TY - JOUR
T1 - Electronic structure of SrTi1-x Vx O3 films studied by in situ photoemission spectroscopy
T2 - Screening for a transparent electrode material
AU - Kanda, Tatsuhiko
AU - Shiga, Daisuke
AU - Yukawa, Ryu
AU - Hasegawa, Naoto
AU - Nguyen, Duy Khanh
AU - Cheng, Xianglin
AU - Tokunaga, Ryosuke
AU - Kitamura, Miho
AU - Horiba, Koji
AU - Yoshimatsu, Kohei
AU - Kumigashira, Hiroshi
N1 - Funding Information:
The authors are very grateful to Y. Kuramoto and M. Kobayashi for their helpful discussions and acknowledge M. Minohara for his advice on sample growth. This work was financially supported by a Grant-in-Aid for Scientific Research (Grants No. 16H02115, No. 16KK0107, and No. 20KK0117) from the Japan Society for the Promotion of Science (JSPS), CREST (JPMJCR18T1) from the Japan Science and Technology Agency (JST), and the MEXT Element Strategy Initiative to Form Core Research Center (Grant No. JPMXP0112101001). The preliminary sample characterization using hard x-ray photoemission at SPring-8 was conducted with approval from the Japan Synchrotron Radiation Research Institute (Proposal No. 2019B1248). The work performed at KEK-PF was approved by the Program Advisory Committee (Proposals No. 2019T004 and No. 2018S2-004) at the Institute of Materials Structure Science, KEK.
Publisher Copyright:
© 2021 American Physical Society.
PY - 2021/9/15
Y1 - 2021/9/15
N2 - This study investigated the electronic structure of SrTi1-xVxO3 (STVO) thin films, which are solid solutions of strongly correlated transparent conductive oxide (TCO) SrVO3 and oxide semiconductor SrTiO3, using in situ photoemission spectroscopy. STVO is one of the most promising candidates for correlated-metal TCO because it has the capability of optimizing the performance of transparent electrodes by varying x. Systematic and significant spectral changes were found near the Fermi level (EF) as a function of x, while the overall electronic structure of STVO is in good agreement with the prediction of band-structure calculations. As x decreases from 1.0, spectral weight transfer occurs from the coherent band near EF to the incoherent states (lower Hubbard band) around 1.0-1.5 eV. Simultaneously, a pseudogap is formed at EF, indicating a significant reduction in quasiparticle spectral weight within close vicinity of EF. This pseudogap seems to evolve into an energy gap at x=0.4, suggesting the occurrence of a composition-driven metal-insulator transition. From angle-resolved photoemission spectroscopic results, the carrier concentration n changes proportionally as a function of x in the metallic range of x=0.6-1.0. In contrast, the mass enhancement factor, which is proportional to the effective mass (m∗), does not change significantly with varying x. These results suggest that the key factor of n/m∗ in optimizing the performance of correlated-metal TCO is tuned by x, highlighting the potential of STVO to achieve the desired TCO performance in the metallic region.
AB - This study investigated the electronic structure of SrTi1-xVxO3 (STVO) thin films, which are solid solutions of strongly correlated transparent conductive oxide (TCO) SrVO3 and oxide semiconductor SrTiO3, using in situ photoemission spectroscopy. STVO is one of the most promising candidates for correlated-metal TCO because it has the capability of optimizing the performance of transparent electrodes by varying x. Systematic and significant spectral changes were found near the Fermi level (EF) as a function of x, while the overall electronic structure of STVO is in good agreement with the prediction of band-structure calculations. As x decreases from 1.0, spectral weight transfer occurs from the coherent band near EF to the incoherent states (lower Hubbard band) around 1.0-1.5 eV. Simultaneously, a pseudogap is formed at EF, indicating a significant reduction in quasiparticle spectral weight within close vicinity of EF. This pseudogap seems to evolve into an energy gap at x=0.4, suggesting the occurrence of a composition-driven metal-insulator transition. From angle-resolved photoemission spectroscopic results, the carrier concentration n changes proportionally as a function of x in the metallic range of x=0.6-1.0. In contrast, the mass enhancement factor, which is proportional to the effective mass (m∗), does not change significantly with varying x. These results suggest that the key factor of n/m∗ in optimizing the performance of correlated-metal TCO is tuned by x, highlighting the potential of STVO to achieve the desired TCO performance in the metallic region.
UR - http://www.scopus.com/inward/record.url?scp=85114891065&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=85114891065&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.104.115121
DO - 10.1103/PhysRevB.104.115121
M3 - Article
AN - SCOPUS:85114891065
SN - 2469-9950
VL - 104
JO - Physical Review B
JF - Physical Review B
IS - 11
M1 - 115121
ER -