the guise of applying the United States Supreme Court’s decision in NLRB v. Yeshiva to faculty at Ohio’s public universities. The avowed intent of the proposed language was to classify all faculty as supervisors or managers and thereby make them ineligible to bargain collectively. After mounting opposition and grass roots efforts, SB5 was ultimately revoked by voter referendum. The general assumption was that if SB5 had gone into effect, faculty would be automatically classified as supervisors and/or managers and be excluded from collective bargaining. Thus, the only way to stop the elimination of faculty from being “Yeshiva’d” was to revoke SB5. This paper questions that assumption and analyzes several questions about the attempt to utilize the Yeshiva decision to re-classify all faculty as supervisors or managers that remained unanswered. Answers to these questions not only provide insight into future issues for higher education faculty in Ohio, but also in other states that attempt similar legislative maneuvering

    A note on Weyl transformations in two-dimensional dilaton gravity

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    We discuss Weyl (conformal) transformations in two-dimensional matterless dilaton gravity. We argue that both classical and quantum dilaton gravity theories are invariant under Weyl transformations.Comment: 8 pages, accepted for publication in Mod. Phys. Lett.

    Exact Quantum States for all Two-Dimensional Dilaton Gravity Theories

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    It is shown that the recently obtained quantum wave functionals in terms of the CJZ variables for generic 2d dilaton gravity are equivalent to the previously reported exact quantum wave functionals in geometrical variables. A third representation of these exact quantum states is also presented

    Geometrodynamical Formulation of Two-Dimensional Dilaton Gravity

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    Two-dimensional matterless dilaton gravity with arbitrary dilatonic potential can be discussed in a unitary way, both in the Lagrangian and canonical frameworks, by introducing suitable field redefinitions. The new fields are directly related to the original spacetime geometry and in the canonical picture they generalize the well-known geometrodynamical variables used in the discussion of the Schwarzschild black hole. So the model can be quantized using the techniques developed for the latter case. The resulting quantum theory exhibits the Birkhoff theorem at the quantum level.Comment: 15 pages, LATE

    TWO DIMENSIONAL DILATON GRAVITY COUPLED TO AN ABELIAN GAUGE FIELD

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    The most general two-dimensional dilaton gravity theory coupled to an Abelian gauge field is considered. It is shown that, up to spacetime diffeomorphisms and U(1)U(1) gauge transformations, the field equations admit a two-parameter family of distinct, static solutions. For theories with black hole solutions, coordinate invariant expressions are found for the energy, charge, surface gravity, Hawking temperature and entropy of the black holes. The Hawking temperature is proportional to the surface gravity as expected, and both vanish in the case of extremal black holes in the generic theory. A Hamiltonian analysis of the general theory is performed, and a complete set of (global) Dirac physical observables is obtained. The theory is then quantized using the Dirac method in the WKB approximation. A connection between the black hole entropy and the imaginary part of the WKB phase of the Dirac quantum wave functional is found for arbitrary values of the mass and U(1)U(1) charge. The imaginary part of the phase vanishes for extremal black holes and for eternal, non-extremal Reissner-Nordstrom black holes.Comment: Minor revisions only. Some references have been added, and some typographical errors correcte

    Dirac Constraint Quantization of a Dilatonic Model of Gravitational Collapse

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    We present an anomaly-free Dirac constraint quantization of the string-inspired dilatonic gravity (the CGHS model) in an open 2-dimensional spacetime. We show that the quantum theory has the same degrees of freedom as the classical theory; namely, all the modes of the scalar field on an auxiliary flat background, supplemented by a single additional variable corresponding to the primordial component of the black hole mass. The functional Heisenberg equations of motion for these dynamical variables and their canonical conjugates are linear, and they have exactly the same form as the corresponding classical equations. A canonical transformation brings us back to the physical geometry and induces its quantization.Comment: 37 pages, LATEX, no figures, submitted to Physical Review

    Free fields via canonical transformations of matter-coupled 2D dilaton gravity models

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    It is shown that the 1+1-dimensional matter-coupled Jackiw-Teitelboim model and the model with an exponential potential can be converted by means of appropriate canonical transformations into a bosonic string theory propagating on a flat target space with an indefinite signature. This makes it possible to consistently quantize these models in the functional Schroedinger representation thus generalizing recent results on CGHS theory.Comment: 15 pages, Late

    A Solvable Model of Two-Dimensional Dilaton-Gravity Coupled to a Massless Scalar Field

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    We present a solvable model of two-dimensional dilaton-gravity coupled to a massless scalar field. We locally integrate the field equations and briefly discuss the properties of the solutions. For a particular choice of the coupling between the dilaton and the scalar field the model can be interpreted as the two-dimensional effective theory of 2+1 cylindrical gravity minimally coupled to a massless scalar field.Comment: 6 pages, RevTeX, to be published in Phys. Rev.

    Radial Solutions of the Schrodinger's Equation with Superposition of Yukawa and Manning-Rosen Applying the Nikiforov-Uvarov Method

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    The solutions of the SchrÓ§dinger equation with Manning-Rosen plus Yukawa potential (MRYP) have been presented using the Pekeris-like approximation of the Coulomb term and parametric Nikiforov-Uvarov (NU) method. The bound state energy eigenvalues and the corresponding un-normalized eigenfunctions are obtained regarding Jacobi polynomials. Also, Yukawa, Manning-Rosen, and Coulomb potentials have been recovered from the mixed potential, and their eigenvalues obtained
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