Magnetic Dimensional Crossover from Two- to Three-Dimensional Heisenberg Magnetism in a Cu–W Cyano-Bridged Bimetal Assembly

Abstract

In this work, we synthesized a cyano-bridged Cu–W bimetal assembly, [Cu<sup>II</sup>(pyrimidine)<sub>2</sub>]<sub>4</sub>­[Cu<sup>II</sup>(H<sub>2</sub>O)<sub>2</sub>]<sub>2</sub>[W<sup>V</sup>(CN)<sub>8</sub>]<sub>4</sub>·4H<sub>2</sub>O (<b>1</b>), which has a monoclinic crystal structure (<i>P</i>2<sub>1</sub>/<i>n</i> space group, <i>a</i> = 15.7365(3) Å, <i>b</i> = 21.1555(4) Å, <i>c</i> = 27.1871(5) Å, β = 91.8630(7)°, and <i>Z</i> = 4). In this compound, Cu and W sites form two-dimensional (2-D) layers along the <i>ab</i> plane, while the other Cu sites are bridged between the 2-D layers, constructing a three-dimensional (3-D) structure. The magnetic susceptibility measurement showed that ferromagnetic interaction operates in the magnetic spins of the present compound. The field-cooled-magnetization (FCM) curve indicates that the magnetization gradually increases in the temperature range of ca. 40–8 K, and the spontaneous magnetization appears at a Curie temperature of 8 K. To understand the anomalous magnetization increase in the temperature range of ca. 40–8 K, we measured the magnetic heat capacity (<i>C</i><sub>mag</sub>). The <i>C</i><sub>mag</sub> vs <i>T</i> plots have a broad peak around 18 K and a sharp peak at 8 K. Such a type of <i>C</i><sub>mag</sub> vs <i>T</i> plots indicates a dimensional crossover from a 2-D to a 3-D Heisenberg magnetic model. This is because <b>1</b> has a pseudo 2-D network structure; that is, the magnitude of the intralayer superexchange interaction is much larger than that of the interlayer superexchange interaction. Such a magnetic dimensional crossover is a rare and intriguing issue in the field of magnetic substances

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