Document Type
Article
Date of Original Version
10-1-1976
Abstract
The spin-Peierls transition is considered as a progressive spin-lattice dimerization occurring below a transition temperature in a system of one-dimensional antiferromagnetic Heisenberg chains. In the simplest theories, the transition is second order and the ground state is a singlet with a magnetic gap. The historical origins and theoretical development of the concept are examined. Magnetic susceptibility and EPR measurements on the π-donor-acceptor compounds TTF·MS4C4(CF3)4 (M=Cu, Au; TTF is tetrathiafulvalene) are reported. These compounds exhibit clearly the characteristics of the spin-Peierls transition in reasonably good agreement with a mean-field theory. The susceptibility of each compound has a broad maximum near 50 K, while the transitions occur at 12 and 2.1 K for M=Cu and Au, respectively. EPR linewidth observations over a broad temperature range are examined. Areas for further experimental and theoretical work are indicated, and a critical comparison is made of related observations on other materials.
Citation/Publisher Attribution
Jacobs, I. S., Bray, J. W., Hart, H. R., Interrrante, L. V., Kasper, J. S., Watkins, G. D., Prober, D. E., & Bonner, J. C. (1976). Phys. Rev. B, 14(7), 3036-3051. doi: 10.1103/PhysRevB.14.3036
Available at: http://dx.doi.org/10.1103/PhysRevB.14.3036
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