The anelastic spectrum (dynamic Young's modulus and elastic energy absorption) of La2CuO4+δ has been measured between 1 and 700 K with 0<δ<0.02. The spectrum of stoichiometric La2CuO4 in the low-temperature orthorhombic (LTO) phase is dominated by two intense relaxation processes which cause softenings of 16% around 150 K and 9% below 30 K at f∼1 kHz. The relaxation at 150 K is attributed to the presence of a fraction of the CuO6 octahedra which are able to change their tilted configuration by thermal activation between orientations which are nearly energetically equivalent, possibly within the twin boundaries. The relaxation below 30 K is governed by tunneling, and involves a considerable fraction of the lattice atoms. It is proposed that ...
Angular dependent x-ray absorption fine structure (XAFS) measurements of all La, Ba, and Cu sites de...
YBCO, LSCO and Ru-1212 have been extensively studied by measuring the complex dynamic Young's modulu...
The representative cuprate La2−xMxCuO4 with M=Sr and x=1/8 is studied via first-principles calculati...
The anelastic relaxation (elastic energy loss and Young modulus) of nearly stoichiometric La2CuO4+de...
NMR and NQR reveal substantial structural changes in the metallic phase of La2CuO4+δ which occur bel...
Heat capacity measurements from 150 to 300 K were carried out on a single crystal of La2CuO4+x synth...
The thermal expansion, α(T), of a La2CuO4 single crystal, measured along and perpendicular to the [0...
The enthalpies of transition among the Tx, T′, and T–La2CuO4 phases are obtained from a combination ...
We present results for the thermal expansion, α(T), of both polycrystalline and single crystalline L...
Definitive understanding of superconductivity and its interplay with structural symmetry in the hole...
We track the systematic variation in magnetic susceptibility (χ), thermal conductivity (κ), anisotro...
Resonant ultrasound spectroscopy is used to measure the temperature dependence of all six elastic mo...
The structure of oxygen-intercalated La(2)CuO(4.07) has been investigated at 20 and 300 K by neutron...
We have studied the local atomic structure of La{sub 2-x}A{sub x}CuO{sub 4} (A=Ba, Sr) through the h...
13 pages, 9 figuresInternational audienceWe study the zero-point and thermal ionic motion in La$_2$C...
Angular dependent x-ray absorption fine structure (XAFS) measurements of all La, Ba, and Cu sites de...
YBCO, LSCO and Ru-1212 have been extensively studied by measuring the complex dynamic Young's modulu...
The representative cuprate La2−xMxCuO4 with M=Sr and x=1/8 is studied via first-principles calculati...
The anelastic relaxation (elastic energy loss and Young modulus) of nearly stoichiometric La2CuO4+de...
NMR and NQR reveal substantial structural changes in the metallic phase of La2CuO4+δ which occur bel...
Heat capacity measurements from 150 to 300 K were carried out on a single crystal of La2CuO4+x synth...
The thermal expansion, α(T), of a La2CuO4 single crystal, measured along and perpendicular to the [0...
The enthalpies of transition among the Tx, T′, and T–La2CuO4 phases are obtained from a combination ...
We present results for the thermal expansion, α(T), of both polycrystalline and single crystalline L...
Definitive understanding of superconductivity and its interplay with structural symmetry in the hole...
We track the systematic variation in magnetic susceptibility (χ), thermal conductivity (κ), anisotro...
Resonant ultrasound spectroscopy is used to measure the temperature dependence of all six elastic mo...
The structure of oxygen-intercalated La(2)CuO(4.07) has been investigated at 20 and 300 K by neutron...
We have studied the local atomic structure of La{sub 2-x}A{sub x}CuO{sub 4} (A=Ba, Sr) through the h...
13 pages, 9 figuresInternational audienceWe study the zero-point and thermal ionic motion in La$_2$C...
Angular dependent x-ray absorption fine structure (XAFS) measurements of all La, Ba, and Cu sites de...
YBCO, LSCO and Ru-1212 have been extensively studied by measuring the complex dynamic Young's modulu...
The representative cuprate La2−xMxCuO4 with M=Sr and x=1/8 is studied via first-principles calculati...