2007/04/30 by Susumu Yamamoto, S. Yamamoto, Takeo Fujiwara +3 · 1 citation
Chemistry · Materials Science · Physics and Astronomy · #Advanced Condensed Matter Physics #Anisotropy #Charge (physics) #Chemistry #Condensed matter physics #Coulomb #Crystallography #Electron #Energy (signal processing) #Hamiltonian (control theory) #Magnetic and transport properties of perovskites and related materials #Mott insulator #Order (exchange) #Physics #Physics of Superconductivity and Magnetism #Quantum mechanics #Spin (aerodynamics) #Thermodynamics #Valency #cond-mat.str-el
paper · pdf · doi:10.1103/physrevb.76.165114
published as Phys. Rev. B 76, 165114 (2007) · 12 pages, 10 figures, fully revised
arxiv created 2007/09/03 · openalex publication_date 2007/10/11 · arxiv updated 2009/12/01 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05
Electronic structure of stripe ordered La_2\ensuremath-xSrxNiO4 is investigated. The system with x=(1)/(3) is insulator, in LSDA+U calculations, and shows charge and spin stripe, consistent with the experimental results. A highly correlated system of x=(1)/(2) is studied by using exact diagonalization of the multiorbital many-body Hamiltonian derived from LDA calculations and including on-site and intersite Coulomb interactions. The fluctuation of the residual spin on Ni3+ (hole) site couples with the charge fluctuation between Ni3+ and Ni2+ states and this correlation lowers the total energy. The resultant ground state is an insulator with charge and spin stripe of the energy gap 0.9\phantom\rule0.3em0exeV, consistent with the observed one. The on-site Coulomb interaction stabilizes integral valency of each Ni ion (Ni3+ and Ni2+), but does not induce the charge order. Two quantities, intersite Coulomb interaction and anisotropy of hopping integrals, play an important role to form the charge and spin stripe order in a system of x=(1)/(2).