84 research outputs found

    Spectral weight redistribution in (LaNiO3)n/(LaMnO3)2 superlattices from optical spectroscopy

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    We have studied the optical properties of four (LaNiO3_3)n_n/(LaMnO3_3)2_2 superlattices (SL) (nn=2, 3, 4, 5) on SrTiO3_3 substrates. We have measured the reflectivity at temperatures from 20 K to 400 K, and extracted the optical conductivity through a fitting procedure based on a Kramers-Kronig consistent Lorentz-Drude model. With increasing LaNiO3_3 thickness, the SLs undergo an insulator-to-metal transition (IMT) that is accompanied by the transfer of spectral weight from high to low frequency. The presence of a broad mid-infrared band, however, shows that the optical conductivity of the (LaNiO3_3)n_n/(LaMnO3_3)2_2 SLs is not a linear combination of the LaMnO3_3 and LaNiO3_3 conductivities. Our observations suggest that interfacial charge transfer leads to an IMT due to a change in valence at the Mn and Ni sites.Comment: Accepted for publication in Phys. Rev. Lett. 5 pages, 5 figure

    Metallic ground state and glassy transport in single crystalline URh2_2Ge2_2: Enhancement of disorder effects in a strongly correlated electron system

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    We present a detailed study of the electronic transport properties on a single crystalline specimen of the moderately disordered heavy fermion system URh2_2Ge2_2. For this material, we find glassy electronic transport in a single crystalline compound. We derive the temperature dependence of the electrical conductivity and establish metallicity by means of optical conductivity and Hall effect measurements. The overall behavior of the electronic transport properties closely resembles that of metallic glasses, with at low temperatures an additional minor spin disorder contribution. We argue that this glassy electronic behavior in a crystalline compound reflects the enhancement of disorder effects as consequence of strong electronic correlations.Comment: 5 pages, 4 figures, accepted for publication in PR

    Evidence of a pressure-induced metallization process in monoclinic VO2_2

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    Raman and combined trasmission and reflectivity mid infrared measurements have been carried out on monoclinic VO2_2 at room temperature over the 0-19 GPa and 0-14 GPa pressure ranges, respectively. The pressure dependence obtained for both lattice dynamics and optical gap shows a remarkable stability of the system up to P*∼\sim10 GPa. Evidence of subtle modifications of V ion arrangements within the monoclinic lattice together with the onset of a metallization process via band gap filling are observed for P>>P*. Differently from ambient pressure, where the VO2_2 metal phase is found only in conjunction with the rutile structure above 340 K, a new room temperature metallic phase coupled to a monoclinic structure appears accessible in the high pressure regime, thus opening to new important queries on the physics of VO2_2.Comment: 5 pages, 3 figure

    Electrodynamics of superconducting pnictide superlattices

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    It has been recently reported (S. Lee et al., Nature Materials 12, 392, 2013) that superlattices where layers of the 8% Co-doped BaFe2As2 superconducting pnictide are intercalated with non superconducting ultrathin layers of either SrTiO3 or of oxygen-rich BaFe2As2, can be used to control flux pinning, thereby increasing critical fields and currents, without significantly affecting the critical temperature of the pristine superconducting material. However, little is known about the electron properties of these systems. Here we investigate the electrodynamics of these superconducting pnictide superlattices in the normal and superconducting state by using infrared reflectivity, from THz to visible range. We find that multi-gap structure of these superlattices is preserved, whereas some significant changes are observed in their electronic structure with respect to those of the original pnictide. Our results suggest that possible attempts to further increase the flux pinning may lead to a breakdown of the pnictide superconducting properties.Comment: 4 pages, two figure

    Pressure dependence of the single particle excitation in the charge-density-wave CeTe3_3 system

