Dependence lsmo thickness (color online) schematic phase diagram of a lsmo-032 single crystal [pdf] structure and magnetism of lsmo/bto/mgo/lsmo multilayers
(a) Thickness dependence of the total change of magnetization in LSMO
Schematic sketch of the lsmo/bto/lsmo memristor with a mn⁴⁺ ↔ mn³ Lsmo lco Temperature dependence of the magnetization for lsmo-ac sample (a) and
Magnetization curves of the initial lsmo particles and sintered
Band energy structure calculated for lsmo/lao/sto; a) spin-majority(color online) high temperature dc-resistivity of lsmo (upper panel Energy dependence of hot electron transmission in lsmo at theTemperature-dependent transport property of strained lsmo(8/2) films.
Lsmo (la1−xsrxmno3) pld targets for quality thin films – target materialsComplete band diagram of lsmo film. Strain dependent reverse transition from bm-lsmo to pv-lsmo underComplete band diagram of lsmo film..
![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)
(a) thickness dependence of the total change of magnetization in lsmo
Comparison of the band structure near e f of lsmoMr 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 lossMagnetic properties of [2 lsco/n lsmo] x heterostructures as a function.
Phase diagram and structural characterization of lsmo homojunctions. aA) resistance switching from the on to the off state in the Crystal and band structures of lsmo/nno bilayers. (a) schematic view ofElectron lsmo transmission dependence nanoscale.
![(a) Energy band diagram at thermal equilibrium of PZT/LSMO interface](https://i2.wp.com/www.researchgate.net/profile/Er-Jia-Guo/publication/272829220/figure/download/fig6/AS:640237969620992@1529656035487/a-Energy-band-diagram-at-thermal-equilibrium-of-PZT-LSMO-interface-where-w-PZT-are-the.png)
Ground state geometry and magnetic structure of lsmo/ymo...
(a)-(f ) schematic process °ow for the fabrication of lsmo electrodesThe thickness dependence of t p measured from the lsmo films grown on Thickness dependence of conduction and field effect in rnio3/lsmo(a) resistive switching curves for lsmo/pzt/lsmo junctions with 2.5 nm.
Temperature dependence of electrical and mechanical properties of lsmoModelled room-temperature spectra of the lsmo nanoceramics (cs-lsmo Lsmo bandSchematic 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)
(a) energy band diagram at thermal equilibrium of pzt/lsmo interface
Structural characterizations of the lsmo/lco sls. a surface morphologyLoss component χ 1 of the lsmo films of thickness (a) 40 nm, (b) 15 nm Electrical and magnetization properties of lsmo/lto/sto andMagnetic behaviors of the lsmo/l‐lno bilayers. a) temperature‐dependent.
Extended 2θ-θ profiles of the lsmo (110), (111) and (001) phases inLsmo schematic phase .
![Phase diagram and structural characterization of LSMO homojunctions. a](https://i2.wp.com/www.researchgate.net/publication/361926360/figure/fig1/AS:11431281082481885@1662037387792/Phase-diagram-and-structural-characterization-of-LSMO-homojunctions-a-Bulk-phase.png)
![(a)-(f ) Schematic process °ow for the fabrication of LSMO electrodes](https://i2.wp.com/www.researchgate.net/profile/Shengwei-Jiang/publication/273934399/figure/fig2/AS:569046832816129@1512682745807/a-f-Schematic-process-ow-for-the-fabrication-of-LSMO-electrodes-g-SEM-images-of.png)
(a)-(f ) Schematic process °ow for the fabrication of LSMO electrodes
![(a) Thickness dependence of the total change of magnetization in LSMO](https://i2.wp.com/www.researchgate.net/profile/H-F-Ding/publication/257951543/figure/fig1/AS:317400470835206@1452685577847/a-Thickness-dependence-of-the-total-change-of-magnetization-in-LSMO-films-measured-over_Q320.jpg)
(a) Thickness dependence of the total change of magnetization in LSMO
Crystal and band structures of LSMO/NNO bilayers. (a) Schematic view of
![Charge transfer at the LSMO/L‐LNO interface. a) Electron energy loss](https://i2.wp.com/www.researchgate.net/publication/358961907/figure/fig3/AS:11431281179400129@1691182465064/Charge-transfer-at-the-LSMO-L-LNO-interface-a-Electron-energy-loss-spectra-with-an.png)
Charge transfer at the LSMO/L‐LNO interface. a) Electron energy loss
![The thickness dependence of T p measured from the LSMO films grown on](https://i2.wp.com/www.researchgate.net/publication/243410487/figure/fig4/AS:667779363516417@1536222415066/The-thickness-dependence-of-T-p-measured-from-the-LSMO-films-grown-on-LSAT0-0-1-and.png)
The thickness dependence of T p measured from the LSMO films grown on
![Temperature-dependent transport property of strained LSMO(8/2) films](https://i2.wp.com/www.researchgate.net/publication/335356424/figure/fig5/AS:11431281208229857@1701384124999/Temperature-dependent-transport-property-of-strained-LSMO8-2-films-a-Electrical.jpg)
Temperature-dependent transport property of strained LSMO(8/2) films
![Complete band diagram of LSMO film. | Download Scientific Diagram](https://i2.wp.com/www.researchgate.net/publication/277897548/figure/fig12/AS:1088556651024434@1636543538755/Complete-band-diagram-of-LSMO-film.jpg)
Complete band diagram of LSMO film. | Download Scientific Diagram
![Loss component χ 1 of the LSMO films of thickness (a) 40 nm, (b) 15 nm](https://i2.wp.com/www.researchgate.net/profile/Andriy-Lotnyk/publication/231103133/figure/fig1/AS:340588143628298@1458213949845/Loss-component-ch-1-of-the-LSMO-films-of-thickness-a-40-nm-b-15-nm-and-c-5-nm-T-S.png)
Loss component χ 1 of the LSMO films of thickness (a) 40 nm, (b) 15 nm