S. Glancy

High-fidelity laser-free universal control of two trapped ion qubits

R. Srinivas [1,2], S. C. Burd [1,2], H. M. Knaack [1,2], R. T. Sutherland [3,4], A. Kwiatkowski [1,2], S. Glancy [1], E. Knill [1,5], D. J. Wineland [1,2,6], D. Leibfried [1], A. C. Wilson [1], D. T. C. Allcock [1,2,6], D. H. Slichter [1]

Abstract

Universal control of multiple qubits -- the ability to entangle qubits and to perform arbitrary individual qubit operations -- is a fundamental resource for quantum computation, simulation, and networking. Here, we implement a new laser-free scheme for universal control of trapped ion qubits based on microwave magnetic fields and radiofrequency magnetic field gradients. We demonstrate high-fidelity entanglement and individual control by creating symmetric and antisymmetric two-qubit maximally entangled states with fidelities in the intervals [0.9983, 1] and [0.9964, 0.9988], respectively, at 68% confidence, corrected for state initialization error. This technique is robust against multiple sources of decoherence, usable with essentially any trapped ion species, and has the potential to perform simultaneous entangling operations on many pairs of ions without increasing control signal power or complexity.

Preparation of entangled states through Hilbert space engineering

Y. Lin [1], J. P. Gaebler [1], F. Reiter [2], T. R. Tan [1], R. Bowler [1], Y. Wan [1], A. Keith [1], E. Knill [1], S. Glancy [1], K. Coakley [1,2], A. S. Sørensen, D. Leibfried [1], D. J. Wineland [1]

Abstract

Entangled states are a crucial resource for quantum-based technologies such as quantum computers and quantum communication systems (1,2). Exploring new methods for entanglement generation is important for diversifying and eventually improving current approaches. Here, we create entanglement in atomic ions by applying laser fields to constrain the evolution to a restricted number of states, in an approach that has become known as "quantum Zeno dynamics" (3-5). With two trapped $^9\rm{Be}^+$ ions, we obtain Bell state fidelities up to $0.990^{+2}_{-5}$, with three ions, a W-state (6) fidelity of $0.910^{+4}_{-7}$ is obtained. Compared to other methods of producing entanglement in trapped ions, this procedure is relatively insensitive to certain imperfections such as fluctuations in laser intensity, laser frequency, and ion-motion frequencies.