Spin-Orbital Separation in the quasi 1D Mott-insulator Sr2CuO3
arXiv:1205.1954 · doi:10.1038/nature10974
Abstract
As an elementary particle the electron carries spin \hbar/2 and charge e. When binding to the atomic nucleus it also acquires an angular momentum quantum number corresponding to the quantized atomic orbital it occupies (e.g., s, p or d). Even if electrons in solids form bands and delocalize from the nuclei, in Mott insulators they retain their three fundamental quantum numbers: spin, charge and orbital[1]. The hallmark of one-dimensional (1D) physics is a breaking up of the elementary electron into its separate degrees of freedom[2]. The separation of the electron into independent quasi-particles that carry either spin (spinons) or charge (holons) was first observed fifteen years ago[3]. Using Resonant Inelastic X-ray Scattering on the 1D Mott-insulator Sr2CuO3 we now observe also the orbital degree of freedom separating. We resolve an orbiton liberating itself from spinons and propagating through the lattice as a distinct quasi-particle with a substantial dispersion of ~0.2 eV.
35 pages, 8 figures
Cited by in corpus (12)
- Crystal field splitting and correlation effect on the electronic structure of A2IrO3
- Spin-orbital quantum liquid on the honeycomb lattice
- Excitonic quasiparticles in a spin-orbit Mott insulator
- Spin excitations in a single LaCuO layer
- Fingerprints of spin-orbital entanglement in transition metal oxides
- High-energy magnetic excitations in BiSrCaCuO: Towards a unified description of the electronic and magnetic degrees of freedom in the cuprates
- CaIrO3 post-perovskite, a j = 1/2 quasi-one-dimensional antiferromagnet
- Noncollinear Magnetic Order Stabilized by Entangled Spin-Orbital Fluctuations
- Von Neumann Entropy Spectra and Entangled Excitations in Spin-Orbital Models
- Spin-independent v-representability of Wigner crystal oscillations in one-dimensional Hubbard chains: The role of spin-charge separation
- Optical conductivity due to orbital polarons in systems with orbital degeneracy
- Spin chain in magnetic field: limitations of the large-N mean-field theory