Excitation spectra of the spin-1/2 triangular-lattice Heisenberg antiferromagnet

ArXiv cond-mat/0608008 (2006)

Authors:

Weihong Zheng, John O Fjaerestad, Rajiv RP Singh, Ross H McKenzie, Radu Coldea

Abstract:

We use series expansion methods to calculate the dispersion relation of the one-magnon excitations for the spin-1/2 triangular-lattice nearest-neighbor Heisenberg antiferromagnet above a three-sublattice ordered ground state. Several striking features are observed compared to the classical (large-S) spin-wave spectra. Whereas at low energies the dispersion is only weakly renormalized by quantum fluctuations, significant anomalies are observed at high energies. In particular, we find roton-like minima at special wave-vectors and strong downward renormalization in large parts of the Brillouin zone, leading to very flat or dispersionless modes. We present detailed comparison of our calculated excitation energies in the Brillouin zone with the spin-wave dispersion to order 1/S calculated recently by Starykh, Chubukov, and Abanov [cond-mat/0608002]. We find many common features but also some quantitative and qualitative differences. We show that at temperatures as low as 0.1J the thermally excited rotons make a significant contribution to the entropy. Consequently, unlike for the square lattice model, a non-linear sigma model description of the finite-temperature properties is only applicable at extremely low temperatures.

A reply to the comment by S.E. Sebatian etal.

Physical Review Letters 96:18 (2006)

Authors:

T Radu, H Wilhelm, V Yushankhai, D Kovrizhin, R Coldea, Z Tylczynski, T Lühmann, F Steglich

Anomalous excitation spectra of frustrated quantum antiferromagnets.

Phys Rev Lett 96:5 (2006) 057201

Authors:

Weihong Zheng, John O Fjaerestad, Rajiv RP Singh, Ross H McKenzie, Radu Coldea

Abstract:

We use series expansions to study the excitation spectra of spin-1/2 antiferromagnets on anisotropic triangular lattices. For the isotropic triangular lattice model (TLM), the high-energy spectra show several anomalous features that differ strongly from linear spin-wave theory (LSWT). Even in the Néel phase, the deviations from LSWT increase sharply with frustration, leading to rotonlike minima at special wave vectors. We argue that these results can be interpreted naturally in a spinon language and provide an explanation for the previously observed anomalous finite-temperature properties of the TLM. In the coupled-chains limit, quantum renormalizations strongly enhance the one-dimensionality of the spectra, in agreement with experiments on Cs2CuCl4.

Magnetic phase transitions in the two-dimensional frustrated quantum antiferromagnet Cs2CuCl4

(2006)

Authors:

Y Tokiwa, T Radu, R Coldea, H Wilhelm, Z Tylczynski, F Steglich

Magnetic phase transitions in the two-dimensional frustrated quantum antiferromagnet Cs2CuCl4

ArXiv cond-mat/0601272 (2006)

Authors:

Y Tokiwa, T Radu, R Coldea, H Wilhelm, Z Tylczynski, F Steglich

Abstract:

We report magnetization and specific heat measurements in the 2D frustrated spin-1/2 Heisenberg antiferromagnet Cs2CuCl4 at temperatures down to 0.05 K and high magnetic fields up to 11.5 T applied along a, b and c-axes. The low-field susceptibility chi (T) M/B shows a broad maximum around 2.8 K characteristic of short-range antiferromagnetic correlations and the overall temperature dependence is well described by high temperature series expansion calculations for the partially frustrated triangular lattice with J=4.46 K and J'/J=1/3. At much lower temperatures (< 0.4 K) and in in-plane field (along b and c-axes) several new intermediate-field ordered phases are observed in-between the low-field incommensurate spiral and the high-field saturated ferromagnetic state. The ground state energy extracted from the magnetization curve shows strong zero-point quantum fluctuations in the ground state at low and intermediate fields.