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    We present new data on the pressure dependence at 300 K of the optical reflectivity of CeTe3_3, which undergoes a charge-density-wave (CDW) phase transition well above room temperature. The collected data cover an unprecedented broad spectral range from the infrared up to the ultraviolet, which allows a robust determination of the gap as well as of the fraction of the Fermi surface affected by the formation of the CDW condensate. Upon compressing the lattice there is a progressive closing of the gap inducing a transfer of spectral weight from the gap feature into the Drude component. At frequencies above the CDW gap we also identify a power-law behavior, consistent with findings along the RRTe3_3 series (i.e., chemical pressure) and suggestive of a Tomonaga-Luttinger liquid scenario at high energy scales. This newest set of data is placed in the context of our previous investigations of this class of materials and allows us to revisit important concepts for the physics of CDW state in layered-like two-dimensional systems

    Incommensurate magnetism in the coupled spin tetrahedra system Cu2Te2O5Cl2

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    Neutron scattering studies on powder and single crystals have provided new evidences for unconventional magnetism in Cu2Te2O5Cl2. The compound is built from tetrahedral clusters of S=1/2 Cu2+ spins located on a tetragonal lattice. Magnetic ordering, emerging at TN=18.2 K, leads to a very complex multi-domain, most likely degenerate, ground state, which is characterized by an incommensurate (ICM) wave vector k ~ [0.15, 0.42,1/2]. The Cu2+ ions carry a magnetic moment of 0.67(1) mB/ Cu2+ at 1.5 K and form a four helices spin arrangement with two canted pairs within the tetrahedra. A domain redistribution is observed when a magnetic field is applied in the tetragonal plane (Hc≈0.5 T), but not for H||c up to 4 T. The excitation spectrum is characterized by two well-defined modes, one completely dispersionless at 6.0 meV, the other strongly dispersing to a gap of 2 meV. The reason for such complex ground state and spin excitations may be geometrical frustration of the Cu2+ spins within the tetrahedra, intra- and inter-tetrahedral couplings having similar strengths and strong Dzyaloshinski-Moriya anisotropy. Candidates for the dominant intra- and inter-tetrahedral interactions are proposed

    Optical investigation of the charge-density-wave phase transitions in NbSe3NbSe_{3}

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    We have measured the optical reflectivity R(ω)R(\omega) of the quasi one-dimensional conductor NbSe3NbSe_{3} from the far infrared up to the ultraviolet between 10 and 300 KK using light polarized along and normal to the chain axis. We find a depletion of the optical conductivity with decreasing temperature for both polarizations in the mid to far-infrared region. This leads to a redistribution of spectral weight from low to high energies due to partial gapping of the Fermi surface below the charge-density-wave transitions at 145 K and 59 K. We deduce the bulk magnitudes of the CDW gaps and discuss the scattering of ungapped free charge carriers and the role of fluctuations effects

    Multi-gap superconductivity in a BaFe1.84Co0.16As2 film from optical measurements at terahertz frequencies

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    We measured the THz reflectance properties of a high quality epitaxial thin film of the Fe-based superconductor BaFe1.84_{1.84}Co0.16_{0.16}As2_2 with Tc_c=22.5 K. The film was grown by pulsed laser deposition on a DyScO3_3 substrate with an epitaxial SrTiO3_3 intermediate layer. The measured RS/RNR_S/R_N spectrum, i.e. the reflectivity ratio between the superconducting and normal state reflectance, provides clear evidence of a superconducting gap ΔA\Delta_A close to 15 cm−1^{-1}. A detailed data analysis shows that a two-band, two-gap model is absolutely necessary to obtain a good description of the measured RS/RNR_S/R_N spectrum. The low-energy ΔA\Delta_A gap results to be well determined (ΔA\Delta_A=15.5±\pm0.5 cm−1^{-1}), while the value of the high-energy gap ΔB\Delta_B is more uncertain (ΔB\Delta_B=55±\pm7 cm−1^{-1}). Our results provide evidence of a nodeless isotropic double-gap scenario, with the presence of two optical gaps corresponding to 2Δ/kTc\Delta/kT_c values close to 2 and 7.Comment: Published Versio
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