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

Comment on "Spin dynamics of the 2D spin 1/2 quantum antiferromagnet copper deuteroformate tetradeuterate (CFTD)" - Reply

Henrik Moodysson Rønnow, MCMORROW Desmond Francis, R. Coldea, Andrew Harrison, I. D. Youngson, T. G. Perring, G. Aeppli, Olav F. Syljuåsen, Kim Lefmann, Christian Rischel

Published Jan 1, 2002• 1 citation
Publisher

Abstract

LQM
DOI
10.1103/physrevlett.89.079702

Related papers

Comment on “Spin Dynamics of the 2D Spin 12 Quantum Antiferromagnet Copper Deuteroformate Tetradeuterate (CFTD)”

Peter Kopietz, Ivan Spremo

Comment on "Spin Dynamics of the 2D Spin 1/2 Quantum Antiferromagnet Copper Deuteroformate Tetradeuterate (CFTD)", H. M. Ronnow et al., Phys. Rev. Lett. 87, 037202 (2001)

arXiv:cond-mat/0206106•Physical Review Letters•Jul 30, 2002•2 citations

Spin Dynamics of the 2D Spin Quantum Antiferromagnet Copper Deuteroformate Tetradeuterate (CFTD)

Christian Rischel

Complex Systems

•Jan 1, 2001•0 citations

Quantum Dynamics of Spins on a Square Lattice

Henrik Moodysson Rønnow

LQM

•Jan 1, 2009•0 citations

Critical spin dynamics of the 2D quantum Heisenberg antiferromagnets

Y. J. Kim, R. J. Birgeneau, F. C. Chou +2 more

APS•Mar 1, 2001•0 citations

Addendum to “Spin Dynamics in Two-Dimensional Quantum Heisenberg Antiferromagnets”

Tatsuya Nagao, Jun-ichi Igarashi

Journal of the Physical Society of Japan•Sep 1, 1999•0 citations

Spin Dynamics of the 2D Spin 12 Quantum Antiferromagnet Copper Deuteroformate Tetradeuterate (CFTD)

Henrik Moodysson Rønnow, MCMORROW Desmond Francis, R. Coldea +7 more

The magnetic excitation spectrum in the two-dimensional (2D) $S\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}1/2$ Heisenberg antiferromagnet copper deuteroformate tetradeuterate has been measured for temperatures up to $T\ensuremath{\sim}J/2$, where $J\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}6.31\ifmmode\pm\else\textpm\fi{}0.02\mathrm{meV}$ is the 2D exchange coupling. For $T\ensuremath{\ll}J$, a dispersion of the zone boundary energy is observed, which is attributed to a wave vector dependent quantum renormalization. At higher temperatures, spin-wavelike excitations persist, but are found to broaden and soften. By combining our data with numerical calculations, and with existing theoretical work, a consistent description of the behavior of the model system is found over the whole temperature interval investigated.

Physical Review Letters•Jun 28, 2001•114 citations
The magnetic excitation spectrum in the two-dimensional (2D) S=1/2S\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}1/2S=1/2 Heisenberg antiferromagnet copper deuteroformate tetradeuterate has been measured for temperatures up to $T\ensuremath{\sim}J/2$, where $J\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}6.31\ifmmode\pm\else\textpm\fi{}0.02\mathrm{meV}$ is the 2D exchange coupling. For $T\ensuremath{\ll}J$, a dispersion of the zone boundary energy is observed, which is attributed to a wave vector dependent quantum renormalization. At higher temperatures, spin-wavelike excitations persist, but are found to broaden and soften. By combining our data with numerical calculations, and with existing theoretical work, a consistent description of the behavior of the model system is found over the whole temperature interval investigated.