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Search Results: 1 - 10 of 401642 matches for " V. J. Goldman "
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Comment on "Observation of the e/3 fractionally charged Laughlin quasiparticles" and "Direct Observation of Fractional Charge"
V. J. Goldman
Physics , 1997,
Abstract: comment on cond-mat/97063007 and cond-mat/9707289
Quantum Antidots: Coulomb Blockade or no Coulomb Blockade?
V. J. Goldman
Physics , 1999,
Abstract: Comment on M. Kataoka et al., Phys. Rev. Lett. 83, 160 (1999).
QHE Today
V. J. Goldman
Physics , 1999, DOI: 10.1016/S0921-4526(99)01760-3
Abstract: I present a brief survey of important recent developments in the quantum Hall effect. The review covers both fractional and integer regimes, from an experimentalist's perspective. The topics include direct measurement of fractional charge, composite fermion Fermi surface, spin textures, and edge state (chiral Luttinger liquid) dynamics.
On Anisotropic Transport in High Landau Levels
V. J. Goldman
Physics , 1999,
Abstract: We would like to point out that: (i) according to the edge-bulk transport models for the quantum Hall regime, the direction of low bulk conductance is actually perpendicular to that expected naively; and (ii) the values of experimental "high resistance" peaks correspond to value of bulk conductance $\approx 1 e^{2}/h$.
Superperiods and quantum statistics of Laughlin quasiparticles
V. J. Goldman
Physics , 2006, DOI: 10.1103/PhysRevB.75.045334
Abstract: Superperiodic conductance oscillations were recently observed in the quasiparticle interferometer, where an edge channel of the 1/3 fractional quantum Hall fluid encircles an island of the 2/5 fluid. We present a microscopic model of the origin of the 5h/e flux superperiod based on the Haldane-Halperin fractional-statistics hierarchical construction of the 2/5 condensate. Since variation of the applied magnetic field does not affect the charge state of the island, the fundamental period comprises the minimal 2/5 island neutral reconstruction. The period consists of incrementing by one the state number of the e/3 Laughlin quasielectron circling the island and the concurrent excitation of ten e/5 quasiparticles out of the island 2/5 condensate. The Berry phase quantization condition yields anyonic quasiparticle braiding statistics consistent with the hierarchical construction. We further discuss a composite fermion representation of quasiparticles consistent with the superperiods. It is shown to be in one-to-one correspondence with the Haldane-Halperin theory, provided a literal interpretation of the 2/5 condensate as comprised of an integer multiple of two-composite fermion, one-vortex blocks is postulated.
Quantum computation with quasiparticles of the Fractional Quantum Hall Effect
D. V. Averin,V. J. Goldman
Physics , 2001, DOI: 10.1016/S0038-1098(01)00447-1
Abstract: We propose an approach that enables implementation of anyonic quantum computation in systems of antidots in the two-dimensional electron liquid in the FQHE regime. The approach is based on the adiabatic transfer of FQHE quasiparticles in the antidot systems, and uses their fractional statistics to perform quantum logic. Advantages of our scheme over other semiconductor-based proposals of quantum computation include the energy gap in the FQHE liquid that suppresses decoherence, and the topological nature of quasiparticle statistics that makes it possible to entangle two quasiparticles without their direct dynamic interaction.
Dependence of the Fractional Quantum Hall Edge Critical Exponent on the Range of Interaction
V. J. Goldman,E. V. Tsiper
Physics , 2001, DOI: 10.1103/PhysRevLett.86.5841
Abstract: Comment on A.M.Chang et al, PRL 86, 143 (2001).
Formation of an Edge Striped Phase in Fractional Quantum Hall Systems
E. V. Tsiper,V. J. Goldman
Physics , 2001, DOI: 10.1103/PhysRevB.64.165311
Abstract: We have performed an exact diagonalization study of up to N=12 interacting electrons on a disk at filling $\nu={1/3}$ for both Coulomb and $V_1$ short-range interaction for which Laughlin wave function is the exact solution. For Coulomb interaction and $N\geq 10$ we find persistent radial oscillations in electron density, which are not captured by the Laughlin wave function. Our results srongly suggest formation of a chiral edge striped phase in quantum Hall systems. The amplitude of the charge density oscillations decays slowly, perhaps as a square root of the distance from the edge; thus the spectrum of edge excitations is likely to be affected.
Energetics of Quantum Antidot States in Quantum Hall Regime
I. J. Maasilta,V. J. Goldman
Physics , 1997, DOI: 10.1103/PhysRevB.57.R4273
Abstract: We report experiments on the energy structure of antidot-bound states. By measuring resonant tunneling line widths as function of temperature, we determine the coupling to the remote global gate voltage and find that the effects of interelectron interaction dominate. Within a simple model, we also determine the energy spacing of the antidot bound states, self consistent edge electric field, and edge excitation drift velocity.
Electron tunneling spectroscopy of a quantum antidot in the quantum Hall regime
V. J. Goldman,Jun Liu,A. Zaslavsky
Physics , 2007, DOI: 10.1103/PhysRevB.77.115328
Abstract: Quantum antidot, a small potential hill introduced into a two-dimensional electron system, presents an attractive tool to study quantum mechanics of interacting electrons.Here, we report experiments on electron resonant tunneling via a quantum antidot on the integer i = 1, 2, 3, 4, 5, and 6 quantum Hall plateaus. Several new features are reported. First, as a function of magnetic field, we observe up to six quasiperiodic resonant tunneling peaks within the fundamental flux period: when flux h/e is added to the area of the antidot there are i peaks on the i-th integer plateau, when i spin-polarized Landau levels are occupied. Corresponding back gate voltage data show one peak per added charge e on all integer plateaus. Second, we observe tunneling dips in four-terminal resistance ("forward scattering") on the even i = 2, 4, and 6 plateaus, when population of both spins is nearly equal. Also, for the first time, we report an internal structure within the h/e period: on the i = 3 spin-split plateau, two of the three resonant tunneling peaks are higher and/or closer than the third. Puzzlingly, in this regime, when back gate voltage is swept, the tunneling peaks are grouped in pairs. These results are attributed to the dominance of the electron-electron Coulomb interaction, effectively mixing Landau level occupation, and to the self-consistent electrostatics of the antidot.
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