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      Raman scattering study of Spin-Density-Wave order and electron-phonon coupling in Ba(Fe\(_{1-x}\)Co\(_x\))\(_2\)As\(_2\)

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          Abstract

          We report Raman scattering measurements on iron-pnictide superconductor Ba(Fe\(_{1-x}\)Co\(_x\))\(_2\)As\(_2\) single crystals with varying cobalt \(x\) content. The electronic Raman continuum shows a strong spectral weight redistribution upon entering the magnetic phase induced by the opening of the Spin Density Wave (SDW) gap. It displays two spectral features that weaken with doping, which are assigned to two SDW induced electronic transitions. Raman symmetry arguments are discussed to identify the origin of these electronic transitions in terms of orbital ordering in the magnetic phase. Our data do not seem consistent with an orbital ordering scenario and advocate for a more conventional band-folding picture with two types of electronic transitions in the SDW state, a high energy transition between two anti-crossed SDW bands and a lower energy transition involving a folded band that do not anti-cross in the SDW state. The latter transition could be linked to the presence of Dirac cones in the electronic dispersion of the magnetic state. The spectra in the SDW state also show significant coupling between the arsenide optical phonon and the electronic continuum. The symmetry dependence of the arsenide phonon intensity indicates a strong in-plane anisotropy of the dielectric susceptibility in the magnetic state.

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          Is LaO\(_{1-x}\)F\(_x\)FeAs an electron-phonon superconductor ?

          In this paper we calculate the electron-phonon coupling of the newly-discovered superconductor LaO\(_{1-x}\)F\(_x\)FeAs from first-principles, using Density Functional Perturbation Theory. For pure LaOFeAs, the calculated electron-phonon coupling constant \(\lambda=0.21\) and logarithmic-averaged frequency \(\omega_{ln}=206 K\), give a maximum \(T_c\) of 0.8 K, using the standard Migdal-Eliashberg theory. For the \(F-\)doped compounds, we predict even smaller coupling constants, due to the strong suppression of the electronic Density of States at the Fermi level. To reproduce the experimental \(T_c=26 K\), a 5-6 times larger coupling constant would be needed. Our results indicate that electron-phonon coupling is not sufficient to explain superconductivity in the newly-discovered LaO\(_{1-x}\)F\(_x\)FeAs superconductor, probably due to the importance of strong correlation effects.
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            Effects of Co substitution on thermodynamic and transport properties and anisotropic \(H_{c2}\) in Ba(Fe\(_{1-x}\)Co\(_x\))\(_2\)As\(_2\) single crystals

            Single crystalline samples of Ba(Fe\(_{1-x}\)Co\(_x\))\(_2\)As\(_2\) with \(x < 0.12\) have been grown and characterized via microscopic, thermodynamic and transport measurements. With increasing Co substitution, the thermodynamic and transport signatures of the structural (high temperature tetragonal to low temperature orthorhombic) and magnetic (high temperature non magnetic to low temperature antiferromagnetic) transitions are suppressed at a rate of roughly 15 K per percent Co. In addition, for \(x \ge 0.038\) superconductivity is stabilized, rising to a maximum \(T_c\) of approximately 23 K for \(x \approx 0.07\) and decreasing for higher \(x\) values. The \(T - x\) phase diagram for Ba(Fe\(_{1-x}\)Co\(_x\))\(_2\)As\(_2\) indicates that either superconductivity can exist in both low temperature crystallographic phases or that there is a structural phase separation. Anisotropic, superconducting, upper critical field data (\(H_{c2}(T)\)) show a significant and clear change in anisotropy between samples that have higher temperature structural phase transitions and those that do not. These data show that the superconductivity is sensitive to the suppression of the higher temperature phase transition.
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              Magnetic order in BaFe2As2, the parent compound of the FeAs based superconductors in a new structural family

              In addition to higher Tc compared with the ubiquitous cuprates for a material composed of a single electronically active layer, the newly discovered LnFeAsO superconductors offer additional compositional variation. In a similar fashion to the CuO2 layers in cuprates, the FeAs layers now dominate the electronic states that produce superconductivity. Cuprate superconductors distinguish themselves structurally by adopting different stacking of the Cu-O and electronically inactive "spacer" layers. Using the same structural philosophy, materials with the formula (A,K)Fe2As2,A=Ba or Sr have been reported and possess a Tc~38 K. Here, we report the neutron diffraction studies of BaFe2As2 that shows, in contrast to previous studies on the LnFeAsO materials, an antiferromagnetic transition which concurs with first-order structural transition. Although the magnetic and structural transitions occur differently in the AFe2As2 and LnFeAsO-type materials, this work clearly demonstrates that the complete evolution to a low symmetry structure is a pre-requirement for the magnetic order.
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                Author and article information

                Journal
                01 June 2011
                2011-10-06
                Article
                10.1103/PhysRevB.84.104508
                1106.0231
                c0bcbef4-8c94-4f9e-95ca-e8f86310b787

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

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                Custom metadata
                Physical Review B 84, 104508 (2011)
                12 pages, 7 figures
                cond-mat.supr-con cond-mat.str-el

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