AVS 65th International Symposium & Exhibition | |
Actinides and Rare Earths Focus Topic | Wednesday Sessions |
Session AC+MI+SA-WeM |
Session: | Magnetism, Complexity, and Superconductivity in the Actinides and Rare Earths |
Presenter: | Navid Mottaghi, West Virginia University |
Authors: | N. Mottaghi, West Virginia University S. Seehra, West Virginia University R. Trappen, West Virginia University S. Kumari, West Virginia University C.-Y. Huang, West Virginia University S.F. Yousefi, West Virginia University G.B. Cabrera, West Virginia University A. Romero, West Virginia University M.B. Holcomb, West Virginia University |
Correspondent: | Click to Email |
Detailed dc magnetization (M) measurements of a 7.6 nm La0.7Sr0.3MnO3 thin film samples is investigated. The sample was fabricated by pulsed laser deposition. Zero-field-cooled (ZFC) M vs. applied field (H) cooled down to T = 5 K reveal the presence of negative remanent magnetization (NRM) as well as in ZFC M vs. temperature (T) measurements in H = 50 Oe and 100 Oe. ZFC and FC (field-cooled) protocols are used to determine the blocking temperature TB in different H. Isothermal hysteresis loops at different T are used to determine the temperature dependence of saturation magnetization (MS), remanence (MR) and coercivity HC. The MS vs. T data are fit to the Bloch law, MS (T) = M0 (1 – BT3/2), showing a good fit for T < 100 K and yielding the nearest-neighbor exchange constant J/kB ≅ 18 K. The variations of TB vs. H and HC vs. T are well described by the model often used for randomly oriented magnetic nanoparticles with magnetic domain diameter ≈ 9 nm present in the dead-layer of thickness d =1.4 nm. Finally, the data available from literature on the thickness (D) variation of Curie temperature (TC) and MS of LSMO films grown under 200, 150, and 0.38 mTorr pressures of O2 are analyzed in terms of the finite-size scaling, with MS vs. D data fit to MS (D) = MS(b)(1-d/D) yielding the dead layer thickness d = 1.1 nm, 1.4nm and 2.4 nm respectively.