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Lsmo Energy Band Diagram Thickness Switching (color Online)

Extended 2θ-θ profiles of the LSMO (110), (111) and (001) phases in

Lsmo band Loss component χ 1 of the lsmo films of thickness (a) 40 nm, (b) 15 nm Modelled room-temperature spectra of the lsmo nanoceramics (cs-lsmo

Extended 2θ-θ profiles of the LSMO (110), (111) and (001) phases in

Complete band diagram of lsmo film. Extended 2θ-θ profiles of the lsmo (110), (111) and (001) phases in Temperature-dependent transport property of strained lsmo(8/2) films

Charge transfer at the lsmo/l‐lno interface. a) electron energy loss

Electron lsmo transmission dependence nanoscaleBand energy structure calculated for lsmo/lao/sto; a) spin-majority Structural characterizations of the lsmo/lco sls. a surface morphology(a) resistive switching curves for lsmo/pzt/lsmo junctions with 2.5 nm.

The thickness dependence of t p measured from the lsmo films grown onTemperature dependence of electrical and mechanical properties of lsmo (color online) high temperature dc-resistivity of lsmo (upper panel(a)-(f ) schematic process °ow for the fabrication of lsmo electrodes.

Extended 2θ-θ profiles of the LSMO (110), (111) and (001) phases in
Extended 2θ-θ profiles of the LSMO (110), (111) and (001) phases in

Crystal and band structures of lsmo/nno bilayers. (a) schematic view of

Schematic electron dos of the lsmo/si heterojunctions and the energy(a) energy band diagram at thermal equilibrium of pzt/lsmo interface Energy dependence of hot electron transmission in lsmo at theDependence lsmo thickness.

(a) thickness dependence of the total change of magnetization in lsmoStrain dependent reverse transition from bm-lsmo to pv-lsmo under Complete band diagram of lsmo film.Thickness dependence of conduction and field effect in rnio3/lsmo.

Temperature dependence of the magnetization for LSMO-AC sample (a) and
Temperature dependence of the magnetization for LSMO-AC sample (a) and

Magnetic behaviors of the lsmo/l‐lno bilayers. a) temperature‐dependent

(color online) schematic phase diagram of a lsmo-032 single crystalLsmo schematic phase Temperature dependence of the magnetization for lsmo-ac sample (a) andGround state geometry and magnetic structure of lsmo/ymo....

Mr for a lsmo–cnt–lsmo device.data recorded at 5 k with a bias voltageMagnetization curves of the initial lsmo particles and sintered Magnetic properties of [2 lsco/n lsmo] x heterostructures as a functionA) resistance switching from the on to the off state in the.

(a) Thickness dependence of the total change of magnetization in LSMO
(a) Thickness dependence of the total change of magnetization in LSMO

[pdf] structure and magnetism of lsmo/bto/mgo/lsmo multilayers

Lsmo (la1−xsrxmno3) pld targets for quality thin films – target materialsLsmo lco Electrical and magnetization properties of lsmo/lto/sto andSchematic sketch of the lsmo/bto/lsmo memristor with a mn⁴⁺ ↔ mn³.

Comparison of the band structure near e f of lsmoPhase diagram and structural characterization of lsmo homojunctions. a .

Thickness dependence of conduction and field effect in RNiO3/LSMO
Thickness dependence of conduction and field effect in RNiO3/LSMO
Modelled room-temperature spectra of the LSMO nanoceramics (CS-LSMO
Modelled room-temperature spectra of the LSMO nanoceramics (CS-LSMO
Loss component χ 1 of the LSMO films of thickness (a) 40 nm, (b) 15 nm
Loss component χ 1 of the LSMO films of thickness (a) 40 nm, (b) 15 nm
Complete band diagram of LSMO film. | Download Scientific Diagram
Complete band diagram of LSMO film. | Download Scientific Diagram
a) Resistance switching from the ON to the OFF state in the
a) Resistance switching from the ON to the OFF state in the
Schematic electron DOS of the LSMO/Si heterojunctions and the energy
Schematic electron DOS of the LSMO/Si heterojunctions and the energy
MR for a LSMO–CNT–LSMO device.Data recorded at 5 K with a bias voltage
MR for a LSMO–CNT–LSMO device.Data recorded at 5 K with a bias voltage
Charge transfer at the LSMO/L‐LNO interface. a) Electron energy loss
Charge transfer at the LSMO/L‐LNO interface. a) Electron energy loss
Magnetic properties of [2 LSCO/N LSMO] x heterostructures as a function
Magnetic properties of [2 LSCO/N LSMO] x heterostructures as a function

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