49th Annual Meeting of the APS Division of Atomic, Molecular and Optical Physics APS Meeting 
Volume 63, Number 5
Monday–Friday, May 28–June 1 2018;
Ft. Lauderdale, Florida
Session R09: Quantum Control and Simulation
10:30 AM–12:30 PM, 
Thursday, May 31, 2018
Room: Grand H
Co-Sponsoring
Unit: 
DQI
Chair: Ken Brown, Duke University
Abstract ID: BAPS.2018.DAMOP.R09.2
Abstract: R09.00002 : A Universal Analog Quantum Simulator Using Atomic Spins*
11:00 AM–11:30 AM
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 Abstract
  Abstract   
Author:
Poul Jessen
(University of Arizona)
Progress in quantum information science has created a need for 
experimental platforms that lend themselves to critical evaluation of 
various paradigms for quantum control and diagnostics. We have developed one 
such platform using the electron-nuclear spins of individual Cs atoms, 
forming a 16-dimensional state space that is fully controllable with phase 
modulated radio-frequency and microwave magnetic fields. Recent work 
includes the implementation of arbitrary unitary control with 
state-of-the-art fidelity, and a comparison of optimal strategies for 
quantum state tomography. The degree of control achievable with this system 
also allows it to be used as a universal, high-fidelity Analog Quantum 
Simulator. Broadly defined, an AQS is a controllable quantum system whose 
time evolution can emulate a Hamiltonian of interest. If used to simulate 
complex dynamics without error correction such a device becomes vulnerable 
to exponential loss of precision due to small imperfections. In the 
classical world this phenomenon manifests itself as deterministic chaos, 
wherein small perturbations are exponentially amplified over time. Given 
that imperfections are unavoidable in the real world, this raises the 
fundamental question whether one can trust the output of an AQS. As a step 
towards addressing these issues, we are using our AQS to simulate a popular 
paradigm for quantum chaos, the Quantum Kicked Top, consisting of a 
periodically driven spin whose classical phase space can be regular, 
chaotic, or mixed. For our work we pick a spin $J=$15/2, map the 
2$J+$1$=$16 spin states onto our AQS, and use optimal control to drive up to 
a few hundred periods of the QKT dynamics. Our experimental results shed 
light on several questions of general interest: Is there an optimal map from 
system to simulator? How accurate must the control be to allow meaningful 
simulation? And how long can we simulate before the physics of interest 
(phase space structure, critical points, scrambling, etc.) is compromised by 
control errors?
*This work was funded by the National Science Foundation
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2018.DAMOP.R09.2