Lsmo Energy Band Diagram Thickness Switching (color Online)
Complete band diagram of lsmo film. Temperature dependence of the magnetization for lsmo-ac sample (a) and Phase diagram and structural characterization of lsmo homojunctions. a
Energy dependence of hot electron transmission in LSMO at the
Dependence lsmo thickness (a) energy band diagram at thermal equilibrium of pzt/lsmo interface (a)-(f ) schematic process °ow for the fabrication of lsmo electrodes
The thickness dependence of t p measured from the lsmo films grown on
Extended 2θ-θ profiles of the lsmo (110), (111) and (001) phases inComparison of the band structure near e f of lsmo Energy dependence of hot electron transmission in lsmo at theMagnetic behaviors of the lsmo/l‐lno bilayers. a) temperature‐dependent.
Crystal and band structures of lsmo/nno bilayers. (a) schematic view ofStrain dependent reverse transition from bm-lsmo to pv-lsmo under Electrical and magnetization properties of lsmo/lto/sto andSchematic electron dos of the lsmo/si heterojunctions and the energy.
![Structural characterizations of the LSMO/LCO SLs. a Surface morphology](https://i2.wp.com/www.researchgate.net/publication/325155503/figure/fig4/AS:958862387576839@1605622016456/Effects-of-layer-thickness-on-magnetic-behaviors-for-LCO-LSMO-LCO-trilayers-a_Q640.jpg)
(color online) schematic phase diagram of a lsmo-032 single crystal
(a) thickness dependence of the total change of magnetization in lsmoElectron lsmo transmission dependence nanoscale Mr for a lsmo–cnt–lsmo device.data recorded at 5 k with a bias voltageStructural characterizations of the lsmo/lco sls. a surface morphology.
Ground state geometry and magnetic structure of lsmo/ymo...Thickness dependence of conduction and field effect in rnio3/lsmo Temperature dependence of electrical and mechanical properties of lsmoLsmo (la1−xsrxmno3) pld targets for quality thin films – target materials.
![Magnetization curves of the initial LSMO particles and sintered](https://i2.wp.com/www.researchgate.net/profile/Jan-Petzelt/publication/341918166/figure/fig4/AS:11431281110570767@1672657551864/a-DC-magnetic-susceptibility-of-LSMO-nanoparticles-and-LSMOTiO-2-ceramics-A-and-B-ZFC_Q640.jpg)
(color online) high temperature dc-resistivity of lsmo (upper panel
Lsmo schematic phaseModelled room-temperature spectra of the lsmo nanoceramics (cs-lsmo Lsmo lco[pdf] structure and magnetism of lsmo/bto/mgo/lsmo multilayers.
Loss component χ 1 of the lsmo films of thickness (a) 40 nm, (b) 15 nmCharge transfer at the lsmo/l‐lno interface. a) electron energy loss Temperature-dependent transport property of strained lsmo(8/2) filmsMagnetic properties of [2 lsco/n lsmo] x heterostructures as a function.
Lsmo band
Band energy structure calculated for lsmo/lao/sto; a) spin-majorityComplete band diagram of lsmo film. A) resistance switching from the on to the off state in the(a) resistive switching curves for lsmo/pzt/lsmo junctions with 2.5 nm.
Schematic sketch of the lsmo/bto/lsmo memristor with a mn⁴⁺ ↔ mn³Magnetization curves of the initial lsmo particles and sintered .
![Electrical and magnetization properties of LSMO/LTO/STO and](https://i2.wp.com/www.researchgate.net/publication/363846348/figure/fig2/AS:11431281086513520@1664247186536/Electrical-and-magnetization-properties-of-LSMO-LTO-STO-and-LSMO-LTO-LSAT-a-Temperature.png)
![Complete band diagram of LSMO film. | Download Scientific Diagram](https://i2.wp.com/www.researchgate.net/profile/Hyung_Ho_Park/publication/277897548/figure/download/fig5/AS:324069695213571@1454275644233/Complete-band-diagram-of-LSMO-film.png)
![Energy dependence of hot electron transmission in LSMO at the](https://i2.wp.com/www.researchgate.net/profile/Subir_Parui/publication/235690033/figure/fig3/AS:293970543431699@1447099447666/Energy-dependence-of-hot-electron-transmission-in-LSMO-at-the-nanoscale-a-Electron.png)
![MR for a LSMO–CNT–LSMO device.Data recorded at 5 K with a bias voltage](https://i2.wp.com/www.researchgate.net/profile/Miguel-Pruneda/publication/6551675/figure/fig3/AS:280368210038794@1443856398178/MR-for-a-LSMO-CNT-LSMO-deviceData-recorded-at-5-K-with-a-bias-voltage-of-25-mV-show-two.png)
![Temperature dependence of electrical and mechanical properties of LSMO](https://i2.wp.com/www.researchgate.net/publication/362520636/figure/fig4/AS:1186792275484675@1659964736423/Temperature-dependence-of-electrical-and-mechanical-properties-of-LSMO-micro-bridge.png)
![Modelled room-temperature spectra of the LSMO nanoceramics (CS-LSMO](https://i2.wp.com/www.researchgate.net/profile/Jan-Petzelt/publication/341918166/figure/fig9/AS:11431281110605224@1672657552213/Modelled-room-temperature-spectra-of-the-LSMO-nanoceramics-CS-LSMO-and-of-the-LSMOTiO.png)
![Extended 2θ-θ profiles of the LSMO (110), (111) and (001) phases in](https://i2.wp.com/www.researchgate.net/publication/258757414/figure/fig7/AS:612917233868801@1523142264373/Extended-2th-th-profiles-of-the-LSMO-110-111-and-001-phases-in-Figure-6-a-LSMO.png)
![Thickness dependence of conduction and field effect in RNiO3/LSMO](https://i2.wp.com/www.researchgate.net/publication/376453731/figure/fig4/AS:11431281211489169@1702439760800/Thickness-dependence-of-conduction-and-field-effect-in-RNiO3-LSMO-bilayer-channels-a.png)