51,329 research outputs found

    Protecting the Least of These: A New Approach to Child Pornography Pandering Provisions

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    The pandering of child pornography - selling, distributing, or conveying the impression that one possesses sexually graphic images of children for sale or distribution - facilitates actual harm to children, such as molestation. Yet legislative attempts to curb pandering inevitably implicate concerns about panderers\u27 First Amendment rights. This Note argues that in balancing the vulnerability of children against the power of the First Amendment, the law must shift to focus more on the subject of this grievous harm - children. This approach will appropriately extend protection to a subset of the population that is least able to protect itself

    Species Profiles: Life Histories and Environmental Requirements of Coastal Fishes and Invertebrates (Pacific Southwest): Northern anchovy

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    Three genetically distinct groups: British Columbia to northern California, Southern California to the northern Baja peninsula, and central and southern Baja California. (PDF contains 21 pages

    Craig on the Resurrection: A Defense

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    This article is a rebuttal to Robert G. Cavin and Carlos A. Colombetti’s article, “Assessing the Resurrection Hypothesis: Problems with Craig’s Inference to the Best Explanation,” which argues that the Standard Model of current particle physics entails that non-physical things (like a supernatural God or a supernaturally resurrected body) can have no causal contact with the physical universe. As such, they argue that William Lane Craig’s resurrection hypothesis is not only incompatible with the notion of Jesus physically appearing to the disciples, but the resurrection hypothesis is significantly limited in both its explanatory scope and explanatory power. This article seeks to demonstrate why their use of the Standard Model does not logically entail a rejection of the physical resurrection of Jesus when considering the scope and limitations of science itself

    Classical to quantum mapping for an unconventional phase transition in a three-dimensional classical dimer model

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    We study the transition between a Coulomb phase and a dimer crystal observed in numerical simulations of the three-dimensional classical dimer model, by mapping it to a quantum model of bosons in two dimensions. The quantum phase transition that results, from a superfluid to a Mott insulator at fractional filling, belongs to a class that cannot be described within the Landau-Ginzburg-Wilson paradigm. Using a second mapping, to a dual model of vortices, we show that the long-wavelength physics near the transition is described by a U(1) gauge theory with SU(2) matter fields.Comment: 15 pages, 5 figures; v2: added appendi

    Employment Instability and High Unemployment Rates

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    macroeconomics, unemployment

    The Impact of Unemployment Insurance on Job Search

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    macroeconomics, unemployment insurance, job search

    Comment on the Nature of the Ds1(2710)D_{s1}^*(2710) and DsJ(2860)D_{sJ}^*(2860) Mesons

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    Two charm-strange mesons, the Ds1(2710)D_{s1}^*(2710) and the DsJ(2860)D_{sJ}^*(2860), have recently been observed by several experiments. There has been speculation in the literature that the Ds1(2710)D_{s1}^*(2710) is the 23S1(csˉ)2^3S_1(c\bar{s}) state and the DsJ(2860)D_{sJ}^*(2860) is the 13D1(csˉ)1^3D_1(c\bar{s}) state. In this paper we explore this and other explanations in the context of the relativized quark model and the pseudoscalar emission decay model. We conclude that the Ds1(2710)D_{s1}^*(2710) is most likely the 13D1(csˉ)1^3D_1 (c\bar{s}) state and the DsJ(2860)D_{sJ}^*(2860) is most likely the 13D3(csˉ)1^3D_3 (c\bar{s}) state with the 1D21D_2 resonances also contributing to the observed signals and explaining the observed ratios of branching ratios to DKD^*K and DKDK final states. We point out that measuring the DsJ(2860)D_{sJ}^*(2860) spin can support or eliminate this explanation and that there are six excited DsD_s states in this mass region; the 23S12^3S_1, 21S02^1S_0, 13D11^3D_1, 13D31^3D_3 and two 1D21D_2 states. Observing some of the missing states would help confirm the nature of the Ds1(2710)D_{s1}^*(2710) and the DsJ(2860)D_{sJ}^*(2860) states.Comment: 8 pages, 2 figure
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