Conductance

About: Conductance is a research topic. Over the lifetime, 8088 publications have been published within this topic receiving 235961 citations.

Effect of surface roughness on the universal thermal conductance

Abstract: We explain the reduction of the thermal conductance below the predicted universal value observed by Schwab et al. [Nature (London) 404, 974 (2000)] in terms of the scattering of thermal phonons off surface roughness using a scalar model for the elastic waves. Our analysis shows that the thermal conductance depends on two roughness parameters: the roughness amplitude δ and the correlation length a. At sufficiently low temperatures the ratio of the conductance to the universal value decreases quadratically with temperature at a rate proportional to δ2a. Values of δ equal to 22% and a equal to about 75% of the width of the conduction pathway give a good fit to the data.

Microwave Transport in Metallic Single-Walled Carbon Nanotubes

Abstract: The dynamical conductance of electrically contacted single-walled carbon nanotubes is measured from dc to 10 GHz as a function of source-drain voltage in both the low-field and high-field limits. The ac conductance of the nanotube itself is found to be equal to the dc conductance over the frequency range studied for tubes in both the ballistic and diffusive limit. This clearly demonstrates that nanotubes can carry high-frequency currents at least as well as dc currents over a wide range of operating conditions. Although a detailed theoretical explanation is still lacking, we present a phenomenological model of the ac impedance of a carbon nanotube in the presence of scattering that is consistent with these results.

Many-body effects on the transport properties of single-molecule devices.

Abstract: The conductance through a molecular device including electron-electron and electron-phonon interactions is calculated using the numerical renormalization group method. At low temperatures and weak electron-phonon coupling the properties of the conductance can be explained in terms of the standard Kondo model with renormalized parameters. At large electron-phonon coupling a charge analog of the Kondo effect takes place that can be mapped into an anisotropic Kondo model. In this regime the molecule is strongly polarized by a gate voltage which leads to rectification in the current-voltage characteristics of the molecular junction.

Characterization of a chloride conductance activated by hyperpolarization in Aplysia neurones.

Abstract: A voltage-clamp study was made of some properties of the non-synaptic hyperpolarization-activated Cl- conductance recently described in Aplysia neurones loaded with Cl- ions (Chesnoy-Marchais, 1982). The experiments were performed on an identified family of neurones, which present cholinergic responses allowing an easy measurement of the equilibrium potentials of Cl- (ECl) and K+ ions (EK). The Cl- selectivity of the hyperpolarization-activated conductance was deduced from four observations: (1) the extrapolated reversal potential of the hyperpolarization-activated current, Er, was close to the reversal potential of the cholinergic Cl- response, which is the equilibrium potential for Cl- ions, ECl. (2) Modifications of the intracellular or extracellular Cl- concentration induced changes of the reversal potential Er. (3) A prolonged and intense activation of the current lowered the intracellular Cl- concentration. (4) The current persisted after complete substitution of intracellular and extracellular cations by CS+ ions, as well as after replacement of extracellular Na+ ions by Tris. The steady-state Cl- conductance (gss) increases steeply with hyperpolarization. The kinetics of activation and deactivation are exponential and are characterized by the same voltage-dependent time constant (tau), of the order of a few seconds or fractions of seconds. The curves gss(V) and tau (V) can both be fitted by a two-state model in which the rate constants are exponential functions of the membrane potential (e-fold change for 12-16 mV). The Cl- current is much more affected by changes of the intracellular Cl- concentration than predicted simply from the change in Cl- driving force. Both the conductance and the time constant of activation are strongly modified. Modifications of the extracellular Cl- concentration do not always alter the amplitude of the hyperpolarization-activated Cl- current, but systematically affect its kinetics. The hyperpolarization-activated current is abolished after prolonged exposure of the cell to an artificial sea water where NO3- ions replace Cl- ions, as well as after intracellular injections of NO3- ions. Increasing the external pH shifts the gss(V) and tau (V) curves to the left. Lowering the external pH has reverse but less pronounced effects. In cells which were not loaded with Cl- ions and did not present the hyperpolarization-activated Cl- current, this current could be detected if the hyperpolarizing jump was preceded by short depolarizing pulses. In cells which were loaded with Cl- ions, the Cl- current became larger after a short depolarizing pulse. In the presence of extracellular Co2+ ions, depolarizing pulses no longer increased the Cl- current.(ABSTRACT TRUNCATED AT 400 WORDS)