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Electronic Structure of the Kitaev Material α-RuCl(3) Probed by Photoemission and Inverse Photoemission Spectroscopies

Recently, α-RuCl(3) has attracted much attention as a possible material to realize the honeycomb Kitaev model of a quantum-spin-liquid state. Although the magnetic properties of α-RuCl(3) have been extensively studied, its electronic structure, which is strongly related to its Kitaev physics, is poo...

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Detalles Bibliográficos
Autores principales: Sinn, Soobin, Kim, Choong Hyun, Kim, Beom Hyun, Lee, Kyung Dong, Won, Choong Jae, Oh, Ji Seop, Han, Moonsup, Chang, Young Jun, Hur, Namjung, Sato, Hitoshi, Park, Byeong-Gyu, Kim, Changyoung, Kim, Hyeong-Do, Noh, Tae Won
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2016
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5175179/
https://www.ncbi.nlm.nih.gov/pubmed/28000731
http://dx.doi.org/10.1038/srep39544
Descripción
Sumario:Recently, α-RuCl(3) has attracted much attention as a possible material to realize the honeycomb Kitaev model of a quantum-spin-liquid state. Although the magnetic properties of α-RuCl(3) have been extensively studied, its electronic structure, which is strongly related to its Kitaev physics, is poorly understood. Here, the electronic structure of α-RuCl(3) was investigated by photoemission (PE) and inverse-photoemission (IPE) spectroscopies. The band gap was directly measured from the PE and IPE spectra and was found to be 1.9 eV, much larger than previously estimated values. Local density approximation (LDA) calculations showed that the on-site Coulomb interaction U could open the band gap without spin-orbit coupling (SOC). However, the SOC should also be incorporated to reproduce the proper gap size, indicating that the interplay between U and SOC plays an essential role. Several features of the PE and IPE spectra could not be explained by the results of LDA calculations. To explain such discrepancies, we performed configuration-interaction calculations for a RuCl(6)(3−) cluster. The experimental data and calculations demonstrated that the 4d compound α-RuCl(3) is a J(eff) = 1/2 Mott insulator rather than a quasimolecular-orbital insulator. Our study also provides important physical parameters required for verifying the proposed Kitaev physics in α-RuCl(3).