2014
DOI: 10.1063/1.4893242
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Circuit-quantum electrodynamics with direct magnetic coupling to single-atom spin qubits in isotopically enriched 28Si

Abstract: Recent advances in silicon nanofabrication have allowed the manipulation of spin qubits that are extremely isolated from noise sources, being therefore the semiconductor equivalent of single atoms in vacuum. We investigate the possibility of directly coupling an electron spin qubit to a superconducting resonator magnetic vacuum field. By using resonators modified to increase the vacuum magnetic field at the qubit location, and isotopically purified 28 Si substrates, it is possible to achieve coupling rates fas… Show more

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Cited by 37 publications
(40 citation statements)
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“…59 We note that, while the qubit-resonator coupling strength g is limited by the constraint ξ 1 required for the validity of the Heisenberg model description of the RX qubit, 18 the estimate we obtain here does not represent a fundamental limit and varies strongly with the chosen parameters. Further enhancements of g may be possible by, e.g., modifying the design of the transmission line resonator to increase the strength of the electric field within the region containing the RX qubit 60,70 and thus the chargecavity coupling strength g 0 . Recent work 70 demonstrates a characteristic impedance Z 0 ≈ 4 kΩ for superconducting nanowire resonators with high kinetic inductance, which leads to g 0 ≈ 2π × 120 MHz and g ≈ 2π × 9 MHz for the same values of ω 0 , v and ξ chosen above.…”
Section: Dipole Coupling Of a Resonant Exchange Qubit To A Transmmentioning
confidence: 99%
“…59 We note that, while the qubit-resonator coupling strength g is limited by the constraint ξ 1 required for the validity of the Heisenberg model description of the RX qubit, 18 the estimate we obtain here does not represent a fundamental limit and varies strongly with the chosen parameters. Further enhancements of g may be possible by, e.g., modifying the design of the transmission line resonator to increase the strength of the electric field within the region containing the RX qubit 60,70 and thus the chargecavity coupling strength g 0 . Recent work 70 demonstrates a characteristic impedance Z 0 ≈ 4 kΩ for superconducting nanowire resonators with high kinetic inductance, which leads to g 0 ≈ 2π × 120 MHz and g ≈ 2π × 9 MHz for the same values of ω 0 , v and ξ chosen above.…”
Section: Dipole Coupling Of a Resonant Exchange Qubit To A Transmmentioning
confidence: 99%
“…However, in this case, the anharmonicity which is inherent to a two level system is lost so that the spin ensemble can only be used as a quantum memory. To remain at the single spin level, it has been suggested to include in the microwave cavity a nanometric constriction to concentrate the cavity field, which would yield g m ∼ 10 kHz 110,111 . Alternatively, various theory Refs.…”
Section: Spin-photon Coupling Due To Spin-orbit Couplingmentioning
confidence: 99%
“…The electrons are confined in a 2DEG at a distance d from a current-carrying wire, which is located above the surface. For our purposes, SC circuits and circuit resonators are attractive because of their capability to generate AC magnetic fields by carry-ing relatively large currents and the possibility to integrate them in semiconductor nanostructures [42,43]. In a simple toy model, we describe the circuit by a meandering wire carrying an AC current ∼ I 0 cos(ωt) through parallel sections of the wire separated by a lattice constant a, see Fig.…”
Section: A Superconducting Circuitmentioning
confidence: 99%