Abstract
In superconducting quantum point contacts, multiple Andreev reflection (MAR), which describes the coherent transport of m quasiparticles each carrying an electron charge with \(m\ge 3\), sets in at voltage thresholds \(eV = 2\Delta /m\). In single-electron transistors, Coulomb blockade, however, suppresses the current at low voltage. The required voltage for charge transport increases with the square of the effective charge \(eV\propto \left( me\right) ^2\). Thus, studying the charge transport in all-superconducting single-electron transistors (SSETs) sets these two phenomena into competition. In this article, we present the fabrication as well as a measurement scheme and transport data for a SSET with one junction in which the transmission and thereby the MAR contributions can be continuously tuned. All regimes from weak to strong coupling are addressed. We extend the Orthodox theory by incorporating MAR processes to describe the observed data qualitatively. We detect a new transport process the nature of which is unclear at present. Furthermore, we observe a renormalization of the charging energy when approaching the strong coupling regime.
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Notes
The used parameters are \(E_\mathrm {C}\,={122}\, \upmu \hbox {eV}\), \(\delta C/C_\Sigma =-0.557\), \(C_\mathrm{G}={75}\, \hbox {aF}\), \(\Delta ={190}\, \upmu \hbox {eV}\), \(Q_0/e=0.625\).
Including (M)AR in the master equation simulation of this regime even with very low conductance will cause numerical artefacts affecting the height and width of the J-QP cycle over the TB.
The used parameters are \(E_\mathrm {C}\,={123}\, \upmu \hbox {eV}\), \(\delta C/C_\Sigma =-0.557\), \(C_\mathrm{G}={74}\, \hbox {aF}\), \(\Delta ={190}\, \upmu \hbox {eV}\), \(Q_0=0.425\).
The used parameters are \(E_\mathrm {C}\,={58}\, \upmu \hbox {eV}\), \(\delta CC_\Sigma =0.252\), \(C_\mathrm{G}={75}\, \hbox {aF}\), \(\Delta ={190}\, \upmu \hbox {eV}\), \(Q_0/e=0.002\).
The AR line is not on top of the ridge intentionally. We expect the maximum in the Andreev conduction to be not at the threshold but at slightly higher bias values for high transmissions as seen in point contacts [32]. The harder criterion is in our opinion the beginning of the J-QP cycle at the intersection to the quasiparticle line.
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Acknowledgements
The authors like to thank Jens Siewert and Wolfgang Belzig for useful discussion. We also thank Olivier Schecker, Ursula Schröter, and Paramita Kar Choudhury for their contributions in the early state of the project.
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Lorenz, T., Sprenger, S. & Scheer, E. Coulomb Blockade and Multiple Andreev Reflection in a Superconducting Single-Electron Transistor. J Low Temp Phys 191, 301–315 (2018). https://doi.org/10.1007/s10909-017-1837-4
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DOI: https://doi.org/10.1007/s10909-017-1837-4