422 research outputs found

    Claytonia lanceolata Pursh

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    https://thekeep.eiu.edu/herbarium_specimens_byname/12506/thumbnail.jp

    The Eighth Sacrament? The Evidence of Hincmar of Rheims

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    The Catholic Church did not dogmatically define the list of seven sacraments until the Council of Trent in the 16th century, marking the culmination of hundreds of years of theological study and reflection upon sacraments. After the definition of seven, French theologians argued that the coronation of their king was an eighth sacrament. In this paper, I contend that Hincmar of Rheims, his theology of kingship, and the coronation rites that he compiled are likely responsible for the French claim. Hincmar was the Archbishop of Rheims from 845 until his death in 882. During his time as archbishop, he compiled four unique coronation rites: two for queens and two for kings. Hincmar’s are the oldest surviving coronation rites from continental Europe and they serve as the foundation of nearly all traditions of European coronations, including those of the French kings, the Holy Roman emperors, and still-reigning English monarchs. By closely analyzing Hincmar’s De Ordine Palatii (DOP) and his Ordo of Charles the Bald (OCB), I was able to determine that Hincmar likely believed his coronation rites to be sacraments. I argue that the DOP contains Hincmar’s theopolitical vision: an ideal conception of the Church and the king’s government working in tandem to bring about the salvation of souls. His theology is wrapped up in his politics and vice versa. This analysis yielded a unified understanding of the distinct offices of kingship and priesthood. The OCB shows, in practice, the theories of the DOP. By closely reading the OCB and the historical circumstances that surrounded the celebration, I was able to clearly highlight Hincmar’s two-fold understanding of coronation: there is the unction, the ostentatiously sacramental part of the rite wherein a man becomes a king in the sight of God, and the crowning, a purely juridical act wherein a man becomes a king in the eyes of his people. In parsing this distinction, I made two notable contributions to the secondary literature: firstly that Hincmar may have used the Old Testament precedent of Aaron’s ordination as inspiration for the rubric of his unction of Charles the Bald; secondly, that the actual crowning was not done by Hincmar, but by a group of bishops from the province of Trier. Hincmar’s attitudes and legal maneuvering, both in the DOP and OCB, can serve as the primary evidence that he believed his coronations to be sacraments. This fact becomes even more convincing when one considers the immediate effects of coronation rites after Hincmar’s death in 882 and Charles the Fat’s deposition in 887. When the Franks outlived the family that was meant to rule over them as their kings forever, the people and the clergy had to find a new way to establish the legitimacy of a monarch. Thanks to the work of Hincmar, that legitimacy came to be sourced in a sacrament of the Church: the sacrament of coronation

    Magnetic-field and current-density distributions in thin-film superconducting rings and disks

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    We show how to calculate the magnetic-field and sheet-current distributions for a thin-film superconducting annular ring (inner radius a, outer radius b, and thickness d<<a) when either the penetration depth obeys lambda < d/2 or, if lambda > d/2, the two-dimensional screening length obeys Lambda = 2 lambda^2/d << a for the following cases: (a) magnetic flux trapped in the hole in the absence of an applied magnetic field, (b) zero magnetic flux in the hole when the ring is subjected to an applied magnetic field, and (c) focusing of magnetic flux into the hole when a magnetic field is applied but no net current flows around the ring. We use a similar method to calculate the magnetic-field and sheet-current distributions and magnetization loops for a thin, bulk-pinning-free superconducting disk (radius b) containing a dome of magnetic flux of radius a when flux entry is impeded by a geometrical barrier.Comment: 10 pages, 13 figure

    Vortex Solid-Liquid Transition in Bi2_{2}Sr2_{2}CaCu2_{2}O8+δ_{8+\delta} with a High Density of Strong Pins

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    The introduction of a large density of columnar defects in %underdoped Bi2_{2}Sr2_{2}CaCu2_{2}O8+δ_{8+\delta} crystals does not, at sufficiently low vortex densities, increase the irreversibility line beyond the first order transition (FOT) field of pristine crystals. At such low fields, the flux line wandering length rwr_{w} behaves as in pristine %Bi2_{2}Sr2_{2}CaCu2_{2}O8+δ_{8+\delta} crystals. Next, vortex positional correlations along the cc--axis in the vortex Bose glass at fields above the FOT are smaller than in the low--field vortex solid. Third, the Bose-glass-to-vortex liquid transition is signaled by a rapid decrease in c-axis phase correlations. These observations are understood in terms of the ``discrete superconductor'' model.Comment: 4 pages, 4 figures Submitted to Phys. Rev. B Rapid Comm. 16-1-2004 Revised version 18-3-200

