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

Physica B Condensed Matter

NMR and relaxation in spin-1 Heisenberg antiferromagnetic chain Y2BaNiO5

Fabio Tedoldi, A. Rigamonti

Published Jan 1, 1999• 3 citations
Publisher
DOI
10.1016/s0921-4526(98)00727-3

Related papers

NMR Response in Antiferromagnetic Spin-1/2 Chains

Jesko Sirker, Nicolas Laflorencie

Bulletin of the American Physical Society•Mar 16, 2009•0 citations

Proton relaxation and the dynamics of the S=1/2 antiferromagnetic Heisenberg chain

J Groen

•Oct 27, 1982•0 citations

Boundary effects in finite Heisenberg antiferromagneticS = 1 chains:89Y NMR in Y2BaNi1−xMgxO5

Fabio Tedoldi, A. Rigamonti, Raoul Santachiara +5 more

Applied Magnetic Resonance•Jul 1, 2000•2 citations

NMR relaxation rates of quantum spin chains in magnetic fields

Sei-ichiro Suga, Takahumi Suzuki

Journal of Magnetism and Magnetic Materials•Nov 8, 2006•0 citations

Excitation spectra of the spin-1 antiferromagnetic Heisenberg chain

Makoto Kaburagi, Takashi Tonegawa

Journal of Magnetism and Magnetic Materials•Jan 1, 1998•0 citations

NMR study of lineshifts and relaxation rates of the one-dimensional antiferromagnet LiCuVO4

C. Kegler, Norbert Büttgen, H.‐A. Krug von Nidda +5 more

NMR measurements were performed on single-crystalline samples of the one-dimensional Heisenberg antiferromagnet (1D HAF) ${\mathrm{LiCuVO}}_{4}$. We investigated $^{7}\mathrm{Li}$ and $^{51}\mathrm{V}$ NMR spectra, deduced the respective lineshifts $K(T)$, spin-lattice relaxation rates $1∕{T}_{1}$, and spin-spin relaxation rates $1∕{T}_{2}$ and $1∕{T}_{2G}$. The results are compared to theoretical predictions for the relaxation rates $1∕{T}_{1}(T)$ and $1∕{T}_{2G}(T)$ deduced from the dynamic susceptibility $\ensuremath{\chi}(\mathbf{q},\ensuremath{\omega})$ of a 1D HAF spin chain as proposed by Sachdev [Phys. Rev. B 50, 13006 (1994)]. We document a correspondence between the anisotropic relaxation rates derived from electron paramagnetic resonance linewidth $\mathrm{\ensuremath{\Delta}}H(T)$ and nuclear magnetic resonance $1∕{T}_{1}(T)$, respectively, the former being well described in the framework of symmetric anisotropic exchange interactions for ${\mathrm{LiCuVO}}_{4}$ by Krug von Nidda et al. [Phys. Rev. B 65, 134445 (2002)].

Physical Review B•Mar 15, 2006•21 citations
NMR measurements were performed on single-crystalline samples of the one-dimensional Heisenberg antiferromagnet (1D HAF) LiCuVO4{\mathrm{LiCuVO}}_{4}LiCuVO4​. We investigated 7Li^{7}\mathrm{Li}7Li and 51V^{51}\mathrm{V}51V NMR spectra, deduced the respective lineshifts K(T)K(T)K(T), spin-lattice relaxation rates 1∕T11∕{T}_{1}1∕T1​, and spin-spin relaxation rates 1∕T21∕{T}_{2}1∕T2​ and 1∕T2G1∕{T}_{2G}1∕T2G​. The results are compared to theoretical predictions for the relaxation rates 1∕T1(T)1∕{T}_{1}(T)1∕T1​(T) and 1∕T2G(T)1∕{T}_{2G}(T)1∕T2G​(T) deduced from the dynamic susceptibility $\ensuremath{\chi}(\mathbf{q},\ensuremath{\omega})$ of a 1D HAF spin chain as proposed by Sachdev [Phys. Rev. B 50, 13006 (1994)]. We document a correspondence between the anisotropic relaxation rates derived from electron paramagnetic resonance linewidth $\mathrm{\ensuremath{\Delta}}H(T)$ and nuclear magnetic resonance 1∕T1(T)1∕{T}_{1}(T)1∕T1​(T), respectively, the former being well described in the framework of symmetric anisotropic exchange interactions for LiCuVO4{\mathrm{LiCuVO}}_{4}LiCuVO4​ by Krug von Nidda et al. [Phys. Rev. B 65, 134445 (2002)].