2D systems can not only have physical properties distinct from those of 3D materials but also allow control/manipulation of their properties through stacking. For example, Mott insulating and superconducting states, unavailable in single layer graphene, are realized in twisted bilayer graphene. While these novel 2D systems are mostly obtained through exfoliation of van der Waals materials, a more conventional approach through thin film growth. In this presentation, I wish to introduce our research efforts to measure and manipulate electronic properties of a few unit-cell (uc) thick thin films including SrRuO3, SrIrO3 and (La,Sr)2CuO4 using thin film growth and in situ angle resolved photoemission (ARPES). We started with ARPES on a few uc thick film of SrRuO3 (SRO), a prototypical metallic ferromagnet with spin-orbit coupling. It was found that nodal lines and quadratic band crossing points are generic features of ultrathin perovskite films. These symmetry-protected nodal lines and quadratic band crossing points are sources of Berry curvature that causes the sign changing anomalous Hall effects [1]. By using additional ‘conducting layer’, we were able to obtain the electronic structure of 1 uc thick SRO films. Our results show that 1 uc films are not insulators but remain metallic. Dosing experiments reveal that 1 uc films are correlated Hund metals caused by the high density of states near EF from the van Hov singularity [2]. We further controlled the strain and octahedron distortion of 1 uc films by using various substrates. We demonstrate that the electronic state of 1 uc films can be manipulated from a good metal to a correlated Hund metal, and finally to a Mott insulator [3][4]. Meanwhile, we were able to grow and measure the electronic structure of SrIrO3 (SIO) as well as (La,Sr)2CuO4 (LSCO) films down to a single layer. 1 uc SIO films has the same crystal structure of that of 1 uc Sr2IrO4. Not surprisingly, it is found that SIO 1uc films have the electronic structure of Sr2IrO4: relativistic Mott insulating state with (short) AF order[5]. Meanwhile, a single layer of LSCO contains a single CuO2 plane and gap measurements indicates superconductivity in a single CuO2 plane[6]. 参考文献 [1] Sohn et al., Nature Materials 20, 1643 (2021) [2] Sohn et al., Nature Communications 12, 6171 (2021) [3] Kim et al., Advanced Materials (2023) [4] Ko et al., Nature Communications (2023) [5] J. Y. Kim, in preparation [6] Y. D. Kim, under review |