A natural heavy-hole flopping mode qubit in germanium
arXiv:2012.10214 · doi:10.1103/PhysRevResearch.3.013194
Abstract
Flopping mode qubits in double quantum dots (DQDs) allow for coherent spin-photon hybridization and fast qubit gates when coupled to either an alternating external or a quantized cavity electric field. To achieve this, however, electronic systems rely on synthetic spin-orbit interaction (SOI) by means of a magnetic field gradient as a coupling mechanism. Here we theoretically show that this challenging experimental setup can be avoided in heavy-hole (HH) systems in germanium (Ge) by utilizing the sizeable cubic Rashba SOI. We argue that the resulting natural flopping mode qubit possesses highly tunable spin coupling strengths that allow for one- and two-qubit gate times in the nanosecond range when the system is designed to function in an optimal operation mode which we quantify.
13 pages, 8 figures
References in corpus (12)
- Prospects for Spin-Based Quantum Computing
- Strong Coupling of a Single Electron in Silicon to a Microwave Photon
- Spin relaxation and decoherence of holes in quantum dots
- Strong Coupling Cavity QED with Gate-Defined Double Quantum Dots Enabled by a High Impedance Resonator
- Electric Dipole Spin Resonance for Heavy Holes in Quantum Dots
- Spin relaxation and anticrossing in quantum dots: Rashba versus Dresselhaus spin-orbit coupling
- Ultra-long distance interaction between spin qubits
- Input-output theory for spin-photon coupling in Si double quantum dots
- Electric Dipole Induced Spin Resonance in Disordered Semiconductors
- Tunable g factor and phonon-mediated hole spin relaxation in Ge/Si nanowire quantum dots
- Breakdown of the Peierls substitution for the Haldane model with ultracold atoms
- Assessing the potential of Ge/SiGe quantum dots as hosts for singlet-triplet qubits