50th Annual Meeting of the APS Division of Atomic, Molecular and Optical Physics APS Meeting
Volume 64, Number 4
Monday–Friday, May 27–31, 2019;
Milwaukee, Wisconsin
Session H08: Continuous Variable Quantum Information Processing
8:00 AM–10:00 AM,
Wednesday, May 29, 2019
Wisconsin Center
Room: 103C
Co-Sponsoring
Unit:
DQI
Chair: Ivan Deutsch, University of New Mexico
Abstract: H08.00001 : Large-Scale Quantum Simulators and Quantum Computers over Continuous Variables: Theory and Experiment*
8:00 AM–8:30 AM
Preview Abstract
Abstract
Author:
Olivier Pfister
(University of Virginia)
Continuous-variable (CV) quantum computing [1,2] is based on
harmonic-oscillator qumodes such as position and momentum, or the two
quadrature amplitudes of the quantized electromagnetic field, rather than on
qubit- or qudit-based discrete encodings. It is a viable approach for which
error correction [3] and fault tolerance [4] have been elucidated. It is
particularly well suited to electromagnetic qumodes, which scale up very
well as the resonant modes of a single optical cavity, such as that of an
optical parametric oscillator, analogously to the classical optical
frequency comb of a femtosecond laser. This allows cluster entangled states,
which are quantum-computing ``substrates'' [5] in a sense, to be implemented
over CV [6] on very large scales [7] as was experimentally demonstrated in
the quantum optical frequency comb of a single OPO (60 entangled qumodes,
simultaneously accessible) [8]. Note that sequential time-bin
implementations are also possible (one million entangled qumodes, accessible
two at a time) [9]. This paves the way to realizing interesting testbeds for
bosonic, and possibly more general, quantum simulation [10]. In this talk, I
will present the fundamentals of scalable CV cluster state generation in
quantum optics, experimental realizations on five different continents, and
applications to quantum simulation.
[1] S. Lloyd and S.L. Braunstein, PRL \textbf{82}, 1784 (1999)
[2] S.D. Bartlett, B.C. Sanders, S.L. Braunstein, K. Nemoto, PRL
\textbf{88}, 097904 (2002)
[3] D. Gottesman, A. Kitaev, and J. Preskill, PRA \textbf{64}, 012310 (2001)
[4] N.C. Menicucci, PRL \textbf{112}, 120504 (2014)
[5] R. Raussendorf and H.-J. Briegel, PRL \textbf{86}, 5188 (2001)
[6] N.C. Menicucci \textit{et al.}, PRL \textbf{97}, 110501 (2006)
[7] O. Pfister \textit{et al.}, PRA \textbf{70}, 020302 (2004)
[8] M. Chen, N.C. Menicucci, and O. Pfister, PRL \textbf{112}, 120505 (2014)
[9] J.-I. Yoshikawa \textit{et al.}, APL Photonics \textbf{1}, 060801 (2016)
[10] K. Marshall, R. Pooser, G. Siopsis, and Ch. Weedbrook, PRA \textbf{92},
063825 (2015)
*This work was supported by the U.S. National Science Foundation.