For several years, the LaTEQS team at PHELIQS has been dedicated to studying the electronic properties of germanium layers a few nanometers thick embedded in a SiGe substrate. These layers exhibit exceptional qualities, with mobilities reaching several hundred thousand cm²/V/s and an elastic mean free path in the micron range. They are fabricated at LETI as 200 mm diameter wafers, then formed using PTA for the design of quantum devices such as spin qubits and superconducting transistors. Through a series of three recent publications and as many theses, we have developed the manufacturing processes for superconducting transistors, studied in detail the properties of the field-induced dissipationless current in the Ge channel, and fabricated our first superconducting qubit.
The superconducting transistors of interest consist of a germanium channel (a semiconductor material) a few hundred nm long and connected to two aluminum superconductors (source and drain). The device is completed by an electrostatic gate that covers the channel, allowing control of the current flowing through it. This operation is similar to the silicon transistors used in cell phones. We exploit the properties of germanium at very low temperatures when the aluminum contacts become superconducting. Thanks to the exceptional quality of the electrical contact between the aluminum and the germanium, it becomes possible to induce superconducting correlations in the channel, thus making it itself "superconducting," i.e., without energy dissipation. We have thus developed a "perfect" transistor which, in its OFF state (positive gate voltage), does not conduct, and which, in its ON state (negative gate voltage), conducts without resistance. This transistor therefore generates no heat dissipation.
The main objective of our work is to deepen our understanding of the properties of this non-dissipative current and to create our first quantum circuit based on this type of transistor.
When a superconducting current flows through a non-superconducting material, there is a relationship between the macroscopic phases of the two superconductors and the current amplitude (the first Josephson relationship). When this weak link is a tunnel barrier, this relationship takes the form of a pure sinusoidal function. This phenomenon (the Josephson effect) forms the basis of superconducting quantum circuits such as those developed by companies like Google, IBM, Rigetti, and, in France, within the start-ups Alice&Bob and SilentWave and in many academic laboratories.
We recently demonstrated that, in the case of our devices, called JoFET (Josephson Field Effect Transistor), this relationship is more complex and includes higher harmonics [1]. This phenomenon demonstrates the very good electrical quality of the source-drain interfaces with germanium. We then fabricated a first device composed of two JoFETs integrated into a small superconducting loop (SQUID) [2]. By modulating the magnetic flux through this loop, it is possible to control the amplitude of the supercurrent and manipulate its different harmonics through interference. We thus developed the equivalent of a JoFET whose first harmonic is reduced by 95% (see
figure). This phenomenon indicates that the non-dissipative current is no longer carried by Cooper pairs but by pairs of pairs, opening the way to new types of superconducting qubits, potentially better protected than those based on tunnel junctions.
With this in mind, we developed a first superconducting qubit from a single JoFET, controllable by a gate [3]. The geometry of this qubit is inspired by superconducting qubits based on tunnel junctions (transmon), composed of a superconducting island connected to a JoFET, itself coupled to a microwave resonator for reading the qubit state. Using circuits quantum electrodynamics (cQED) techniques, we demonstrated the coherent control of the qubit's quantum states using microwave signals. We also measured the impact of gate control on the qubit's states, by evaluating its coherence times. Although these times are still modest (in the order of a few tens of nanoseconds), this advance paves the way for qubits whose protection and coherence times should be considerably improved.