APS March Meeting 2017
Volume 62, Number 4
Monday–Friday, March 13–17, 2017;
New Orleans, Louisiana
Session B19: Progress in Quantum Simulation
11:15 AM–2:15 PM,
Monday, March 13, 2017
Room: 278-279
Sponsoring
Units:
GQI DAMOP
Chair: Ivan Deutsch, University of New Mexico
Abstract ID: BAPS.2017.MAR.B19.2
Abstract: B19.00002 : Quantum simulation of the spin-boson model: monitoring the bath
11:51 AM–12:27 PM
Preview Abstract
Abstract
Author:
Nicolas Roch
(Institut Néel, CNRS and Université Grenoble Alpes, F-38042 Grenoble, France)
The spin-boson model
occupies a central position in condensed matter physics. It describes the
interaction between a two-level system and a collection of harmonic
oscillators or dissipative bath. It was originally developed as a general,
fully quantum-mechanical, framework to account for the dissipation inherent
to any quantum system [1]. This formalism was successfully applied to
various physical systems weakly coupled to a bosonic bath (mesoscopic
circuits, amorphous solids\textellipsis ). However only a few experiments
[2,3] explored its more challenging limit -when the quantum system is
strongly coupled to the many degrees of freedom of the bath - despite
numerous theoretical predictions. In this regime the ground state of the
whole system is non-trivial: the spin is highly entangled with the bath,
forming a many-body system. I will present a new architecture based on
superconducting circuits to tackle this challenging problem. It offers two
main advantages: first it allows to reach the ultra-strong coupling between
the quantum system and its bath; second one can experimentally monitor the
qubit and its bath at the same time, and thus reveal the many-body
correlations which are building up when all the degrees of freedom become
entangled. Our approach consists in coupling a superconducting artificial
atom (namely a transmon qubit) to a meta-material made of thousands of
SQUIDs. The latter sustains many photonic modes and shows characteristic
impedance close to the quantum of resistance. As a direct application, we
use this circuit to explore quantum optics in the ultrastrong coupling
regime, where new phenomena arise [4--7]. [1] Leggett, A. et al., Rev. Mod.
Phys. 59(1), 1 (1987). [2] Forn-D\'{\i}az, P. et al., Nat. Phys. AOP (2016).
[3] Haeberlein, M. et al., arXiv: 1506.09114 (2015). [4] Le Hur K., Phys.
Rev. B 85, 140506(R) (2012). [5] Goldstein M. et al., Phys. Rev. Lett. 110,
017002 (2013). [6] Gheeraert N. et al., arXiv :1601.01545 (2015). [7]
Yoshihara F. et al., Nat. Phys. AOP (2016).
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2017.MAR.B19.2