(color online) high temperature dc-resistivity of lsmo (upper panel Lsmo band (a)-(f ) schematic process °ow for the fabrication of lsmo electrodes lsmo energy band diagram thickness switching
Schematic sketch of the LSMO/BTO/LSMO memristor with a Mn⁴⁺ ↔ Mn³
(color online) schematic phase diagram of a lsmo-032 single crystal Electrical and magnetization properties of lsmo/lto/sto and Schematic electron dos of the lsmo/si heterojunctions and the energy
Magnetic properties of [2 lsco/n lsmo] x heterostructures as a function
Lsmo (la1−xsrxmno3) pld targets for quality thin films – target materials(a) resistive switching curves for lsmo/pzt/lsmo junctions with 2.5 nm Crystal and band structures of lsmo/nno bilayers. (a) schematic view ofLsmo lco.
Magnetic behaviors of the lsmo/l‐lno bilayers. a) temperature‐dependentElectron lsmo transmission dependence nanoscale Lsmo schematic phase(a) energy band diagram at thermal equilibrium of pzt/lsmo interface.

Mr for a lsmo–cnt–lsmo device.data recorded at 5 k with a bias voltage
Dependence lsmo thickness(a) thickness dependence of the total change of magnetization in lsmo Temperature dependence of electrical and mechanical properties of lsmoMagnetization curves of the initial lsmo particles and sintered.
Complete band diagram of lsmo film.Loss component χ 1 of the lsmo films of thickness (a) 40 nm, (b) 15 nm Energy dependence of hot electron transmission in lsmo at theStrain dependent reverse transition from bm-lsmo to pv-lsmo under.
Ground state geometry and magnetic structure of lsmo/ymo...
Comparison of the band structure near e f of lsmoPhase diagram and structural characterization of lsmo homojunctions. a Complete band diagram of lsmo film.Band energy structure calculated for lsmo/lao/sto; a) spin-majority.
Extended 2θ-θ profiles of the lsmo (110), (111) and (001) phases inTemperature-dependent transport property of strained lsmo(8/2) films Schematic sketch of the lsmo/bto/lsmo memristor with a mn⁴⁺ ↔ mn³A) resistance switching from the on to the off state in the.

Modelled room-temperature spectra of the lsmo nanoceramics (cs-lsmo
Thickness dependence of conduction and field effect in rnio3/lsmoTemperature dependence of the magnetization for lsmo-ac sample (a) and [pdf] structure and magnetism of lsmo/bto/mgo/lsmo multilayersThe thickness dependence of t p measured from the lsmo films grown on.
Charge transfer at the lsmo/l‐lno interface. a) electron energy lossStructural characterizations of the lsmo/lco sls. a surface morphology .








