Low-temperature specific heat of BaCuO2 and BaCuO2.14 in magnetic fields to 7 T

Citation
Ra. Fisher et al., Low-temperature specific heat of BaCuO2 and BaCuO2.14 in magnetic fields to 7 T, PHYS REV B, 61(1), 2000, pp. 538-548
Citations number
37
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science
Journal title
PHYSICAL REVIEW B
ISSN journal
10980121 → ACNP
Volume
61
Issue
1
Year of publication
2000
Pages
538 - 548
Database
ISI
SICI code
1098-0121(20000101)61:1<538:LSHOBA>2.0.ZU;2-Y
Abstract
The specific heats of samples of BaCuO2 and BaCuO2.14, on which magnetizati on and/or neutron-diffraction measurements had been made earlier, were meas ured for the temperature range 0.35 less than or equal to T less than or eq ual to 30 K in magnetic fields to 7 T. BaCuO2+x has a complex structure wit h 90 formula units in a bcc unit cell; 6 Cu are "lone spins,'' 48 are in 8 Cu6O12 "ring clusters," and 36 are in 2 Cu18O24 "sphere clusters." The ring and sphere clusters have ferromagnetically ordered ground states with spin s S=3 and 9, respectively. Antiferromagnetic ordering of the ring clusters occurs with a Neel temperature T-N(0)similar to 15 K. The specific heat of BaCuO2 shows a cooperative ordering anomaly associated with the antiferroma gnetic ordering of the ring clusters. Schottky-like anomalies, having maxim a at similar to 5 and similar to 0.7 K, are identified with the ordering of the sphere clusters and the lone spins, respectively. Only Schottky-like a nomalies are observed for the specific heat of BaCuO2.14. It is suggested t hat the increase in the Cu oxidation state, due to the addition of 0.14 mol of O, increases Cu-O covalent bonding (spin compensation) and/or produces nonmagnetic Cu3+, which in addition to the known increase in the Cu-O bond lengths, disrupts the superexchange paths that lead to the antiferromagneti c ordering of the ring clusters in BaCuO2. For BaCuO2 the magnetic entropy was 90% of that predicted for the ordering of the three Cu structures. On t he other hand, the magnetic entropy for BaCuO2.14 was only 65% of that pred icted, which suggests a relative large suppression of some magnetic entitie s due to the addition of 0.14 mol of O. Although BaCuO2+x is an insulator, the specific heat has a T-proportional component that is magnetic field dep endent and is presumably associated with the magnetic degrees of freedom.