Search results for "Residual resistivity"

showing 8 items of 8 documents

Conductivity of the two-dimensional electron gas atLaAlO3/SrTiO3interface

2017

We propose an analytical theory of metallic conductivity in the two-dimensional (2D) ${\mathrm{LaAlO}}_{3}/{\mathrm{SrTiO}}_{3}$ (LAO/STO) interface. For that we consider the electron-phonon interaction at the interface. The electronic part is taken from our previous work [Phys. Chem. Chem. Phys. 18, 2104 (2016)], considering the conditions for the interfacial charge carrier (electron or hole) to become itinerant. The second ingredient deals with the atomic oscillations localized near the interface and decaying rapidly at its both sides, which can be regarded as 2D acoustic phonons. The dispersion of such phonons depends on the characteristics of phonon spectra of LAO and STO. Calculating t…

Materials scienceCondensed matter physicsPhononInverseElectronConductivity01 natural sciences010305 fluids & plasmasResidual resistivityElectrical resistivity and conductivityScattering rate0103 physical sciencesCharge carrier010306 general physicsPhysical Review B
researchProduct

Finite range scattering of Ni and Zn impurities in Y-123 thin films

1997

Abstract We investigated YBa 2 (Cu 1− z M z ) 3 O 7-δ (M Ni,Zn) thin films and determined the decrease of T c and the increase of residual resistivity due to Cu-site substitution, taking into account the CuO-chain contributions to the total conductivity. Although Zn suppresses T c stronger than Ni by a factor of 2.3 the increase of resistivity differs only slightly. Furthermore the observed resistivities are too high to be explained within scattering from point-like defects. To reconcile these contradictions, we assumed finite size scattering potentials, which lead to scattering phase shifts δ l of higher angular momebtum l > 0. T c -suppression is discussed qalitatively within this picture.

Materials scienceCondensed matter physicsScatteringEnergy Engineering and Power TechnologyConductivityCondensed Matter PhysicsFinite rangeElectronic Optical and Magnetic MaterialsResidual resistivityImpurityElectrical resistivity and conductivityPhase (matter)Electrical and Electronic EngineeringThin filmPhysica C: Superconductivity
researchProduct

Zero Temperature Magnetoresistance of the HF Metal: Enigma of $$\mathrm{Sr}_{3}\mathrm{Ru}_{2}\mathrm{O}_{7}$$

2014

To understand the nature of field-tuned metamagnetic quantum criticality in the ruthenate \(\mathrm{Sr}_{3}\mathrm{Ru}_{2}\mathrm{O}_{7}\) is one of the significant challenges in the condensed matter physics. It is established experimentally that the entropy has a peak in the ordered phase. It is unexpectedly higher than that outside latter phase, while the magnetoresistivity varies abruptly near the ordered phase boundary. We demonstrate unexpected similarity between \(\mathrm{Sr}_{3}\mathrm{Ru}_{2}\mathrm{O}_{7}\) and HF metals expressing universal physics that transcends microscopic details. Our \(T-B\) phase diagram of \(\mathrm{Sr}_{3}\mathrm{Ru}_{2}\mathrm{O}_{7}\) explains main featu…

PhysicsMetalResidual resistivityPhase boundaryCrystallographyMagnetoresistanceRestricted rangevisual_artvisual_art.visual_art_mediumFlat bandZero temperaturePhase diagram
researchProduct

Influence of disorder on anomalous Hall effect for Heusler compounds

2011

The anomalous Hall effect (AHE) is a long known but still not fully understood transport effect. Most theory papers focus on the influence of one particular contribution to the AHE. Actual measured experimental data, however, often are not in accord with idealized assumptions. In this work we discuss the data analysis for materials with low residual resistivity ratios. As prototypical materials we study half metallic Heusler compounds. Here the influence of defects and disorder is apparent in a material with a complex topology of the Fermi surface. Using films of different degree of disorder, we show how different scattering mechanisms can be separated. For ${\text{Co}}_{2}{\text{FeSi}}_{0.…

