14,376 research outputs found

    Field-Induced Ferromagnetic Order and Colossal Magnetoresistance in La_{1.2}Sr_{1.8}Mn_2O_7: a ^{139}La NMR study

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    In order to gain insights into the origin of colossal magneto-resistance (CMR) in manganese oxides, we performed a ^{139}La NMR study in the double-layered compound La_{1.2}Sr_{1.8}Mn_2O_7. We find that above the Curie temperature T_C=126 K, applying a magnetic field induces a long-range ferromagnetic order that persists up to T=330 K. The critical field at which the induced magnetic moment is saturated coincides with the field at which the CMR effect reaches to a maximum. Our results therefore indicate that the CMR observed above T_C in this compound is due to the field-induced ferromagnetism that produces a metallic state via the double exchange interaction

    Association schemes from the action of PGL(2,q)PGL(2,q) fixing a nonsingular conic in PG(2,q)

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    The group PGL(2,q)PGL(2,q) has an embedding into PGL(3,q)PGL(3,q) such that it acts as the group fixing a nonsingular conic in PG(2,q)PG(2,q). This action affords a coherent configuration R(q)R(q) on the set L(q)L(q) of non-tangent lines of the conic. We show that the relations can be described by using the cross-ratio. Our results imply that the restrictions R+(q)R_{+}(q) and R(q)R_{-}(q) to the sets L+(q)L_{+}(q) of secant lines and to the set L(q)L_{-}(q) of exterior lines, respectively, are both association schemes; moreover, we show that the elliptic scheme R(q)R_{-}(q) is pseudocyclic. We further show that the coherent configuration R(q2)R(q^2) with qq even allow certain fusions. These provide a 4-class fusion of the hyperbolic scheme R+(q2)R_{+}(q^2), and 3-class fusions and 2-class fusions (strongly regular graphs) of both schemes R+(q2)R_{+}(q^2) and $R_{-}(q^2). The fusion results for the hyperbolic case are known, but our approach here as well as our results in the elliptic case are new.Comment: 33 page

    Interpretations and Implications of the Top Quark Rapidity Asymmetries AFBtA_{FB}^t and AFBA_{FB}^{\ell}

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    Forward-backward asymmetries AFBtA_{FB}^t and AFBA_{FB}^\ell are observed in the top quark tt rapidity distribution and in the rapidity distribution of charged leptons \ell from top quark decay at the Tevatron proton-antiproton collider, and a charge asymmetry ACA_C is seen in proton-proton collisions at the Large Hadron Collider (LHC). In this paper, we update our previous studies of the Tevatron asymmetries using the most recent data. We provide expectations for ACA_C at the LHC based first on model independent extrapolations from the Tevatron, and second based on new physics models that can explain the Tevatron asymmetries. We examine the relationship of the two asymmetries AFBtA_{FB}^t and AFBA_{FB}^\ell. We show their connection through the (VA)(V-A) spin correlation between the charged lepton and the top quark with different polarization states. We show that the ratio of the two asymmetries provides independent insight into new physics models that are invoked to fit the top quark asymmetry. We emphasize the value of the measurement of both asymmetries, and we conclude that a model which produces more right-handed than left-handed top quarks is favored by the present Tevatron data.Comment: Some figures changed. A typo in appendix fixed. Published in Physical Review

    Phase transition in site-diluted Josephson junction arrays: A numerical study

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    We numerically investigate the intriguing effects produced by random percolative disorder in two-dimensional Josephson-junction arrays. By dynamic scaling analysis, we evaluate critical temperatures and critical exponents with high accuracy. It is observed that, with the introduction of site-diluted disorder, the Kosterlitz-Thouless phase transition is eliminated and evolves into a continuous transition with power-law divergent correlation length. Moreover, genuine depinning transition and creep motion are studied, evidence for distinct creep motion types is provided. Our results not only are in good agreement with the recent experimental findings, but also shed some light on the relevant phase transitions.Comment: 7 pages, 8 figures, Phys. Rev. B (in press

    Color Sextet Scalars in Early LHC Experiments

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    We explore the potential for discovery of an exotic color sextet scalar in same-sign top quark pair production in early running at the LHC. We present the first phenomenological analysis at colliders of color sextet scalars with full top quark spin correlations included. We demonstrate that one can measure the scalar mass, the top quark polarization, and confirm the scalar resonance with 1 inverse fb of integrated luminosity. The top quark polarization can distinguish gauge triplet and singlet scalars.Comment: Published version. Title changed in the journal. Table added. Modifications made to the text. References added. 4 pages and 3 figure

    The Top Quark Production Asymmetries AFBtA_{FB}^t and AFBA_{FB}^{\ell}

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    A large forward-backward asymmetry is seen in both the top quark rapidity distribution AFBtA_{FB}^t and in the rapidity distribution of charged leptons AFBA_{FB}^\ell from top quarks produced at the Tevatron. We study the kinematic and dynamic aspects of the relationship of the two observables arising from the spin correlation between the charged lepton and the top quark with different polarization states. We emphasize the value of both measurements, and we conclude that a new physics model which produces more right-handed than left-handed top quarks is favored by the present data.Comment: accepted for publication in Physical Review Letter

    Derivation of Electroweak Chiral Lagrangian from One Family Technicolor Model

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    Based on previous studies deriving the chiral Lagrangian for pseudo scalar mesons from the first principle of QCD in the path integral formalism, we derive the electroweak chiral Lagrangian and dynamically compute all its coefficients from the one family technicolor model. The numerical results of the p4p^4 order coefficients obtained in this paper are proportional to the technicolor number NTCN_{\rm TC} and the technifermion number NTFN_{\rm TF}, which agrees with the arguments in previous works, and which confirms the reliability of this dynamical computation.Comment: 6 page
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