We present an extension of the Keldysh-Green s function method, which allows one to calculate the full distribution of transmitted particles through a mesoscopic superconductor. The method is applied to the statistics of supercurrent in short contacts. If the current is carried by Andreev bound states the distribution corresponds to switching between long trains of electrons going in opposite directions. For weak (gapless) superconductors or tunnel junctions we find that at low temperatures the distribution has negative probabilities. Accounting for the quantum mechanical nature of the measuring device shows that these negative values can indeed be measured
We calculate the distribution of current fluctuations in two simple exclusion models. Although these...
We consider the production of spatially separated entangled electrons in transport between a superco...
Submitted to Eur. Phys. J. BInternational audienceWe calculate the distribution of current fluctuati...
We study the current statistics in normal diffusive conductors in contact with a superconductor. Usi...
We derive the full counting statistics of charge transfer through a voltage biased superconducting j...
We derive the full distribution of transmitted particles through a superconducting point contact of ...
We studythe full counting statistics of heterostructures consisting of normalmetal parts connected t...
We study the statistics of charge transport in a mesoscopic three-terminal device with one supercond...
We demonstrate that the probability distribution of the net number of electrons passing through a qu...
We present a comprehensive theoretical analysis of the dc transport properties of superconducting po...
A method to calculate the statistics of energy exchange between quantum systems is presented. The ge...
The statistical properties of quantum particles moving between two heat reservoirs at different temp...
We employ a single-charge counting technique to measure the full counting statistics of Andreev even...
We employ a single-charge counting technique to measure the full counting statistics of Andreev even...
The calculation of the full counting statistics (FCS) for quantum mechanical systems has attracted m...
We calculate the distribution of current fluctuations in two simple exclusion models. Although these...
We consider the production of spatially separated entangled electrons in transport between a superco...
Submitted to Eur. Phys. J. BInternational audienceWe calculate the distribution of current fluctuati...
We study the current statistics in normal diffusive conductors in contact with a superconductor. Usi...
We derive the full counting statistics of charge transfer through a voltage biased superconducting j...
We derive the full distribution of transmitted particles through a superconducting point contact of ...
We studythe full counting statistics of heterostructures consisting of normalmetal parts connected t...
We study the statistics of charge transport in a mesoscopic three-terminal device with one supercond...
We demonstrate that the probability distribution of the net number of electrons passing through a qu...
We present a comprehensive theoretical analysis of the dc transport properties of superconducting po...
A method to calculate the statistics of energy exchange between quantum systems is presented. The ge...
The statistical properties of quantum particles moving between two heat reservoirs at different temp...
We employ a single-charge counting technique to measure the full counting statistics of Andreev even...
We employ a single-charge counting technique to measure the full counting statistics of Andreev even...
The calculation of the full counting statistics (FCS) for quantum mechanical systems has attracted m...
We calculate the distribution of current fluctuations in two simple exclusion models. Although these...
We consider the production of spatially separated entangled electrons in transport between a superco...
Submitted to Eur. Phys. J. BInternational audienceWe calculate the distribution of current fluctuati...