Fabrication and Properties of Cr2O3 and La0.7Sr0.3MnO3 Thin Film Heterostructures Integrated on Si(001)

Spintronics that utilizes both the spin and charge degrees of freedom of an electron is emerged as an alternate memory technology to conventional CMOS electronics. Many proposed spintronic devices require multifunctional properties in a single material. The oxides Cr2O3 and La0.7Sr0.3MnO3 are such materials which exhibit unique physical properties at room temperature. The Cr2O3 is an antiferromagnetic and magnetoelectric material below its Neel temperature 307K. The La0.7Sr0.3MnO3 is a ferromagnetic half metal with a Curie temperature of 360K and exhibits colossal magnetoresistance. However, the reach of this spintronic technology into more device applications is possible only when these materials in epitaxial thin film form are integrated with Si(001) which is the mainstay substrate in semiconductor industry.;The primary objective of this dissertation was to integrate epitaxial Cr2O3, La0.7Sr0.3MnO3 and Cr2O3/La0.7Sr0.3MnO3 thin film heterostructure on Si(001) and, study their physical properties to investigate structure-processing-property relationship in these heterostructures.;The epitaxial integration of Cr2O3 thin films on Si(001) was done using epitaxial cubic yttria stabilized zirconia (c-YSZ) buffer layer by pulsed laser deposition. Detailed structural characterizations XRD (2theta and phi) and TEM confirm the epitaxial nature of the films. Though bulk Cr2O3 is antiferromagnetic along the c-axis, the in-plane magnetization measurements on Cr2O3(0001) thin films showed ferromagnetic behavior up to 400K. The thickness dependent magnetization together with oxygen annealing results suggested that the in-plane ferromagnetism in Cr2O3 was due to the oxygen related defects whose concentration is controlled by strain in the films. The out-of-plane magnetic measurements on Cr2O3(0001) films showed magnetic behavior indicative of antiferromagnetic nature.;To verify whether ferromagnetism can be induced by strain in Cr 2O3 thin films with orientation other than (0001), epitaxial thin films were prepared on r-Al2O3 substrate and their magnetic properties were studied. The XRD (2theta and phi) and TEM confirm that the films were grown epitaxially. The epitaxial relations were given as: [011¯2]Cr2O3 || [011¯2]Al2O 3 and [1¯1¯20]Cr2O3 || [1¯1¯20]Al 2O3. The as-deposited films showed ferromagnetic behavior up to 400K but it almost vanished with oxygen annealing. The Raman spectroscopy data together with strain measurements using XRD indicated that ferromagnetism in r-Cr2O3 thin films was due to the strain caused by defects such as oxygen vacancies.;Bi-epitaxial La0.7Sr0.3MnO3(110) thin films were integrated on Si(100) with c-YSZ/SrTiO3(STO) buffer layers by pulsed laser deposition. The La0.7Sr0.3MnO 3 and STO thin films had a single [110] out-of-plane orientation but with two in-plane domain variants as confirmed from XRD and TEM study. The growth of STO on c-YSZ was explained by the domain matching epitaxy paradigm. The epitaxial relationship between STO and c-YSZ were written as [110](001)c-YSZ || [1¯11¯](110)STO (or) [110](001)c-YSZ || [1¯12¯](110)STO. The La0.7Sr0.3MnO3 thin films were ferromagnetic with Curie temperature 324K. They also exhibited hysteresis in magnetoresistance under both in-plane and out-of-plane magnetic fields. The highest magnetoresistance in this study was -32% at 50K and 50 kOe for in-plane configuration.;Lastly, the epitaxial La0.7Sr0.3MnO3-delta -d(LSMO)/Cr2O3 bilayer structure was integrated with Si(001) using c-YSZ by pulsed laser deposition. The XRD (2theta and phi) and TEM characterizations confirm that the films were grown epitaxially. The epitaxial relations were written as [0001]Cr2O3 || [111]LSMO and [112¯0]Cr2O3 || [101¯]LSMO. Interestingly, when the LSMO thickness was increased from 66 to 528 nm (Cr2O 3=55nm), the magnetization increased by 2-fold and the magnetic nature changed from ferromagnetic to super paramagnetic. In addition, LSMO/Cr 2O3 showed in-plane exchange bias. We believe that the change in the magnetic anisotropy as a function of LSMO layer thickness could cause the change in magnetization and magnetic nature. The magnetic phase separation in oxygen deficient LSMO layer could lead to in-plane exchange bias as Cr 2O3 is not expected to show in-plane exchange.