Localization Transition in a Ballistic Quantum Wire
arXiv:cond-mat/0506812 · doi:10.1103/PhysRevB.73.113307
Abstract
The many-body wave-function of an interacting one-dimensional electron system is probed, focusing on the low-density, strong interaction regime. The properties of the wave-function are determined using tunneling between two long, clean, parallel quantum wires in a GaAs/AlGaAs heterostructure, allowing for gate-controlled electron density. As electron density is lowered to a critical value the many-body state abruptly changes from an extended state with a well-defined momentum to a localized state with a wide range of momentum components. The signature of the localized states appears as discrete tunneling features at resonant gate-voltages, corresponding to the depletion of single electrons and showing Coulomb-blockade behavior. Typically 5-10 such features appear, where the one-electron state has a single-lobed momentum distribution, and the few-electron states have double-lobed distributions with peaks at . A theoretical model suggests that for a small number of particles (N<6), the observed state is a mixture of ground and thermally excited spin states.
10 pages, 4 figures, 1 table
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- Spin-charge separation and localization in one-dimension
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- Green's function for magnetically incoherent interacting electrons in one dimension
- Finite-size effects in tunneling between parallel quantum wires
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Cited by in corpus (37)
- The spin-incoherent Luttinger liquid
- Ground state properties of the one dimensional Coulomb gas
- Coulomb drag between two spin incoherent Luttinger liquids
- Spectral properties of a spin-incoherent Luttinger Liquid
- AFM probe for the signatures of Wigner correlations in the conductance of a one-dimensional quantum dot
- Localization in an Inhomogeneous Quantum Wire
- Ground state properties of the one-dimensional electron liquid
- Correlation effects in quasi one dimensional electron wires
- The electron lifetime in Luttinger liquids
- Electron tunneling into a quantum wire in the Fabry-Perot regime
- Spectral function of few electrons in quantum wires and carbon nanotubes as a signature of Wigner localization
- Kondo screening cloud and the charge staircase in one-dimensional mesoscopic devices
- Absence of Wigner molecules in one-dimensional few-fermion systems with short-range interactions
- High-density correlation energy expansion of the one-dimensional uniform electron gas
- Deformed Wigner crystal in a one-dimensional quantum dot
- Spin-catalyzed hopping conductivity in disordered strongly interacting quantum wires
- Chemistry in One Dimension
- Local Density of States for Individual Energy Levels in Finite Quantum Wires
- Evolution of the quantum Hall bulk spectrum into chiral edge states
- Boundary Green's Function for Spin-Incoherent Interacting Electrons in One Dimension
- Spin-incoherent behavior in the ground state of strongly correlated systems
- Fermi-edge singularity in a spin-incoherent Luttinger liquid
- Thermal disruption of a Luttinger liquid
- Thermoelectric Scanning Gate Interferometry on a Quantum Point Contact
- Signatures of Strong Correlations in One-Dimensional Ultra-Cold Atomic Fermi Gases
- Ground states of long-range interacting fermions in one spatial dimension
- Symmetry-broken local-density approximation for one-dimensional systems
- Effects of interedge scattering on the Wigner crystallization in graphene nanoribbons
- Tunneling Density of States, Pair Correlation, and Josephson Current in Spin-Incoherent Luttinger Liquid-Superconductor Hybrid Systems
- Probing Wigner correlations in a suspended carbon nanotube
- Wigner crystallization at graphene edges
- Singular responses of spin-incoherent Luttinger liquids
- Non-equilibrium charge noise and dephasing from a spin-incoherent Luttinger liquid
- Hartree-Fock calculations of a finite inhomogeneous quantum wire
- Junctions of Spin-Incoherent Luttinger Liquids with Ferromagnets and Superconductors
- Real-Time Ramsey Interferometry in Fractional Quantum Hall States
- Impact of the non-canonical approach to the exact solution of the ideal one-dimensional electron gas confined with an anisotropic quantum wire of oscillator-shaped profile