Towards the realization of CMOS compatible superconducting qubits
On one hand, Ge system offers a rather unique combination of excellent transport properties (micron-scale elastic mean-free path at low carrier densities), intrinsically strong spin-orbit coupling, and generally low p-type Shottky barriers, which is expected to facilitate the achievement of a good electrical contact with superconducting metals, and hence a sizeable superconducting proximity effect. In addition, Ge/SiGe can be epitaxially grown on large silicon wafers, which would eventually enable a straightforward path to large scale integration. Following highly encouraging first results - observation of ballistic one-dimensional hole transport and Josephson field-effect transistor (JoFET) functionality, we intend to strengthen our research in this direction. In this endeavour, we shall as well rely on recently established collaboration with LETI, which brings a valuable expertise in material growth/deposition, device processing, and integration.
On the other hand, Si technology is the most mature technology but suffer from a Schottky barrier with superconducting materials that reduces strongly proximity effect. The possibility to include, in the CMOS technology, superconducting silicon obtained by laser annealing combined with superconducting silicides offers a new opportunity towards the realization of silicon JoFET’s.
Our research activity is oriented towards the realization of Josephson field-effect transistors and their incorporation in transmon-type superconducting qubits (gatemon’s). It is a great challenge with basic science issues together with potential outcomes for quantum information. This objective will also require interaction with the LETI for material growth and integration and with the Néel Institute for quantum manipulation of superconducting qubits.
Helical states and Majorana fermions in topological nanostructures
Similar concepts have led to the superconducting counterpart of topological insulators: topological superconductors. The topological character manifest itself in the excitation spectrum of the superconducting state and gives rise to quasiparticles analog to Majorana fermions. Majorana particle is known to be its own antiparticle, have no charge or spin and are therefore very well isolated from the environment and are ideal for storing quantum information. The existence of Majorana fermions was predicted and intensely studied in particle physics but this quest was unsuccessful. The experimental realization of topological superconductivity in superconductor-semiconductor hybrid structures allowed to reproduce the experimental conditions for the creation of Majorana fermions and the first experimental signatures in transport was obtained recently. Since then, the search around the Majorana fermions has become a major theme in condensed matter physics. However, most of these theoretical predictions about these excitations have not received any experimental confirmations