2020/12/30 by Takeo Miyashita, Hideaki Iwasawa, Tomoki Yoshikawa +8
Chemistry · Materials Science · Physics and Astronomy · #Advanced Condensed Matter Physics #Angle-resolved photoemission spectroscopy #Brillouin zone #Chemistry #Condensed matter physics #Electron #Electronic and Structural Properties of Oxides #Electronic structure #Fermi level #Fermi surface #Magnetic and transport properties of perovskites and related materials #Materials science #Mott insulator #Nuclear magnetic resonance #Photoemission spectroscopy #Physics #Quantum mechanics #Superconductivity #Tetragonal crystal system #X-ray photoelectron spectroscopy #cond-mat.str-el
paper · pdf · doi:10.1016/j.ssc.2020.114180
published as Solid State Communications 326, 114180 (2021) · 9 pages, 6 figures
openalex publication_date 2020/12/30 · openalex created_date 2021/01/05 · arxiv created 2021/02/03 · arxiv updated 2021/02/04 · openalex updated_date 2026/08/05
Insulator-to-metal transition in Ca2RuO4 has drawn keen attention because of its sensitivity to various stimulation and its potential controllability. Here, we report a direct observation of Fermi surface, which emerges upon introducing excess oxygen into an insulating Ca2RuO4, by using angle-resolved photoemission spectroscopy. Comparison between energy distribution curves shows that the Mott insulating gap is closed by eV-scale spectral-weight transfer with excess oxygen. Momentum-space mapping exhibits two square-shaped sheets of the Fermi surface. One is a hole-like α sheet around the corner of a tetragonal Brillouin zone, and the other is an electron-like β sheet around the Γ point. The electron occupancies of the α and β bands are determined to be nα=1.6 and nβ=0.6, respectively. Our result indicates that the insulator-to-metal transition occurs selectively in dxz and dyz bands and not yet in dxy band. This orbital selectivity is most likely explained in terms of the energy level of dxy, which is deeper for Ca2RuO4+δ than for Ca1.8Sr0.2RuO4. Consequently, we found substantial differences from the Fermi surface of other ruthenates, shedding light on a unique role of excess oxygen among the metallization methods of Ca2RuO4.