Fig. 2: Electrical and magnetization properties of LSMO/LTO/STO and LSMO/LTO/LSAT. | Nature Communications

Fig. 2: Electrical and magnetization properties of LSMO/LTO/STO and LSMO/LTO/LSAT.

From: Giant spin-to-charge conversion at an all-epitaxial single-crystal-oxide Rashba interface with a strongly correlated metal interlayer

Fig. 2

a Temperature (T) dependence of the sheet resistance Rsheet of the LSMO (30 u.c.)/LTO (3 u.c.)/STO and the LSMO (30 u.c.)/LTO (3 u.c.)/LSAT samples. b T dependence of the magnetization M of LSMO (30 u.c.)/LTO (3 u.c.)/STO and LSMO (30 u.c.)/LTO (3 u.c.)/LSAT. The Curie temperatures of LSMO/LTO/STO and LSMO/LTO/LSAT are 320 and 340 K, respectively. c Magnetization M for LSMO (30 u.c.)/LTO (3 u.c.)/STO and LSMO (30 u.c.)/LTO (3 u.c.)/LSAT measured at 10 K as a function of a magnetic field H applied along the [110] direction of the STO substrate.

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