    Scaling in Small-World Resistor Networks

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    We study the effective resistance of small-world resistor networks. Utilizing recent analytic results for the propagator of the Edwards-Wilkinson process on small-world networks, we obtain the asymptotic behavior of the disorder-averaged two-point resistance in the large system-size limit. We find that the small-world structure suppresses large network resistances: both the average resistance and its standard deviation approaches a finite value in the large system-size limit for any non-zero density of random links. We also consider a scenario where the link conductance decays as a power of the length of the random links, lαl^{-\alpha}. In this case we find that the average effective system resistance diverges for any non-zero value of α\alpha.Comment: 15 pages, 6 figure

    Extreme Ultra-Violet Spectroscopy of the Lower Solar Atmosphere During Solar Flares

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    The extreme ultraviolet portion of the solar spectrum contains a wealth of diagnostic tools for probing the lower solar atmosphere in response to an injection of energy, particularly during the impulsive phase of solar flares. These include temperature and density sensitive line ratios, Doppler shifted emission lines and nonthermal broadening, abundance measurements, differential emission measure profiles, and continuum temperatures and energetics, among others. In this paper I shall review some of the advances made in recent years using these techniques, focusing primarily on studies that have utilized data from Hinode/EIS and SDO/EVE, while also providing some historical background and a summary of future spectroscopic instrumentation.Comment: 34 pages, 8 figures. Submitted to Solar Physics as part of the Topical Issue on Solar and Stellar Flare

    Decoupling and decommensuration in layered superconductors with columnar defects

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    We consider layered superconductors with a flux lattice perpendicular to the layers and random columnar defects parallel to the magnetic field B. We show that the decoupling transition temperature Td, at which the Josephson coupling vanishes, is enhanced by columnar defects by an amount ~B^2 relative to Td. Decoupling by increasing field can be followed by a reentrant recoupling transition for strong disorder. We also consider a commensurate component of the columnar density and show that its pinning potential is renormalized to zero above a critical long wavelength disorder. This decommnesuration transition may account for a recently observed kink in the melting line.Comment: 5 pages, Revte

    D* Production in Deep Inelastic Scattering at HERA

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    This paper presents measurements of D^{*\pm} production in deep inelastic scattering from collisions between 27.5 GeV positrons and 820 GeV protons. The data have been taken with the ZEUS detector at HERA. The decay channel D+(D0Kπ+)π+D^{*+}\to (D^0 \to K^- \pi^+) \pi^+ (+ c.c.) has been used in the study. The e+pe^+p cross section for inclusive D^{*\pm} production with 5<Q2<100GeV25<Q^2<100 GeV^2 and y<0.7y<0.7 is 5.3 \pms 1.0 \pms 0.8 nb in the kinematic region {1.3<pT(D±)<9.01.3<p_T(D^{*\pm})<9.0 GeV and η(D±)<1.5| \eta(D^{*\pm}) |<1.5}. Differential cross sections as functions of p_T(D^{*\pm}), η(D±),W\eta(D^{*\pm}), W and Q2Q^2 are compared with next-to-leading order QCD calculations based on the photon-gluon fusion production mechanism. After an extrapolation of the cross section to the full kinematic region in p_T(D^{*\pm}) and η\eta(D^{*\pm}), the charm contribution F2ccˉ(x,Q2)F_2^{c\bar{c}}(x,Q^2) to the proton structure function is determined for Bjorken xx between 2 \cdot 104^{-4} and 5 \cdot 103^{-3}.Comment: 17 pages including 4 figure

    Observation of Scaling Violations in Scaled Momentum Distributions at HERA

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    Charged particle production has been measured in deep inelastic scattering (DIS) events over a large range of xx and Q2Q^2 using the ZEUS detector. The evolution of the scaled momentum, xpx_p, with Q2,Q^2, in the range 10 to 1280 GeV2GeV^2, has been investigated in the current fragmentation region of the Breit frame. The results show clear evidence, in a single experiment, for scaling violations in scaled momenta as a function of Q2Q^2.Comment: 21 pages including 4 figures, to be published in Physics Letters B. Two references adde

    Observation of hard scattering in photoproduction events with a large rapidity gap at HERA

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    Events with a large rapidity gap and total transverse energy greater than 5 GeV have been observed in quasi-real photoproduction at HERA with the ZEUS detector. The distribution of these events as a function of the γp\gamma p centre of mass energy is consistent with diffractive scattering. For total transverse energies above 12 GeV, the hadronic final states show predominantly a two-jet structure with each jet having a transverse energy greater than 4 GeV. For the two-jet events, little energy flow is found outside the jets. This observation is consistent with the hard scattering of a quasi-real photon with a colourless object in the proton.Comment: 19 pages, latex, 4 figures appended as uuencoded fil
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