21,187 research outputs found

    Relics of Supersymmetry in Ordinary 1-flavor QCD: Hairpin Diagrams and Scalar-Pseudoscalar Degeneracy

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    The large-NcN_c orientifold planar equivalence between N=1\mathcal{N}=1 SUSY Yang-Mills theory and ordinary 1-flavor QCD suggests that low-energy quark-gluon dynamics in QCD should be constrained by the supersymmetry of the parent theory. One SUSY relic expected from orientifold equivalence is the approximate degeneracy of the scalar and pseudoscalar mesons in 1-flavor QCD. Here we study the role of the qqˉq\bar{q} annihilation (hairpin) contributions to the meson correlators. These annihilation terms induce mass shifts of opposite sign in the scalar and pseudoscalar channels, making degeneracy plausible. Calculations of valence and hairpin correlators in quenched lattice QCD are consistent with approximate degeneracy, although the errors on the scalar hairpin are large. We also study the role of qqˉq\bar{q} annihilation in the 1- and 2-flavor Nambu-Jona Lasinio model, where annihilation terms arise from the chiral field determinant representing the axial U(1) anomaly. Scalar-pseudoscalar degeneracy for the 1-flavor case reduces to a constraint on the relative size of the anomalous and non-anomalous 4-fermion couplings.Comment: 17 pages, 3 figure

    Transport phenomenology for a holon-spinon fluid

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    We propose that the normal-state transport in the cuprate superconductors can be understood in terms of a two-fluid model of spinons and holons. In our scenario, the resistivity is determined by the properties of the holons while magnetotransport involves the recombination of holons and spinons to form physical electrons. Our model implies that the Hall transport time is a measure of the electron lifetime, which is shorter than the longitudinal transport time. This agrees with our analysis of the normal-state data. We predict a strong increase in linewidth with increasing temperature in photoemission. Our model also suggests that the AC Hall effect is controlled by the transport time.Comment: 4 pages, 1 postscript figure. Uses RevTeX, epsf, multico

    Computing equilibrium states of cholesteric liquid crystals in elliptical channels with deflation algorithms

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    We study the problem of a cholesteric liquid crystal confined to an elliptical channel. The system is geometrically frustrated because the cholesteric prefers to adopt a uniform rate of twist deformation, but the elliptical domain precludes this. The frustration is resolved by deformation of the layers or introduction of defects, leading to a particularly rich family of equilibrium configurations. To identify the solution set, we adapt and apply a new family of algorithms, known as deflation methods, that iteratively modify the free energy extremisation problem by removing previously known solutions. A second algorithm, deflated continuation, is used to track solution branches as a function of the aspect ratio of the ellipse and preferred pitch of the cholesteric.Comment: 9 pages, 6 figure

    Developmental and tissue-specific expression of the Q5k gene

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    Expression of the Q5k gene was examined by northern blot analysis and polymerase chain reaction (PCR) in the AKR mouse and various cell lines, each of the H-2k haplotype. Our results show that Q5k mRNA is present during the whole postimplantational development of the AKR embryo/fetus (gestation day 6 to 15). In the juvenile mouse (week 2 to 4) transcription of the Q5k gene persisted in all organs examined. In contrast, in the adult animal expression of the Q5k gene was limited to the thymus and uterus of the pregnant mouse. Upon malignant transformation, the amount of Q5k-specific mRNA increased dramatically in thymus and could also be observed in the spleen of thymoma bearing animals. Expression of the Q5k gene was also detectable in several transformed mouse cell lines. Mitogen stimulation or treatment with cytokines induced Q5k expression in primary spleen cell cultures. A possible explanation for the tissue-restricted expression in the adult AKR mouse is discussed

    Complex microwave conductivity of Pr1.85_{1.85}Ce0.15_{0.15}CuO4δ_{4-\delta} thin films using a cavity perturbation method

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    We report a study of the microwave conductivity of electron-doped Pr1.85_{1.85}Ce0.15_{0.15}CuO4δ_{4-\delta} superconducting thin films using a cavity perturbation technique. The relative frequency shifts obtained for the samples placed at a maximum electric field location in the cavity are treated using the high conductivity limit presented recently by Peligrad et\textit{et} al.\textit{al.} Using two resonance modes, TE102_{102} (16.5 GHz) and TE101_{101} (13 GHz) of the same cavity, only one adjustable parameter Γ\Gamma is needed to link the frequency shifts of an empty cavity to the ones of a cavity loaded with a perfect conductor. Moreover, by studying different sample configurations, we can relate the substrate effects on the frequency shifts to a scaling factor. These procedures allow us to extract the temperature dependence of the complex penetration depth and the complex microwave conductivity of two films with different quality. Our data confirm that all the physical properties of the superconducting state are consistent with an order parameter with lines of nodes. Moreover, we demonstrate the high sensitivity of these properties on the quality of the films

    Fractionally charged Wilson loops as a probe of θ\theta-dependence in CPN1CP^{N-1} sigma models: Instantons vs. large N

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    The behavior of Wilson loops with fractional charge is used to study the θ\theta-dependence of the free energy density ϵ(θ)\epsilon(\theta) for the CP1CP^1, CP5CP^5, and CP9CP^9 sigma models in two spacetime dimensions. The function ϵ(θ)\epsilon(\theta) is extracted from the area law for a Wilson loop of charge q=θ/2πq=\theta/2\pi. For CP1CP^1, ϵ(θ)\epsilon(\theta) is smooth in the region θπ\theta\approx\pi and well-described by a dilute instanton gas throughout the range 0<θ<2π0<\theta<2\pi. For CP5CP^5 and CP9CP^9 the energy exhibits a clear cusp and evidence for discrete, degenerate vacua at θ=π\theta = \pi, as expected from large NN arguments. For CP9CP^9 the θ\theta-dependence is in good quantitative agreement with the leading order large NN prediction ϵ(θ)=1/2χtθ2\epsilon(\theta)={1/2}\chi_t\theta^2 throughout the range 0<θ<π0<\theta<\pi.Comment: 16 pages, 10 figure

    Diffusion of a granular pulse in a rotating drum

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    The diffusion of a pulse of small grains in an horizontal rotating drum is studied through discrete elements methods simulations. We present a theoretical analysis of the diffusion process in a one-dimensional confined space in order to elucidate the effect of the confining end-plate of the drum. We then show that the diffusion is neither subdiffusive nor superdiffusive but normal. This is demonstrated by rescaling the concentration profiles obtained at various stages and by studying the time evolution of the mean squared deviation. Finally we study the self-diffusion of both large and small grains and we show that it is normal and that the diffusion coefficient is independent of the grain size
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