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Single trapped ion

Single trapped ion

Credit: David Nadlinger

David Lucas

Professor of Physics

Sub department

  • Atomic and Laser Physics

Research groups

  • Ion trap quantum computing
David.Lucas@physics.ox.ac.uk
Telephone: 01865 (2)72384,01865 (2)72346
Clarendon Laboratory, room -170,-172,-171,316.6
  • About
  • Publications

The effect of atomic response time in the theory of Doppler cooling of trapped ions

JOURNAL OF MODERN OPTICS 65:5-6 (2018) 577-584

Authors:

H Janacek, AM Steane, DM Lucas, DN Stacey

A short response-time atomic source for trapped ion experiments

(2017)

Authors:

Timothy G Ballance, Joseph F Goodwin, Bethan Nichol, Laurent J Stephenson, Christopher J Ballance, David M Lucas

Fast quantum logic gates with trapped-ion qubits

(2017)

Authors:

VM Sch盲fer, CJ Ballance, K Thirumalai, LJ Stephenson, TG Ballance, AM Steane, DM Lucas

The effect of atomic response time in the theory of Doppler cooling of trapped ions

(2017)

Authors:

H Janacek, AM Steane, DM Lucas, DN Stacey

High-fidelity spatial and polarization addressing of 43Ca+ qubits using near-field microwave control

Physical Review A American Physical Society 95:2 (2017) 022337

Authors:

Diana PL Aude Craik, Norbert M Linke, Martin A Sepiol, Thomas Harty, Joseph Goodwin, Christopher J Ballance, Derek Stacey, Andrew Steane, David M Lucas, David TC Allcock

Abstract:

Individual addressing of qubits is essential for scalable quantum computation. Spatial addressing allows unlimited numbers of qubits to share the same frequency, whilst enabling arbitrary parallel operations. We demonstrate addressing of long-lived $^{43}\text{Ca}^+$ "atomic clock" qubits held in separate zones ($960\mu$m apart) of a microfabricated surface trap with integrated microwave electrodes. Such zones could form part of a "quantum CCD" architecture for a large-scale quantum information processor. By coherently cancelling the microwave field in one zone we measure a ratio of Rabi frequencies between addressed and non-addressed qubits of up to 1400, from which we calculate a spin-flip probability on the qubit transition of the non-addressed ion of $1.3\times 10^{-6}$. Off-resonant excitation then becomes the dominant error process, at around $5 \times 10^{-3}$. It can be prevented either by working at higher magnetic field, or by polarization control of the microwave field. We implement polarization control with error $2 \times 10^{-5}$, which would suffice to suppress off-resonant excitation to the $\sim 10^{-9}$ level if combined with spatial addressing. Such polarization control could also enable fast microwave operations.

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