TY - JOUR
T1 - Two-dimensional conducting states in infinite-layer oxide/perovskite oxide hetero-structures
AU - Chen, Xiaobing
AU - Zhang, Jine
AU - Liu, Banggui
AU - Hu, Fengxia
AU - Shen, Baogen
AU - Sun, Jirong
N1 - Publisher Copyright:
© 2021 IOP Publishing Ltd Printed in the UK
PY - 2022/1/19
Y1 - 2022/1/19
N2 - Heterointerfaces sandwiched by oxides of dissimilar crystal structures will show strong interface reconstruction, leading to distinct interfacial effect arising from unusual physics. Here, we present a theoretical investigation on the interfaces between infinite-layer oxide and perovskite oxide (SrCuO2/SrTiO3 and SrCuO2/KTaO3). Surprisingly, we found well-defined two-dimensional electron gas (2DEG), stemming from atomic reconstruction and polar discontinuity at interface. Moreover, the 2DEG resides in both the TiO2 and CuO2 interfacial layers, unlike LaAlO3/SrTiO3 for which 2DEG exists only in the TiO2 interfacial layer. More than that, no metal-to-insulator transition is observed as the SrCuO2 layer thickness decreases to one unit cell, i.e., the metallicity of the new interface is robust. Further investigations show more unique features of the 2DEG. Due to the absence of apical oxygen at the SrCuO2/SrTiO3 (KTaO3) interface, the conducting states in the interface TiO2 (TaO2) layer follows the dxy < d3z2−r2 < dxz/yz orbital order rather than the dxy < dxz/yz orbital order of paradigm LaAlO3/SrTiO3 (KTaO3), exhibiting enhanced interfacial conduction. This work suggests the great potential of heterointerfaces composed of non-isostructural oxides for fundamental research.
AB - Heterointerfaces sandwiched by oxides of dissimilar crystal structures will show strong interface reconstruction, leading to distinct interfacial effect arising from unusual physics. Here, we present a theoretical investigation on the interfaces between infinite-layer oxide and perovskite oxide (SrCuO2/SrTiO3 and SrCuO2/KTaO3). Surprisingly, we found well-defined two-dimensional electron gas (2DEG), stemming from atomic reconstruction and polar discontinuity at interface. Moreover, the 2DEG resides in both the TiO2 and CuO2 interfacial layers, unlike LaAlO3/SrTiO3 for which 2DEG exists only in the TiO2 interfacial layer. More than that, no metal-to-insulator transition is observed as the SrCuO2 layer thickness decreases to one unit cell, i.e., the metallicity of the new interface is robust. Further investigations show more unique features of the 2DEG. Due to the absence of apical oxygen at the SrCuO2/SrTiO3 (KTaO3) interface, the conducting states in the interface TiO2 (TaO2) layer follows the dxy < d3z2−r2 < dxz/yz orbital order rather than the dxy < dxz/yz orbital order of paradigm LaAlO3/SrTiO3 (KTaO3), exhibiting enhanced interfacial conduction. This work suggests the great potential of heterointerfaces composed of non-isostructural oxides for fundamental research.
KW - Complex oxide interface
KW - Density functional calculations
KW - Nonisostructural interface
KW - Two dimensional electron gas
UR - https://www.scopus.com/pages/publications/85119411030
U2 - 10.1088/1361-648X/ac30b6
DO - 10.1088/1361-648X/ac30b6
M3 - 文章
C2 - 34663765
AN - SCOPUS:85119411030
SN - 0953-8984
VL - 34
JO - Journal of Physics Condensed Matter
JF - Journal of Physics Condensed Matter
IS - 3
M1 - A5
ER -