Collective excitations in the 1-D-ferromagnet CsFeCl3 with singlet ground state |
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Authors: | M. Steiner K. Kakurai W. Knop B. Dorner R. Pynn U. Happek P. Day G. McLeen |
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Affiliation: | 1. Hahn-Meitner-Institut für Kernforschung Postfach 390128, D-1000 Berlin 39, W. Germany;2. Institut Laue Langevin, Grenoble, France;3. Institut für Physik III der Universität Regensburg, W. Germany;4. Inorganic Chemistry Laboratory, Oxford University, England |
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Abstract: | By means of inalastic neutron scattering we have determined the dispersion relation of the magnetic excitations in CsFeCl3 at different temperatures.The dispersion in c-direction, along the Fe-chains is typically ferromagnetic and in the hexagonal plane antiferromagnetic. Due to the lack of an applicable theory the data were parametrized by the simple heuristic formula:?ω = [2J[1 - cos πqc] [A + 2J(1 - cos π)qc)] + [C + J' (1.5 + γ(q))]2]The gap was found to be C = 0.148 THz, the easy plane anisotropy A = 0.308 THz, the ferromagnetic interaction J = 0.148 THz and the antiferromagnetic interaction J' = -0.04 THz. At 1.25 K all excitations had a width smaller than the instrumental resolution ΔE = 0.025 THz. These results can be interpreted as follows: CsFeCl3 is a singlet ground state system with strong ferromagnetic interaction J along the crystallographic c-axis and weak antiferromagnetic interaction J' in the plane perpendicular to c.In addition we have measured the influence of a magnetic field along the hexagonal c-axis. The splitting found agrees with the assumed level scheme yielding g = 2.5 for the first excited level. |
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