2,095 research outputs found

    A Ranking of State Governments' Efficient Use of Expenditures to Encourage Small Firm Births

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    We assume state governments are rational in their budgeting behavior. If this is true, then it is intuitive that they would allocate their expenditures so as to receive the maximum possible benefit for the least cost. Within the parameters of this study, we assume state governments work to receive the maximum number of firm births for the least amount of expenditure. Using regression analysis, we attempt to determine common state government expenditures that indirectly promote firm birth. We then employ non-parametric efficiency testing to rank states by their relative efficiency in using the significant expenditures to promote firm births. The regression results reveal three positive and significant expenditures in determining small firm birth, while relative efficiency rankings based on the use of these target expenditures indicate how states compare to their peers in terms of efficient expenditure use

    Scaling and the Metal-Insulator Transition in Si/SiGe Quantum Wells

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    The existence of a metal-insulator transition at zero magnetic field in two- dimensional electron systems has recently been confirmed in high mobility Si-MOSFETs. In this work, the temperature dependence of the resistivity of gated Si/SiGe/Si quantum well structures has revealed a similar metal- insulator transition as a function of carrier density at zero magnetic field. We also report evidence for a Coulomb gap in the temperature dependence of the resistivity of the dilute 2D hole gas confined in a SiGe quantum well. In addition, the resistivity in the insulating phase scales with a single parameter, and is sample independent. These results are consistent with the occurrence of a metal-insulator transition at zero magnetic field in SiGe square quantum wells driven by strong hole-hole interactions.Comment: 3 pages, 3 figures, LaTe

    Exploring Halo Substructure with Giant Stars. XV. Discovery of a Connection between the Monoceros Ring and the Triangulum-Andromeda Overdensity?

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    Thanks to modern sky surveys, over twenty stellar streams and overdensity structures have been discovered in the halo of the Milky Way. In this paper, we present an analysis of spectroscopic observations of individual stars from one such structure, "A13", first identified as an overdensity using the M giant catalog from the Two Micron All-Sky Survey. Our spectroscopic observations show that stars identified with A13 have a velocity dispersion of \lesssim 40 km s1\mathrm{km~s^{-1}}, implying that it is a genuine coherent structure rather than a chance super-position of random halo stars. From its position on the sky, distance (\sim15~kpc heliocentric), and kinematical properties, A13 is likely to be an extension of another low Galactic latitude substructure -- the Galactic Anticenter Stellar Structure (also known as the Monoceros Ring) -- towards smaller Galactic longitude and farther distance. Furthermore, the kinematics of A13 also connect it with another structure in the southern Galactic hemisphere -- the Triangulum-Andromeda overdensity. We discuss these three connected structures within the context of a previously proposed scenario that one or all of these features originate from the disk of the Milky Way.Comment: 12 pages, 9 figures. Accepted for publication in Ap

    Singularity theory study of overdetermination in models for L-H transitions

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    Two dynamical models that have been proposed to describe transitions between low and high confinement states (L-H transitions) in confined plasmas are analysed using singularity theory and stability theory. It is shown that the stationary-state bifurcation sets have qualitative properties identical to standard normal forms for the pitchfork and transcritical bifurcations. The analysis yields the codimension of the highest-order singularities, from which we find that the unperturbed systems are overdetermined bifurcation problems and derive appropriate universal unfoldings. Questions of mutual equivalence and the character of the state transitions are addressed.Comment: Latex (Revtex) source + 13 small postscript figures. Revised versio

    Can the trace formula describe weak localisation?

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    We attempt to systematically derive perturbative quantum corrections to the Berry diagonal approximation of the two-level correlation function (TLCF) for chaotic systems. To this end, we develop a ``weak diagonal approximation'' based on a recent description of the first weak localisation correction to conductance in terms of the Gutzwiller trace formula. This semiclassical method is tested by using it to derive the weak localisation corrections to the TLCF for a semiclassically disordered system. Unfortunately the method is unable to correctly reproduce the ``Hikami boxes'' (the relatively small regions where classical paths are glued together by quantum processes). This results in the method failing to reproduce the well known weak localisation expansion. It so happens that for the first order correction it merely produces the wrong prefactor. However for the second order correction, it is unable to reproduce certain contributions, and leads to a result which is of a different form to the standard one.Comment: 23 pages in Latex (with IOP style files), 3 eps figures included, to be a symposium paper in a Topical Issue of Waves in Random Media, 199

    Form factor for a family of quantum graphs: An expansion to third order

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    For certain types of quantum graphs we show that the random-matrix form factor can be recovered to at least third order in the scaled time τ\tau from periodic-orbit theory. We consider the contributions from pairs of periodic orbits represented by diagrams with up to two self-intersections connected by up to four arcs and explain why all other diagrams are expected to give higher-order corrections only. For a large family of graphs with ergodic classical dynamics the diagrams that exist in the absence of time-reversal symmetry sum to zero. The mechanism for this cancellation is rather general which suggests that it may also apply at higher-orders in the expansion. This expectation is in full agreement with the fact that in this case the linear-τ\tau contribution, the diagonal approximation, already reproduces the random-matrix form factor for τ<1\tau<1. For systems with time-reversal symmetry there are more diagrams which contribute at third order. We sum these contributions for quantum graphs with uniformly hyperbolic dynamics, obtaining +2τ3+2\tau^{3}, in agreement with random-matrix theory. As in the previous calculation of the leading-order correction to the diagonal approximation we find that the third order contribution can be attributed to exceptional orbits representing the intersection of diagram classes.Comment: 23 pages (including 4 fig.) - numerous typos correcte

    Asymptotic Limits and Zeros of Chromatic Polynomials and Ground State Entropy of Potts Antiferromagnets

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    We study the asymptotic limiting function W(G,q)=limnP(G,q)1/nW({G},q) = \lim_{n \to \infty}P(G,q)^{1/n}, where P(G,q)P(G,q) is the chromatic polynomial for a graph GG with nn vertices. We first discuss a subtlety in the definition of W(G,q)W({G},q) resulting from the fact that at certain special points qsq_s, the following limits do not commute: limnlimqqsP(G,q)1/nlimqqslimnP(G,q)1/n\lim_{n \to \infty} \lim_{q \to q_s} P(G,q)^{1/n} \ne \lim_{q \to q_s} \lim_{n \to \infty} P(G,q)^{1/n}. We then present exact calculations of W(G,q)W({G},q) and determine the corresponding analytic structure in the complex qq plane for a number of families of graphs G{G}, including circuits, wheels, biwheels, bipyramids, and (cyclic and twisted) ladders. We study the zeros of the corresponding chromatic polynomials and prove a theorem that for certain families of graphs, all but a finite number of the zeros lie exactly on a unit circle, whose position depends on the family. Using the connection of P(G,q)P(G,q) with the zero-temperature Potts antiferromagnet, we derive a theorem concerning the maximal finite real point of non-analyticity in W(G,q)W({G},q), denoted qcq_c and apply this theorem to deduce that qc(sq)=3q_c(sq)=3 and qc(hc)=(3+5)/2q_c(hc) = (3+\sqrt{5})/2 for the square and honeycomb lattices. Finally, numerical calculations of W(hc,q)W(hc,q) and W(sq,q)W(sq,q) are presented and compared with series expansions and bounds.Comment: 33 pages, Latex, 5 postscript figures, published version; includes further comments on large-q serie
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