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Magnon Dispersion in the Field-Induced Magnetically Ordered Phase of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msub><mml:mrow><mml:mi mathvariant="normal">T</mml:mi><mml:mi mathvariant="normal">l</mml:mi><mml:mi mathvariant="normal">C</mml:mi><mml:mi mathvariant="normal">u</mml:mi><mml:mi mathvariant="normal">C</mml:mi><mml:mi mathvariant="normal">l</mml:mi></mml:mrow><mml:mn>3</mml:mn></mml:msub></mml:math>

M. MatsumotoTheoretische Physik, ETH-Hönggerberg, CH-8093 Zürich, SwitzerlandB. NormandDépartement de Physique, Université de Fribourg, CH-1700 Fribourg, SwitzerlandT. M. RiceTheoretische Physik, ETH-Hönggerberg, CH-8093 Zürich, SwitzerlandManfred SigristTheoretische Physik, ETH-Hönggerberg, CH-8093 Zürich, Switzerland
2002lv
ABI

Аннотация

The magnetic properties of the interacting dimer system TlCuCl3 are investigated within a bond-operator formulation. The observed field-induced staggered magnetic order perpendicular to the field is described as a Bose condensation of magnons which are linear combinations of dimer singlet and triplet modes. This technique accounts for the magnetization curve and for the field dependence of the magnon dispersion curves observed by high-field neutron scattering measurements.

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