Spin dynamics in the high-field phase of quantum-critical S = 1/2 TlCuCl3

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Abstract

An external magnetic field suppresses the spin-energy gap in singlet ground state S = 1/2 TlCuCl3. The system becomes quantum-critical at Hc ≈ 5.7 T, where the energy of the lowest Zeeman-split triplet excitation crosses the nonmagnetic ground state. Antiferromagnetic ordering is reported above Hc, which underlines the three-dimensional nature of the observed quantum phase transition. The intrinsic parameters of S = 1/2 TlCuCl3 allow us to access the critical region microscopically by neutron scattering. A substantial study of the spin dynamics in the high-field phase of TlCuCl3 at T = 1.5 K up to H = 12 T was performed for the first time. The results possibly indicate two dynamical regimes, which can be understood within characteristically renormalized triplet modes and a low-lying dynamics of potentially collective origin.

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Rüegg, C., Cavadini, N., Furrer, A., Krämer, K., Güdel, H. U., Vorderwisch, P., & Mutka, H. (2002). Spin dynamics in the high-field phase of quantum-critical S = 1/2 TlCuCl3. Applied Physics A: Materials Science and Processing, 74(SUPPL.I). https://doi.org/10.1007/s003390101156

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