ReCFI, Department of Physics and Astronomy, Seoul National University, Seoul, Republic of Korea.
J Phys Condens Matter. 2010 Dec 8;22(48):485602. doi: 10.1088/0953-8984/22/48/485602. Epub 2010 Nov 16.
We have investigated the electronic structure of meta-stable perovskite Ca(1 - x)Sr(x)IrO(3)(x = 0, 0.5, and 1) thin films using transport measurements, optical spectroscopy, and first-principles calculations. We artificially fabricated the perovskite phase of Ca(1 - x)Sr(x)IrO(3), which has a hexagonal or post-perovskite crystal structure in bulk form, by growing epitaxial thin films on perovskite GdScO(3) substrates using an epi-stabilization technique. The transport properties of the perovskite Ca(1 - x)Sr(x)IrO(3) films systematically change from nearly insulating (or semi-metallic) for x = 0 to weakly metallic for x = 1. Due to the extended wavefunctions, 5d electrons are usually delocalized. However, the strong spin-orbit coupling in Ca(1 - x)Sr(x)IrO(3) results in the formation of effective total angular momentum J(eff) = 1/2 and 3/2 states, which puts Ca(1 - x)Sr(x)IrO(3) in the vicinity of a metal-insulator phase boundary. As a result, the electrical properties of the Ca(1 - x)Sr(x)IrO(3) films are found to be sensitive to x and strain.
我们使用输运测量、光学光谱和第一性原理计算研究了亚稳钙钛矿 Ca(1 - x)Sr(x)IrO(3)(x = 0、0.5 和 1) 薄膜的电子结构。我们通过在钙钛矿 GdScO(3) 衬底上使用外延稳定技术生长外延薄膜,人为地制造了具有六方或后钙钛矿晶体结构的块状钙钛矿 Ca(1 - x)Sr(x)IrO(3)的钙钛矿相。钙钛矿 Ca(1 - x)Sr(x)IrO(3) 薄膜的输运性质系统地从 x = 0 的近绝缘(或半金属)变化为 x = 1 的弱金属。由于扩展的波函数,5d 电子通常是离域的。然而,Ca(1 - x)Sr(x)IrO(3)中的强自旋轨道耦合导致形成有效总角动量 J(eff) = 1/2 和 3/2 态,这使得 Ca(1 - x)Sr(x)IrO(3)处于金属-绝缘相边界附近。因此,Ca(1 - x)Sr(x)IrO(3) 薄膜的电学性质被发现对 x 和应变敏感。