Heisenberg spin triangles in{ V 6 } -type magnetic molecules: Experiment and theory
Author(s) -
Marshall Luban,
F. Borsa,
Sergey L. Bud’ko,
P. C. Canfield,
Suckjoon Jun,
Jae Kap Jung,
Paul Kögerler,
Detlef Mentrup,
Achim Müller,
R. Modler,
Daniele Procissi,
Byoung Jin Suh,
M. S. Torikachvili
Publication year - 2002
Publication title -
physical review. b, condensed matter
Language(s) - English
Resource type - Journals
eISSN - 1095-3795
pISSN - 0163-1829
DOI - 10.1103/physrevb.66.054407
Subject(s) - antiferromagnetism , physics , heisenberg model , magnetization , spins , condensed matter physics , ground state , spin (aerodynamics) , magnetic susceptibility , magnetic field , atomic physics , quantum mechanics , thermodynamics
We report the results of systematic experimental and theoretical studies of two closely related species of magnetic molecules of the type ${{\mathrm{V}}_{6}},$ where each molecule includes a pair of triangles of exchange-coupled vanadyl $({\mathrm{VO}}^{2+},$ spin $s=1/2)$ ions. The experimental studies include the temperature dependence of the low-field susceptibility from room temperature down to 2 K, the dependence of the magnetization on magnetic field up to 60 T for several low temperatures, the temperature dependence of the magnetic contribution to the specific heat, and the ${}^{1}\mathrm{H}$ and ${}^{23}\mathrm{Na}$ nuclear magnetic resonance spin-lattice relaxation rates ${1/T}_{1}.$ This body of experimental data is accurately reproduced for both compounds by a Heisenberg model for two identical uncoupled triangles of spins; in each triangle, the spins interact via isotropic antiferromagnetic exchange, where two of the three V-V interactions have exchange constants that are equal and an order of magnitude larger than the third; the ground-state eigenfunction has total spin quantum number $S=1/2$ for magnetic fields below a predicted critical field ${H}_{c}\ensuremath{\approx}74\mathrm{T}$ and $S=3/2$ for fields above ${H}_{c}.$
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