Bose-Einstein Condensation of Magnons in TlCuCl3: Phase diagram and specific heat from a self-consistent Hartee-Fock calculation with a realistic dispersion relation

Abstract

We extend the self-consistent Hartree-Fock-Popov calculations by Nikuni et al. [Phys. Rev. Lett. 84, 5868 (2000)] concerning the Bose-Eistein condensation of magnons in TlCuCl3 to include a realistic dispersion of the excitations. The result for the critical field as a function of temperature behaves as Hc(T)-Hc(0) T^{3/2} below 2K but deviates from this simple power-law at higher temperature and is in very good agreement with the experimental results. The specific heat is computed as a function of temperature for different values of the magnetic field. It shows a lambda-like shape at the transition and is in good qualitative agreement with the results of Oosawa et al. [Phys. Rev. B 63, 134416 (2001)].

arXiv comment7 pages, 6 figures (.eps), submitted to J. Phys. Soc. Jpn

References in corpus (10)

• Realization of Bose-Einstein condensation of dilute magnons in TlCuCl${}_3$
• Critical behavior of the three-dimensional XY universality class
• Magnon Dispersion in the Field-Induced Magnetically Ordered Phase of TlCuCl3
• Observation of Field-Induced Transverse Néel Ordering in the Spin Gap System TlCuCl${}_3$
• Universal scaling at field-induced magnetic phase transitions
• Spin-resonance modes of the spin-gap magnet TlCuCl_3
• Specific Heat Study of the Field-Induced Magnetic Ordering in the Spin Gap System TlCuCl${}_3$
• Sound attenuation on the Bose-Einstein condensation of magnons in TlCuCl_3
• Consequences of spin-orbit coupling for the Bose-Einstein condensation of magnons
• Field-Induced Magnetic Order and Simultaneous Lattice Deformation in TlCuCl3

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