Abstract

The influence of the ${}^{16}\mathrm{O}{\ensuremath{-}}^{18}\mathrm{O}$ isotope substitutions on magnetic state of perovskite-type manganite $({\mathrm{La}}_{0.25}{\mathrm{Pr}}_{0.75}{)}_{0.7}{\mathrm{Ca}}_{0.3}{\mathrm{MnO}}_{3}$ is studied by ${}^{55}\mathrm{Mn}$ NMR. Successive cycling with an isochronal exposure at different magnetic fields up to $H=8T$ is used to study the field-induced transition from antiferromagnetic insulating (AFI) state to the ferromagnetic metal (FMM) one in the ${}^{18}\mathrm{O}$-enriched sample. After exposure at $Hg{H}_{\mathrm{cr}}\ensuremath{\sim}5.3T$ the NMR spectrum of the ${}^{18}\mathrm{O}$ sample provides evidence for a magnetic phase separation (PS) into the coexisting AFI and FMM domains. Further increase of exposing field leads to a progressive growth of the FMM phase at the expense of AFI domains. Its relative fraction can be controlled by external magnetic field and the resulting magnetic structure in the PS region is discussed. Anomalous T dependence of the ${}^{55}\mathrm{Mn}$ nuclear spin-lattice relaxation rate is revealed in the FMM state of both ${}^{16}\mathrm{O}$- and ${}^{18}\mathrm{O}$-enriched samples. The possible influence of the Pr magnetic ordering at $T\ensuremath{\sim}40\mathrm{K}$ on the spin-lattice relaxation is considered.

Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.