Comparison of the crystal structures and magnetic properties of the low- and high-temperature forms of AgCuPO4 : crystal structure determination, magnetic susceptibility measurements, and spin dimer analysis
hal.structure.identifier | Institut de Chimie de la Matière Condensée de Bordeaux [ICMCB] | |
dc.contributor.author | BEN YAHIA, Hamdi | |
hal.structure.identifier | Institut de Chimie de la Matière Condensée de Bordeaux [ICMCB] | |
dc.contributor.author | GAUDIN, Etienne | |
hal.structure.identifier | Institut de Chimie de la Matière Condensée de Bordeaux [ICMCB] | |
dc.contributor.author | DARRIET, Jacques | |
hal.structure.identifier | Department of Chemistry, North Carolina Raleigh | |
dc.contributor.author | DAI, Dadi | |
hal.structure.identifier | Department of Chemistry, North Carolina Raleigh | |
dc.contributor.author | WHANGBO, Myung-Hwan | |
dc.date.issued | 2006 | |
dc.identifier.issn | 0020-1669 | |
dc.description.abstractEn | The crystal structure of the low-temperature form of AgCuPO4 (i.e., -AgCuPO4) was determined by powder X-ray diffraction and was compared with that of the high-temperature form of AgCuPO4 (i.e., -AgCuPO4). The magnetic properties of the two forms were examined by measuring their magnetic susceptibilities and evaluating the relative strengths of their spin-exchange interactions on the basis of spin-dimer analysis. Both forms of AgCuPO4 have layers of Cu2P2O8 alternating with silver-atom double layers; -AgCuPO4 has two Cu2P2O8 layers per unit cell, while -AgCuPO4 has one. The coordinate environment of each Cu2+ ion is close to being a distorted square pyramid in -AgCuPO4, but it is close to being a distorted trigonal bipyramid in -AgCuPO4. The magnetic susceptibilities of - and -AgCuPO4 are well simulated by an antiferromagnetic alternating-chain model, which leads to J/kB = -146.1 K and J/kB = -75.8 K for -AgCuPO4, and J/kB = -82.6 K and J/kB = -31.7 K for -AgCuPO4 (with the convention in which the spin-exchange parameter between two adjacent spin sites is written as 2J). The spin gaps, /kB, obtained from these parameters are 93.7 K for -AgCuPO4 and 62.3 K for -AgCuPO4. The strongest spin exchange in both forms of AgCuPO4 comes from a super-superexchange path, and this interaction is stronger for -AgCuPO4 than for -AgCuPO4 by a factor of ~2, in good agreement with the experiment. Our analysis supports the use of this model for -AgCuPO4 and indicates that the spin lattice of -AgCuPO4 would be better described by a two-dimensional net made up of weakly interacting alternating chains. | |
dc.language.iso | en | |
dc.publisher | American Chemical Society | |
dc.subject.en | High temperature | |
dc.subject.en | Magnetic phenomena | |
dc.subject.en | Low temperature | |
dc.subject.en | AgCuPO4 | |
dc.subject.en | Crystal structure | |
dc.subject.en | Magnetism | |
dc.subject.en | Measurements | |
dc.subject.en | Magnetic properties | |
dc.title.en | Comparison of the crystal structures and magnetic properties of the low- and high-temperature forms of AgCuPO4 : crystal structure determination, magnetic susceptibility measurements, and spin dimer analysis | |
dc.type | Article de revue | |
dc.identifier.doi | 10.1021/ic060484l | |
dc.subject.hal | Chimie/Matériaux | |
bordeaux.journal | Inorganic Chemistry | |
bordeaux.page | p. 5501-5509 | |
bordeaux.volume | vol. 45, n° 14 | |
bordeaux.peerReviewed | oui | |
hal.identifier | hal-00084957 | |
hal.version | 1 | |
hal.popular | non | |
hal.audience | Non spécifiée | |
hal.origin.link | https://hal.archives-ouvertes.fr//hal-00084957v1 | |
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