Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Bulletin of the American Physical Society

Phonon down-conversion in a linear ion trap

Shiqian Ding, Gleb Maslennikov, Roland Hablützel, Huanqian Loh, Dzmitry Matsukevich

Published Jun 9, 2015• 0 citations
OpenAlex

Related papers

Phonon-phonon interactions due to non-linear effects in a linear ion trap

Cyrille Marquet, Ferdinand Schmidt‐Kaler, Daniel F. V. James

arXiv:quant-ph/0211079•Applied Physics B•Mar 1, 2003•80 citations

Linear mode-mixing of phonons with trapped ions

Kevin Marshall, Daniel F. V. James

arXiv:1610.04803•Applied Physics B•Dec 24, 2016•6 citations

Phonon-number-resolving detection of multiple local phonon modes in trapped ions

Takashi Mukaiyama

•Jan 1, 2019•0 citations

Phonon-number-resolving detection of multiple radial phonon modes with trapped ions

Yoshikazu MARUHASHI

The International Commission for Optics•May 16, 2017•0 citations

Phonon-phonon interactions in a linear ion trap

Shiqian Ding, Gleb Maslennikov, Roland Hablützel +2 more

We observe nonlinear coupling of phonons between radial and axial directions in a system of two ions in a linear Paul trap. Anticrossing of phonon modes and adiabatic energy transfer are demonstrated.

Conference on Lasers and Electro-Optics Pacific Rim (CLEO-PR)•Aug 1, 2015•0 citations

Maximum quantum entanglement and linearity in the second-order terms of the Lamb–Dicke parameter

Rasim Dermez, Soner Özen

In this work, the quantum entanglement and quantum linearity in a trapped ion–phonon system are theoretically explained in terms of the second-order terms of the Lamb–Dicke parameter, η . For the trapped ion–phonon system, the optimum times are 2 and 10 and the optimum probability amplitudes of ions are 0.4 and 0.58, respectively. With the optimum times and amplitudes, it is shown that as η grows, the quality of the entanglement in the trapped ion–phonon system increases. In particular, we have demonstrated the quantum linearity due to second-order terms of η .

Physica Scripta•May 1, 2012•8 citations
In this work, the quantum entanglement and quantum linearity in a trapped ion–phonon system are theoretically explained in terms of the second-order terms of the Lamb–Dicke parameter, η . For the trapped ion–phonon system, the optimum times are 2 and 10 and the optimum probability amplitudes of ions are 0.4 and 0.58, respectively. With the optimum times and amplitudes, it is shown that as η grows, the quality of the entanglement in the trapped ion–phonon system increases. In particular, we have demonstrated the quantum linearity due to second-order terms of η .