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Regensburg 1998 – wissenschaftliches Programm

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TT: Tiefe Temperaturen

TT 21: Postersitzung III: Spin-Peierls-Systeme, Metall-Isolator-Übergang, Lokalisierung; SL: Theorie; Quantenflüssigkeiten und -kristalle; Amorphe Materialien, Tunnelsysteme; Borcarbide, Fullerene, konventionelle SL; SL dünner Filme; Experimentiertechniken

TT 21.32: Poster

Donnerstag, 26. März 1998, 15:00–18:30, D

Raman Scattering on the S=1/2 Alternating Chain Compound (VO)2P2O7 — •M. Grove1, P. Lemmens1, G. Güntherodt1, and B.C. Sales212. Physikalisches Institut, RWTH Aachen, 52056 Aachen — 2Oak Ridge National Laboratory, Oak Ridge, Tennessee, USA

Recently it was shown by inelastic neutron scattering experiments that the compound (VO)2P2O7 is best described as an alternating spin chain with the chains running along b direction [1]. Magnetic triplet excitations have been found with a magnetic zone-center energy gap Δ01=3.1 meV. A second excitation is observed at Δ11=5.8 meV, an energy just below 2Δ01. This mode is interpreted as a triplet two-magnon bound state.

(VO)2P2O7 single crystals have been investigated by means of Raman scattering. At low temperatures (5 K) an additional shoulder appears at 50 cm−1 (6.2 meV) for aa- and bb-polarizations due to two-magnon scattering from the Δ01-branch. We observe a decrease of the scattering intensity at 50 cm−1 on warming up with two temperature regimes. One for 5 K ≤ T ≤ 20 K and another regime for 20 K ≤ T ≤ 55 K (aa-geometry) or 20 K ≤ T ≤ 70 K (2Δ01=72 K) (bb-geometry). In aa-geometry quasielastic scattering due to fluctuations in the spin system can be observed for temperatures above 55 K.
Work supported by DFG through SFB 341 and BMBF Fkz. 13N6586

[1] A.W. Garrett, S.E. Nagler, D.A. Tennant, B.C. Sales, T. Barnes, Phys. Rev. Lett. 79(4), 745 (1997)

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