97 research outputs found

    Probing local electronic states in the quantum Hall regime with a side coupled quantum dot

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    We demonstrate a new method for locally probing the edge states in the quantum Hall regime utilizing a side coupled quantum dot positioned at an edge of a Hall bar. By measuring the tunneling of electrons from the edge states into the dot, we acquire information on the local electrochemical potential and electron temperature of the edge states. Furthermore, this method allows us to observe the spatial modulation of the electrostatic potential at the edge state due to many-body screening effect.Comment: 5 pages, 5 figure

    Anisotropic Behavior of the Thermoelectric Power and the Thermal Conductivity in a Unidirectional Lateral Superlattice: A Typical Anisotropic System Exhibiting Two Distinct Nernst Coefficients

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    We have calculated the thermoelectric conductivity tensor εij\varepsilon_{ij} and the thermal conductivity tensor λij\lambda_{ij} of a unidirectional lateral superlattice (ULSL) (i,j=x,yi,j = x,y, with the xx-axis aligned to the principal axis of the ULSL), %, given as the first- and the second-order moments, employing based on the asymptotic analytic formulas of the electrical conductivity tensor σij\sigma_{ij} in the literature valid at low magnetic fields where large numbers of Landau levels are occupied. With the resulting analytic expressions, we clarify the conditions for the Mott formula (Wiedemann-Franz law) to be applicable with high precision to εij\varepsilon_{ij} (λij\lambda_{ij}). We further present plots of the commensurability oscillations δεij\delta\varepsilon_{ij}, δλij\delta\lambda_{ij}, δκij\delta\kappa_{ij}, and δSij\delta S_{ij} in εij\varepsilon_{ij}, λij\lambda_{ij}, (an alternative, more standard definition of) the thermal conductivity tensor κij\kappa_{ij}, and the thermopower tensor SijS_{ij}, calculated using typical parameters for a ULSL fabricated from a GaAs/AlGaAs two-dimensional electron gas (2DEG). Notable features of the δSij\delta S_{ij} are (i) anisotropic behavior (δSxx≠δSyy\delta S_{xx} \ne \delta S_{yy}) and (ii) the dominance of the xyxy component over the other components (∣δSxy∣≫∣δSyx∣,∣δSxx∣,∣δSyy∣|\delta S_{xy}| \gg |\delta S_{yx}|, |\delta S_{xx}|, |\delta S_{yy}|). The latter clearly indicates that the two Nernst coefficients, SxyS_{xy} and SyxS_{yx}, can be totally different from each other in an anisotropic system. Both (i) and (ii) are at variance with the previous theory and are attributable to the inclusion of a damping factor due to the small-angle scattering characteristic of GaAs/AlGaAs 2DEGs, which have not been taken into consideration in δSij\delta S_{ij} thus far.Comment: 14 pages, 9 figures, Title and Introduction altered to make the main point of the paper clearer. Minor revisions throughout the paper. Some additions to the IV Discussion. Explicit energy dependence of the zero-temperature conductivity newly presented in the Appendi

    Detection of spin polarization with a side coupled quantum dot

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    We propose realistic methods to detect local spin polarization, which utilize a quantum dot side coupled to the target system. By choosing appropriate states in the dot, we can put spin selectivity to the dot and detect spins in the target with small disturbance. We also present an experiment which realizes one of the proposed spin detection schemes in magnetic fields.Comment: 5 pages, 6 figure

    Observation of the Fano-Kondo Anti-Resonance in a Quantum Wire with a Side-Coupled Quantum Dot

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    We have observed the Fano-Kondo anti-resonance in a quantum wire with a side-coupled quantum dot. In a weak coupling regime, dips due to the Fano effect appeared. As the coupling strength increased, conductance in the regions between the dips decreased alternately. From the temperature dependence and the response to the magnetic field, we conclude that the conductance reduction is due to the Fano-Kondo anti-resonance. At a Kondo valley with the Fano parameter q≈0q\approx 0, the phase shift is locked to π/2\pi/2 against the gate voltage when the system is close to the unitary limit in agreement with theoretical predictions by Gerland {\it et al.} [Phys. Rev. Lett. {\bf 84}, 3710 (2000)].Comment: 4 pages, 4 figure
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