2020年10月16日 · Here, we present the control of magnetic domain formation in paradigmatic SrRuO 3 /SrTiO 3 heterostructures via structural domain engineering. The formation of structural twin domains in SrRuO...

2020年1月10日 · Using the ferromagnetic metal SrRuO 3 as a model system, we demonstrate an efficient and reversible control of both structural and electronic phase transformations through the electric-field...

SrRuO3 is (Cubic) Perovskite structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional.

2012年3月8日 · In this review, the present state of knowledge of $ {\mathrm {SrRuO}}_ {3}$ thin films is summarized. Their role as a model system for studying magnetism and electron transport characterized by intermediate electron correlation and large magnetocrystalline anisotropy is …

2021年3月31日 · We have constructed an SrRuO 3 -PbTiO 3 (Ferromagnetic – Ferroelectric) bilayer that exhibits features in the Hall Hysteresis previously attributed to a Topological Hall Effect, and Skyrmions.

SrRuO3 is Orthorhombic Perovskite structured and crystallizes in the orthorhombic Pnma space group. The structure is three-dimensional. Sr2+ is bonded in a 12-coordinate geometry to nine O2- atoms.

SrRuO 3 is a ferromagnet with the Curie temperature TC of 163 K. The magnetic moment is found to be 1.44 μ B per formula unit at 5 K and 70 kOe [05DKC]. The inverse magnetic susceptibility follows the Curie-Weiss law at high temperature.

2022年2月11日 · In the third part, we discuss the spin-charge interconversion phenomena in SRO-based heterostructures, covering the inverse spin Hall effect and current-induced spin-orbit torques.

2022年9月8日 · In this fast-developing field, often referred to as quantum electronics, the metal-oxide perovskite SrRuO 3 can play an important role thanks to its diverse physical properties, which have been intensively investigated, mostly for conventional electronics.

2013年11月1日 · SrRuO 3 films and SrRuO 3 /SrTiO 3 superlattices grown on SrTiO 3 (001) were studied by structural, magnetic, magnetoresistance and Hall effect measurements. The superlattices showed heteroepitaxial growth with coherent interfaces and a Ru/Ti diffusion region of 1–1.5 unit cells.