PhysicsResidual resistivityCondensed matter physicsDegree (graph theory)Hall effectScatteringTransport effectFermi surfaceQuantum Hall effectCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsPhysical Review B
researchProduct

Violation of the Wiedemann-Franz Law in HF Metals

2014

Experimental observations of the much-studied compounds CeCoIn\(_5\) and YbRh\(_2\)Si\(_2\) at vanishing temperatures carefully probe the nature of their magnetic-field-tuned QCPs. The violation of Wiedemann-Franz (WF) law, along with jumps revealed both in the residual resistivity \(\rho _0\) and the Hall resistivity \(R_H\), provide vital clues to the origin of their non-Fermi-liquid behavior. The empirical facts point unambiguously to association of the observed QCP with FC forming flat bands.

PhysicsResidual resistivityCondensed matter physicsElectrical resistivity and conductivitySeebeck coefficientLorenz numberFermi liquid theoryFlat bandWiedemann–Franz lawPhase diagram
researchProduct

Metals with a Strongly Correlated Electron Liquid

2014

In this chapter, we consider the main properties of strongly correlated Fermi systems, which are formed by the fermion condensate leading to the emergence of flat bands. Namely, we consider the residual entropy \(S_0\) related to the flat bands that leads to the violation of the quasiparticle—hole symmetry. The presence of \(S_0\) has a profound impact on the universality of second order phase transitions. In that case under the application of magnetic field the curve of the second order AF phase transitions passes into a curve of the first order ones at the tricritical point, thus leading to a violation of the critical universality of the fluctuation theory. We demonstrate that a jump in t…

Quantum phase transitionPhysicsPhase transitionResidual resistivityTricritical pointCondensed matter physicsmedia_common.quotation_subjectElectron liquidFermionResidual entropyAsymmetrymedia_common
researchProduct

Effect of disorder produced by cationic vacancies at theBsites on the electronic properties of mixed valence manganites

1999

An alloy series of single-phased polycrystalline ${\mathrm{La}}_{1\ensuremath{-}x}{\mathrm{Na}}_{x}{\mathrm{MnO}}_{3+\mathrm{\ensuremath{\delta}}} (0l~xl~0.15)$ has been synthesized in order to study the effect of disorder on the electronic properties of mixed valence manganites. The synthetic variables allow one to maintain a constant proportion of ${\mathrm{Mn}}^{4+}$ in the samples $({\mathrm{Mn}}^{3+}{/\mathrm{M}\mathrm{n}}^{4+}=2.1\ifmmode\pm\else\textpm\fi{}0.2),$ while the similar size of ${\mathrm{La}}^{3+}$ and ${\mathrm{Na}}^{+}$ ions results in no appreciable change in the tolerance factor of the perovskite structure throughout the series. In this way, the sodium content x contro…

Residual resistivityParamagnetismValence (chemistry)Materials scienceCondensed matter physicsElectrical resistivity and conductivitySeebeck coefficientTransition temperatureElectronic band structurePolaronPhysical Review B
researchProduct

Magnetoresistance in the HF Metal at Zero Temperature

2014

In this chapter we consider the paradoxical behavior of the residual resistivity \(\rho _0\) of HF metals in magnetic fields and under pressure. Our consideration is based on the idea of flattening of the single-particle spectrum \(\varepsilon (\mathbf{p})\) that profoundly effects on the specific heat \(C\), thermal expansion coefficient \(\alpha \) and magnetic susceptibility \(\chi \) in the normal state, the jump of \(C\) at the point of superconducting phase transition etc. We show that FC associated with flat bands contributes to the residual resistivity \(\rho _0\), while the application of the magnetic field or pressure to the system with a flat band removes the flat band and leads …

SuperconductivityPhysicsResidual resistivityPhase transitionColossal magnetoresistanceEffective mass (solid-state physics)Condensed matter physicsMagnetoresistanceFermi surfaceMagnetic susceptibility
researchProduct