0000000000621368

AUTHOR

Julien Bok

showing 3 related works from this author

The effect of Cu substitution on the A1g mode of La(0.7)Sr(0.3)MnO3 manganites

2003

We report on the first Raman data of Cu substituted La(1-y)Sr(y)Mn(1-x)Cu(x)O3 (0 < x < 0.10 and 0.17 < y < 0.3, accordingly in order to have the same Mn(4+)/[Mn(4+)+Mn(3+)] ratio), collected in the frequency range 100-900 cm-1 and at room temperature, with parallel and crossed polarizations of the incident and scattered light. Spectra were fitted with a Drude-Lorentz model, and peaks at 190-220 and 430 cm-1, together with two broad structures centered at near 500 and 670 cm-1, have been found. We also have observed that the A1g mode is substantially shifted with increasing Cu substitution. The A1g phonon shift is a linear function of the tolerance factor t and the rhombohedral …

Condensed Matter - Materials ScienceMaterials sciencePhononAnalytical chemistryMaterials Science (cond-mat.mtrl-sci)FOS: Physical sciencesGeneral ChemistryTrigonal crystal systemCondensed Matter PhysicsSpectral linesymbols.namesakeOctahedronMaterials ChemistrysymbolsScattered lightRaman spectroscopy
researchProduct

Coulomb interaction in disordered metals and HTSC

2001

Abstract We consider underdoped or overdoped cuprates as disordered conductors. The diffusion coefficient D can be as low as 10 −5 m 2 s −1 . Under these conditions Coulomb interaction between electrons must be taken into account. The main effect is to open a dip in the density of state near the Fermi level. We show that this model explains most of the observed features of the so-called “pseudogap” in the normal state including its value, anisotropy and variation with doping. Such a model applied to disordered metals explains the dips observed in conductance measurements.

PhysicsCondensed matter physicsFermi levelEnergy Engineering and Power TechnologyElectronCondensed Matter PhysicsElectronic Optical and Magnetic Materialssymbols.namesakeCondensed Matter::SuperconductivityCoulombDensity of statessymbolsCondensed Matter::Strongly Correlated ElectronsCuprateElectrical and Electronic EngineeringDiffusion (business)PseudogapAnisotropyPhysica C: Superconductivity and its Applications
researchProduct

Effect ofA-site andB-site substitution on the infrared reflectivity spectra ofLa1−yAyMn1−xBxO3(A=Ba,Sr;B=Cu,Zn,Sc;0<y<~0.3;0<~x<~0.1)mang…

2003

We have measured the infrared reflectivity spectra of ${\mathrm{La}}_{1\ensuremath{-}y}[\mathrm{Sr}(\mathrm{Ba}){]}_{y}{\mathrm{Mn}}_{1\ensuremath{-}x}[\mathrm{Cu}(\mathrm{Zn},\mathrm{Sc}){]}_{x}{\mathrm{O}}_{3}$ $(0lyl~0.3,0l~xl~0.10)$ manganites, in a wide frequency $(100\char21{}4000{\mathrm{cm}}^{\ensuremath{-}1})$ and temperature (80 K\char21{}300 K) range. The reflectivity spectra were analyzed by a fitting procedure based on a model that includes Drude, midinfrared electronic, and phonon oscillator contributions to the dielectric constant. Six infrared active ${(3A}_{u}$ and ${3E}_{u})$ modes of rhombohedral symmetry are clearly observed. We assigned all observed modes according to e…

PhysicsCondensed Matter::Materials ScienceCrystallographyNuclear magnetic resonanceInfraredPhononLattice (order)Infrared reflectivityCondensed Matter::Strongly Correlated ElectronsDielectricTrigonal crystal systemReflectivitySpectral linePhysical Review B
researchProduct