2008年10月7日 · We calculate the properties of the $4d$ ferromagnet ${\text{SrRuO}}_{3}$ in bulk and thin film form with the aim of understanding the experimentally observed metal-to-insulator transition at reduced thickness.

SrRuO3 is (Cubic) Perovskite structured and crystallizes in the cubic Pm-3m space group. The structure is three-dimensional. Sr2+ is bonded to twelve equivalent O2- atoms to form SrO12 cuboctahedra that share corners with twelve equivalent SrO12 cuboctahedra, faces with six equivalent SrO12 cuboctahedra, and faces with eight equivalent RuO6 ...

2008年7月8日 · We calculate the properties of the 4$d$ ferromagnet SrRuO$_3$ in bulk and thin film form with the aim of understanding the experimentally observed metal to insulator transition at reduced...

2016年7月8日 · We observed THE in epitaxial bilayers consisting of ferromagnetic SrRuO 3 and paramagnetic SrIrO 3 over a wide region of both temperature and magnetic field. The magnitude of THE rapidly decreases with the thickness of SrRuO 3, suggesting that the interface DM interaction plays a significant role.

In this chapter, crystallographic data and bulk modulus and magnetic properties of SrRuO 3 are given. It also discussed pressure dependence of the Curie temperature, spontaneous magnetization, coercive field and remanent magnetization of SrRuO 3.

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. There are a spread of Sr–O bond distances ranging from 2.51–3.00 Å. Ru4+ is bonded to six O2- atoms to form corner-sharing RuO6 octahedra.

We calculate the properties of the 4d ferromagnet SrRuO3 in bulk and thin film form with the aim of understanding the experimentally observed metal-to-insulator transition at reduced thickness. Although the spatial extent of the 4d orbitals is quite large, many experimental results have suggested that electron-electron correlations play an ...

2022年9月8日 · The growth of SrRuO 3 thin films with properties identical to bulk is essential to investigate emergent phenomena and discover new quantum effects in SrRuO 3. A high scalability in making optimal SrRuO 3 thin films is in turn crucial for the development of device applications exploiting such effects and phenomena.

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...

2021年9月20日 · The RuO 2 clusters exhibit ultrahigh OER activity with overpotential of ∼ 160 mV at 10 mA·cm geo−2 in 1.0 M HClO 4 solution for 30-h testing. The extended X-ray absorption fine structure measurement reveals enlarged Jahn-Teller distortion of RuO octahedra in the RuO 2 clusters compared to its bulk counterpart.