Data for Colossal terahertz magnetoresistance at room temperature in epitaxial La0.7Sr0.3MnO3 nanocomposites and single-phase thin films

This suggests that colossal magnetoresistance at THz frequencies may find use in nanoelectronics and in THz optical components controlled by magnetic fields. The VAN can be scaled in thickness while retaining a high structural quality, and offers a larger THz CMR at room temperature than the planar film.<br><br>figure1(c)-FC figure1(c)-FC-magnetisation-v-temperature figure1(c)-ZFC figure1(c)-ZFC, figure1(c)-ZFC-magnetisation-v-temperature figure2(a)-sigma1-v-frequency figure2(b)-dc-rho(10K)-rho(T)-v-temperature figure2(b)-sigma0-v-temperature figure3-(a)-VAN-sigma1-v-freq-at-B=0T-and-B=4T-T50K figure3-(b)-VAN-sigma1-v-freq-at-B=0T-T200K figure3-(b)-VAN-sigma1-v-freq-at-B=2T-T200K figure3-(b)-VAN-sigma1-v-freq-at-B=4T-T200K figure3-(b)-VAN-sigma1-v-freq-at-B=6T-T200K figure3-(b)-VAN-sigma1-v-freq-at-B=6T-T200K figure3-(b)-VAN-sigma1-v-freq-at-B=6T-T200K figure3-(c)-VAN-sigma1-v-freq-at-B=2T-T300K figure3-(c)-VAN-sigma1-v-freq-at-B=4T-T300K figure3-(c)-VAN-sigma1-v-freq-at-B=6T-T300K figure3-(c)-VAN-sigma1-v-freq-at-B=8T-T300K figure3-(d)-LSMO-sigma1-v-freq-at-B=0T-T300K figure3-(d)-LSMO-sigma1-v-freq-at-B=2T-T300K figure3-(d)-LSMO-sigma1-v-freq-at-B=4T-T300K figure3-(d)-LSMO-sigma1-v-freq-at-B=6T-T300K figure3-(d)-LSMO-sigma1-v-freq-at-B=8T-T300K