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Field-Induced Magnetic Long-Range Order in the Ferromagnetic-Antiferromagnetic Alternating Heisenberg Chain System (CH<sub><b> 3</b></sub>)<sub><b> 2</b></sub>CHNH<sub><b> 3</b></sub>CuCl<sub><b> 3</b></sub> Observed by Specific Heat Measurements
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References
1998
Year
Magnetic PropertiesEngineeringLow-dimensional MagnetismMagnetic ResonanceSpecific Heat MeasurementsChnh 3ChemistryMagnetic MaterialsMagnetoresistanceMagnetismQuantum MaterialsThermodynamicsCucl 3PhysicsSpecific HeatQuantum ChemistrySolid-state PhysicQuantum MagnetismFerromagnetismMolecule-based MagnetNatural SciencesApplied PhysicsCondensed Matter PhysicsMagnetic Property
The compound (CH 3 ) 2 CHNH 3 CuCl 3 has recently been found to be an ideal ferromagnetic-antiferromagnetic alternating Heisenberg chain with the energy gap Δ/ k =17∼18 K [H. Manaka et al. : J. Phys. Soc. Jpn. 66 (1997) 564]. When an external field H is applied to this compound, the energy gap should vanish at the critical field H c1 = Δ/ g µ B . Just above H c1 , the three-dimensional magnetic long-range order is expected, if the interchain coupling exists. Motivated by this expectation, we performed specific heat measurements over a temperature range from 0.5 to 5 K applying H up to 12 T. As a result, we found a λ-type anomaly of specific heat over 10∼12 T, which indicates a transition to the three-dimensional long range order. The temperature at which the λ-type anomaly appears increases with increasing H . The critical field obtained by extrapolating the curve of the λ peak position versus H is 9.0 T, which is close to that obtained from a magnetization measurement.
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