191 research outputs found

    Electromagnetic Response of a kx±ikyk_x\pm ik_y Superconductor: Effect of Order Parameter Collective Modes

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    Effects of order parameter collective modes on electromagnetic response are studied for a clean spin-triplet superconductor with kx±ikyk_x\pm ik_y orbital symmetry, which has been proposed as a candidate pairing symmetry for Sr2_2RuO4_4. It is shown that the kx±ikyk_x \pm ik_y superconductor has characteristic massive collective modes analogous to the clapping mode in the A-phase of superfluid 3^3He. We discuss the contribution from the collective modes to ultrasound attenuation and electromagnetic absorption. We show that in the electromagnetic absorption spectrum the clapping mode gives rise to a resonance peak well below the pair breaking frequency, while the ultrasound attenuation is hardly influenced by the collective excitations.Comment: 4 pages RevTex, 1 eps figur

    Light Quark Masses with an O(a)-Improved Action

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    We present the recent Fermilab calculations of the masses of the light quarks, using tadpole-improved Sheikholeslami-Wohlert (SW) quarks. Various sources of systematic errors are studied. Our final result for the average light quark mass in the quenched approximation evaluated in the MSˉ\bar{MS} scheme is mˉq(ÎŒ=2GeV;nf=0)=(mu+md)/2=3.6±0.6MeV\bar{m}_q(\mu=2 GeV;n_f=0)= (m_u+m_d)/2=3.6 \pm 0.6 MeV.Comment: 3 pgs. 3 figures. espcrc2.sty included. Talk presented at LATTICE96(phenomenology

    Anisotropy in the Antiferromagnetic Spin Fluctuations of Sr2RuO4

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    It has been proposed that Sr_2RuO_4 exhibits spin triplet superconductivity mediated by ferromagnetic fluctuations. So far neutron scattering experiments have failed to detect any clear evidence of ferromagnetic spin fluctuations but, instead, this type of experiments has been successful in confirming the existence of incommensurate spin fluctuations near q=(1/3 1/3 0). For this reason there have been many efforts to associate the contributions of such incommensurate fluctuations to the mechanism of its superconductivity. Our unpolarized inelastic neutron scattering measurements revealed that these incommensurate spin fluctuations possess c-axis anisotropy with an anisotropic factor \chi''_{c}/\chi''_{a,b} of \sim 2.8. This result is consistent with some theoretical ideas that the incommensurate spin fluctuations with a c-axis anisotropy can be a origin of p-wave superconductivity of this material.Comment: 5 pages, 3 figures; accepted for publication in PR

    Magnetic Phase Diagram of Ca2-xSrxRuO4 Governed by Structural Distortions

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    We constructed, by the first-principles calculations, a magnetic phase diagram of Sr2_{2}RuO4_4 in the space spanned by structural distortions. Our phase diagram can qualitatively explain the experimental one for Ca2−x_{2-x}Srx_xRuO4_4. We found that the rotation and the tilting of RuO6_6 octahedron are responsible for the ferro- and antiferro-magnetism, respectively, while the flattening of RuO6_6 is the key factor to stabilize those magnetic ground states. Our results imply that the magnetic and the structural instabilities in Sr2_2RuO4_4 are closely correlated cooperatively rather than competitively.Comment: 3 figures; accepted by PRB as rapid communicatio

    Linear Field Dependence of the Normal-State In-Plane Magnetoresistance of Sr2RuO4

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    The transverse and longitudinal in-plane magnetoresistances in the normal state of superconducting Sr2RuO4 single crystals have been measured. At low temperatures, both of them were found to be positive with a linear magnetic-field dependence above a threshold field, a result not expected from electronic band theory. We argue that such behavior is a manifestation of a novel coherent state characterized by a spin pseudo gap in the quasi-particle excitation spectrum in Sr2RuO4.Comment: 4 pages + 5 figure

