corner
corner

Phys. Rev. B 75, 165417 (2007) [11 pages]

Quantum electromechanics: Quantum tunneling near resonance and qubits from buckling nanoscale bars

Download: PDF (608 kB) Buy this article Export: BibTeX or EndNote (RIS)

Sergey Savel’ev1,2, A. L. Rakhmanov1,3, Xuedong Hu1,4, A. Kasumov5, and Franco Nori1,6
1Frontier Research System, The Institute of Physical and Chemical Research (RIKEN), Wako-shi, Saitama, 351-0198, Japan
2Department of Physics, Loughborough University, Loughborough LE11 3TU, United Kingdom
3Institute for Theoretical and Applied Electrodynamics RAS, 125412 Moscow, Russia
4Department of Physics, University at Buffalo, SUNY, Buffalo, New York 14260-1500, USA
5Laboratoire de Physique des Solides, Associé au CNRS, Université Paris-Sud, F-91405, Orsay, France
6Center for Theoretical Physics, Department of Physics, University of Michigan, Ann Arbor, Michigan 48109-1040, USA

Received 31 August 2005; revised 29 December 2006; published 25 April 2007

Analyzing recent experimental results [ Reulet et al. Phys. Rev. Lett. 85 2829 (2000); Izmalkov et al. Europhys. Lett. 65 844 (2004)], we find strikingly similar behaviors between two very different systems: three-junction superconducting qubits and suspended carbon nanotubes. When these different systems are ac-driven near their resonances, the resonance single-peak, observed at weak driving amplitudes, splits into two subpeaks for strong driving amplitudes. We describe this unusual behavior by considering quantum tunneling in a double well potential. Inspired by these experiments, we propose a mechanical qubit based on buckling nanoscale bars (nanobars)—a nanoelectromechanical system so small as to be quantum coherent. We consider how this nanomechanical qubit can be manipulated. A comparison between nanobars and superconducting qubits suggests several future experiments on quantum electromechanics.

© 2007 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.75.165417
DOI:
10.1103/PhysRevB.75.165417
PACS:
85.85.+j, 85.35.Be, 85.35.Kt, 74.50.+r