S. A. King

Scalable, high-fidelity all-electronic control of trapped-ion qubits

C. M. Löschnauer, J. Mosca Toba [1], A. C. Hughes [1], S. A. King [1], M. A. Weber [1], R. Srinivas [1,2], R. Matt [1], R. Nourshargh [1], D. T. C. Allcock [1,3], C. J. Ballance [1,2], C. Matthiesen [1], M. Malinowski [1], T. P. Harty [1]

Abstract

The central challenge of quantum computing is implementing high-fidelity quantum gates at scale. However, many existing approaches to qubit control suffer from a scale-performance trade-off, impeding progress towards the creation of useful devices. Here, we present a vision for an electronically controlled trapped-ion quantum computer that alleviates this bottleneck. Our architecture utilizes shared current-carrying traces and local tuning electrodes in a microfabricated chip to perform quantum gates with low noise and crosstalk regardless of device size. To verify our approach, we experimentally demonstrate low-noise site-selective single- and two-qubit gates in a seven-zone ion trap that can control up to 10 qubits. We implement electronic single-qubit gates with 99.99916(7)% fidelity, and demonstrate consistent performance with low crosstalk across the device. We also electronically generate two-qubit maximally entangled states with 99.97(1)% fidelity and long-term stable performance over continuous system operation. These state-of-the-art results validate the path to directly scaling these techniques to large-scale quantum computers based on electronically controlled trapped-ion qubits.

Coherent Control of Trapped Ion Qubits with Localized Electric Fields

R. Srinivas [1,2], C. M. Löschnauer, M. Malinowski [1], A. C. Hughes [1], R. Nourshargh [1], V. Negnevitsky [1], D. T. C. Allcock [1,3], S. A. King [1], C. Matthiesen [1], T. P. Harty [1], C. J. Ballance [1,2]

Abstract

We present a new method for coherent control of trapped ion qubits in separate interaction regions of a multi-zone trap by simultaneously applying an electric field and a spin-dependent gradient. Both the phase and amplitude of the effective single-qubit rotation depend on the electric field, which can be localised to each zone. We demonstrate this interaction on a single ion using both laser-based and magnetic field gradients in a surface-electrode ion trap, and measure the localisation of the electric field.

An ultralow-noise superconducting radio-frequency ion trap for frequency metrology with highly charged ions

J. Stark [1,2], C. Warnecke [1,2], S. Bogen [1], S. Chen [1,3], E. A. Dijck [1,2], S. Kühn, M. K. Rosner [1,2], A. Graf [1], J. Nauta [1,2], J. -H. Oelmann [1,2,4], L. Schmöger, M. Schwarz [1,4], D. Liebert [1,4], L. J. Spieß, S. A. King [4], T. Leopold [4], P. Micke [1,4], P. O. Schmidt [4,5], T. Pfeifer [1], J. R. Crespo López-Urrutia

Abstract

We present a novel ultrastable superconducting radio-frequency (RF) ion trap realized as a combination of an RF cavity and a linear Paul trap. Its RF quadrupole mode at 34.52 MHz reaches a quality factor of $Q\approx2.3\times 10^5$ at a temperature of 4.1 K and is used to radially confine ions in an ultralow-noise pseudopotential. This concept is expected to strongly suppress motional heating rates and related frequency shifts which limit the ultimate accuracy achieved in advanced ion traps for frequency metrology. Running with its low-vibration cryogenic cooling system, electron beam ion trap and deceleration beamline supplying highly charged ions (HCI), the superconducting trap offers ideal conditions for optical frequency metrology with ionic species. We report its proof-of-principle operation as a quadrupole mass filter with HCI, and trapping of Doppler-cooled ${}^9\text{Be}^+$ Coulomb crystals.

Closed-cycle, low-vibration 4 K cryostat for ion traps and other applications

P. Micke [1,2], J. Stark [1,3], S. A. King [2], T. Leopold [2], T. Pfeifer [1,2], L. Schmöger, M. Schwarz [1,2], L. J. Spieß, P. O. Schmidt [2,4,1], J. R. Crespo López-Urrutia

Abstract

In-vacuo cryogenic environments are ideal for applications requiring both low temperatures and extremely low particle densities. This enables reaching long storage and coherence times for example in ion traps, essential requirements for experiments with highly charged ions, quantum computation, and optical clocks. We have developed a novel cryostat continuously refrigerated with a pulse-tube cryocooler and providing the lowest vibration level reported for such a closed-cycle system with 1 W cooling power for a <5 K experiment. A decoupling system suppresses vibrations from the cryocooler by three orders of magnitude down to a level of 10 nm peak amplitudes in the horizontal plane. Heat loads of about 40 W (at 45 K) and 1 W (at 4 K) are transferred from an experimental chamber, mounted on an optical table, to the cryocooler through a vacuum-insulated massive 120 kg inertial copper pendulum. The 1.4 m long pendulum allows installation of the cryocooler in a separate, acoustically isolated machine room. In the laser laboratory, we measured the residual vibrations using an interferometric setup. The positioning of the 4 K elements is reproduced to better than a few micrometer after a full thermal cycle to room temperature. Extreme high vacuum on the $10^{-15}$ mbar level is achieved. In collaboration with the Max-Planck-Intitut für Kernphysik (MPIK), such a setup is now in operation at the Physikalisch-Technische Bundesanstalt (PTB) for a next-generation optical clock experiment using highly charged ions.

A Single-Ion Trap with Minimized Ion-Environment Interactions

P. B. R. Nisbet-Jones, S. A. King, J. M. Jones, R. M. Godun, C. F. A. Baynham, K. Bongs, M. Doležal, P. Balling, P. Gill

Abstract

We present a new single-ion endcap trap for high precision spectroscopy that has been designed to minimize ion-environment interactions. We describe the design in detail and then characterize the working trap using a single trapped 171 Yb ion. Excess micromotion has been eliminated to the resolution of the detection method and the trap exhibits an anomalous phonon heating rate of d<n> /dt = 24 +30/-24 per second. The thermal properties of the trap structure have also been measured with an effective temperature rise at the ion's position of 0.14 +/- 0.14 K. The small perturbations to the ion caused by this trap make it suitable to be used for an optical frequency standard with fractional uncertainties below the 10^-18 level.