Abstract
The effect of exchange randomness on field-induced magnetic ordering was investigated through specific heat measurements in Tl 1- x K x CuCl 3 with x ≤0.22. The isostructural parent compounds TlCuCl 3 and KCuCl 3 are coupled spin dimer systems with a gapped ground state and their field-induced antiferromagnetic ordering is described by the Bose–Einstein condensation (BEC) of spin triplets. Well-defined field-induced phase transitions were observed in Tl 1- x K x CuCl 3 . The critical exponent φ of the phase boundary defined by T ( H ) ∝( H - H c ) 1/φ is reevaluated in TlCuCl 3 as φ=1.67 ±0.07, which is close to φ BEC =3/2 derived from the magnon BEC theory. For x ≠0, the exponent φ decreases systematically with x . The phase boundary observed below 2 K for x >0.1 approximates a linear function of temperature T . In the low-field region for H < H c , no magnetic ordering is observed despite finite susceptibility. These properties are discussed in connection with the Bose glass phase argued by Fisher et al...
Highlights
The effect of exchange randomness on field-induced magnetic ordering was investigated through specific heat measurements in Tl1x Kx CuCl3 with x 0:22
TlCuCl3 and KCuCl3 are coupled spin dimer systems with a gapped ground state and their field-induced antiferromagnetic ordering is described by the Bose–Einstein condensation (BEC) of spin triplets
The critical exponent of the phase boundary defined by TðHÞ / ðH Hc Þ1= is reevaluated in TlCuCl3 as 1⁄4 1:67 0:07, which is close to BEC 1⁄4 3=2 derived from the magnon BEC theory
Summary
The effect of exchange randomness on field-induced magnetic ordering was investigated through specific heat measurements in Tl1x Kx CuCl3 with x 0:22. Welldefined field-induced phase transitions were observed in Tl1x Kx CuCl3 .
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