    Impurities and orbital dependent superconductivity in Sr_2RuO_4

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    There now exists a wealth of experimental evidence that Sr_2RuO_4 is an odd-parity superconductor. Experiments further indicate that among the bands stemming from the Ru {xy,xz,yz} orbitals, the portion of the Fermi surface arising from the xy orbitals exhibits a much larger gap than the portions of the Fermi surface arising from the {xz,yz} orbitals. In this paper the role of impurities on such an orbital dependent superconducting state is examined within the Born approximation. In contrast to expected results for a nodeless p-wave superconductor the unique nature of the superconducting state in Sr_2RuO_4 implies that a low concentration of impurities strongly influences the low temperature behavior.Comment: 5 pages 3 figure

    Detailed study of the ac susceptibility of Sr2RuO4 in oriented magnetic fields

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    We have investigated the ac susceptibility of the spin triplet superconductor Sr2_2RuO4_4 as a function of magnetic field in various directions at temperatures down to 60 mK. We have focused on the in-plane field configuration (polar angle ξ≃90∘\theta \simeq 90^{\circ}), which is a prerequisite for inducing multiple superconducting phases in Sr2_2RuO4_4. We have found that the previous attribution of a pronounced feature in the ac susceptibility to the second superconducting transition itself is not in accord with recent measurements of the thermal conductivity or of the specific heat. We propose that the pronounced feature is a consequence of additional involvement of vortex pinning originating from the second superconducting transition.Comment: Accepted for publication in Phys. Rev.

    Low temperature electronic properties of Sr_2RuO_4 III: Magnetic fields

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    Based on the microscopic model introduced previously the observed specific heat and ac-susceptibility data in the superconducting phase in Sr_2RuO_4 with applied magnetic fields are described consistently within a phenomenological approach. Discussed in detail are the temperature dependence of the upper critical fields H_{c2} and H_2, the dependence of the upper critical fields on the field direction, the linear specific heat below the superconducting phase transition as a function of field or temperature, the anisotropy of the two spatial components of the order parameter, and the fluctuation field H_p.Comment: 8 pages REVTEX, 4 figure

    Experiential contributions to social dominance in a rat model of Fragile-X syndrome

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    Social withdrawal is one phenotypic feature of the monogenic neurodevelopmental disorder Fragile-X. Using a ‘knock-out’ rat model of Fragile-X, we examined whether deletion of the Fmr1 gene that causes this condition would affect the ability to form and express a social hierarchy as measured in a tube-test. Male Fragile-X ‘knock-out’ rats living together could successfully form a social dominance hierarchy, but were significantly subordinate to wild-type animals in mixed group cages. Over 10 days of repeated testing, the Fragile-X mutant rats gradually showed greater variance and instability of rank during their tube-test encounters. This affected the outcome of future encounters with stranger animals from other cages, with the initial phenotype of wild-type dominance lost to a more complex picture that reflected, regardless of genotype, the prior experience of winning or losing. Our findings offer a novel insight into the complex dynamics of social interactions between laboratory living groups of Fragile X and wild-type rats. Even though this is a monogenic condition, experience has an impact upon future interactions with other animals. Gene/environment interactions should therefore be considered in the development of therapeutics

    Spin glass overlap barriers in three and four dimensions

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    For the Edwards-Anderson Ising spin-glass model in three and four dimensions (3d and 4d) we have performed high statistics Monte Carlo calculations of those free-energy barriers FBqF^q_B which are visible in the probability density PJ(q)P_J(q) of the Parisi overlap parameter qq. The calculations rely on the recently introduced multi-overlap algorithm. In both dimensions, within the limits of lattice sizes investigated, these barriers are found to be non-self-averaging and the same is true for the autocorrelation times of our algorithm. Further, we present evidence that barriers hidden in qq dominate the canonical autocorrelation times.Comment: 20 pages, Latex, 12 Postscript figures, revised version to appear in Phys. Rev.
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