23,254 research outputs found

    Multidimensional Bosonization

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    Bosonization of degenerate fermions yields insight both into Landau Fermi liquids, and into non-Fermi liquids. We begin our review with a pedagogical introduction to bosonization, emphasizing its applicability in spatial dimensions greater than one. After a brief historical overview, we present the essentials of the method. Well known results of Landau theory are recovered, demonstrating that this new tool of many-body theory is robust. Limits of multidimensional bosonization are tested by considering several examples of non-Fermi liquids, in particular the composite fermion theory of the half-filled Landau level. Nested Fermi surfaces present a different challenge, and these may be relevant in the cuprate superconductors. We conclude by discussing the future of multidimensional bosonization.Comment: 91 pages, 15 eps figures, LaTeX. Minor changes to match the published versio

    Electronic Structures of Antiperovskite Superconductor MgCNi3_3 and Related Compounds

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    Electronic structure of a newly discovered antiperovskite superconductor MgCNi3_3 is investigated by using the LMTO band method. The main contribution to the density of states (DOS) at the Fermi energy EFE_{\rm F} comes from Ni 3dd states which are hybridized with C 2pp states. The DOS at EFE_{\rm F} is varied substantially by the hole or electron doping due to the very high and narrow DOS peak located just below EFE_{\rm F}. We have also explored electronic structures of C-site and Mg-site doped MgCNi3_3 systems, and described the superconductivity in terms of the conventional phonon mechanism.Comment: 3 pages, presented at ORBITAL2001 September 11-14, 2001 (Sendai, JAPAN

    Electronic structures of antiperovskite superconductors: MgXNi3_3 (X=B,C,N)

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    We have investigated electronic structures of a newly discovered antiperovskite superconductor MgCNi3_3 and related compounds MgBNi3_3 and MgNNi3_3. In MgCNi3_3, a peak of very narrow and high density of states is located just below EF\rm E_F, which corresponds to the π\pi^* antibonding state of Ni-3d and C-2p2p but with the predominant Ni-3d character. The prominent nesting feature is observed in the Γ\Gamma-centered electron Fermi surface of an octahedron-cage-like shape that originates from the 19th band. The estimated superconducting parameters based on the simple rigid-ion approximation are in reasonable agreement with experiment, suggesting that the superconductivity in MgCNi3_3 is described well by the conventional phonon mechanism.Comment: 5 pages, 5 figure

    Electronic structure of metallic antiperovskite compound GaCMn3_3

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    We have investigated electronic structures of antiperovskite GaCMn3_3 and related Mn compounds SnCMn3_3, ZnCMn3_3, and ZnNMn3_3. In the paramagnetic state of GaCMn3_3, the Fermi surface nesting feature along the ΓR\Gamma{\rm R} direction is observed, which induces the antiferromagnetic (AFM) spin ordering with the nesting vector {\bf Q} ΓR\sim \Gamma{\rm R}. Calculated susceptibilities confirm the nesting scenario for GaCMn3_3 and also explain various magnetic structures of other antiperovskite compounds. Through the band folding effect, the AFM phase of GaCMn3_3 is stabilized. Nearly equal densities of states at the Fermi level in the ferromagnetic and AFM phases of GaCMn3_3 indicate that two phases are competing in the ground state.Comment: 4 pages, 5 figure

    Electron-boson spectral density of LiFeAs obtained from optical data

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    We analyze existing optical data in the superconducting state of LiFeAs at T=T = 4 K, to recover its electron-boson spectral density. A maximum entropy technique is employed to extract the spectral density I2χ(ω)I^2\chi(\omega) from the optical scattering rate. Care is taken to properly account for elastic impurity scattering which can importantly affect the optics in an ss-wave superconductor, but does not eliminate the boson structure. We find a robust peak in I2χ(ω)I^2\chi(\omega) centered about ΩR\Omega_R \cong 8.0 meV or 5.3 kBTck_B T_c (with Tc=T_c = 17.6 K). Its position in energy agrees well with a similar structure seen in scanning tunneling spectroscopy (STS). There is also a peak in the inelastic neutron scattering (INS) data at this same energy. This peak is found to persist in the normal state at T=T = 23 K. There is evidence that the superconducting gap is anisotropic as was also found in low temperature angular resolved photoemission (ARPES) data.Comment: 17 pages, 6 figure

    Weakly Supervised Localization using Deep Feature Maps

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    Object localization is an important computer vision problem with a variety of applications. The lack of large scale object-level annotations and the relative abundance of image-level labels makes a compelling case for weak supervision in the object localization task. Deep Convolutional Neural Networks are a class of state-of-the-art methods for the related problem of object recognition. In this paper, we describe a novel object localization algorithm which uses classification networks trained on only image labels. This weakly supervised method leverages local spatial and semantic patterns captured in the convolutional layers of classification networks. We propose an efficient beam search based approach to detect and localize multiple objects in images. The proposed method significantly outperforms the state-of-the-art in standard object localization data-sets with a 8 point increase in mAP scores

    Raman Scattering Study of the Lattice Dynamics of Superconducting LiFeAs

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    We report an investigation of the lattice dynamical properties of LiFeAs using inelastic light scattering. Five out of the six expected phonon modes are observed. The temperature evolution of their frequencies and linewidths is in good agreement with an anharmonic-decay model. We find no evidence for substantial electron-phonon coupling, and no superconductivity-induced phonon anomalies.Comment: 5 pages, 3 figures, 1 tabl
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