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Characteristic temperatures of a triplon system of dimerized quantum magnets

Abdulla RakhimovDepartment of Physics, Bilkent University, Bilkent, 06800 Ankara, TurkeyMukhtorali NishonovInstitute of Nuclear Physics, 100214 Tashkent, UzbekistanLuxmi RaniDepartment of Physics, Bilkent University, Bilkent, 06800 Ankara, TurkeyBilal TanatarDepartment of Physics, Bilkent University, Bilkent, 06800 Ankara, Turkey
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Exploiting the analogy between ultracold atomic gases and the system of triplons, we study magneto-thermodynamic properties of dimerized quantum magnets in the framework of Bose–Einstein condensation (BEC). Particularly, introducing the inversion (or Joule–Thomson) temperature [Formula: see text] as the point where Joule–Thomson coefficient of an isenthalpic process changes its sign, we show that for a simple paramagnet, this temperature is infinite, while for three-dimensional (3D) dimerized quantum magnets it is finite and always larger than the critical temperature [Formula: see text] of BEC. Below the inversion temperature [Formula: see text], the system of triplons may be in a liquid phase, which undergoes a transition into a superfluid phase at [Formula: see text]. The dependence of the inversion temperature on the external magnetic field [Formula: see text] has been calculated for quantum magnets of TlCuCl 3 and Sr 3 Cr 2 O 8 .

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