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Two magnetic phase transitions, driven by symmetry breaking and isostructural phase transitions, in a nickel-bis-dithiotene spin system

机译:镍-双-二硫代噻吩自旋体系中由对称断裂和同构相变驱动的两个磁性相变

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A one-dimensional (1-D) magnetic chain compound, [(CD3)2C=N-Py][Ni(mnt)2l, where (CD3)2C=N-Py~+ = l-(propan-d6-2-ylideneamino)pyridinium and mnt~2= maleonitriledithiolate, was synthesized and characterized. This compound undergoes two structural phase transitions, at around 267 K and 325 K. The three phases are sequentially labeled as α (below 267 K), β (between 267 and 325 K) and γ (above 325 K). The [Ni(mnt)2]~-anions form irregular stacks, with two values of neighboring Ni Ni distances. The cations align in a straight and regular arrangement along the crystallographic a-axis direction in the β phase. The asymmetric unit switches from one anion-cation pair to two anion-cation pairs in the transition from the β to the a phase. This leads to a doubling of the crystallographic axis length, parallel to the anion stack. It also results in the irregular anion stack showing three non-equivalent neighboring Ni Ni distances, as well as making the straight cation arrangement irregular. The β and γ phases are isostructural and exhibit quite similar packing structures. The anion stack shrinks a little with increasing temperature, with all crystallographic axes showing small reduction from the β to γ phase. The two observed magnetic phase transitions are driven by these various structural phase transitions. A thermal hysteresis loop, with a separation of ~8 K, appears in the transition between the β and α phases. However, this is absent in the transition between the β and γ phases. A dielectric anomaly appears across the phase transition between the β and γ phases but not between the β and a phases.
机译:一维(1-D)磁链化合物,[(CD3)2C = N-Py] [Ni(mnt)2l,其中(CD3)2C = N-Py〜+ = 1-(丙烷-d6-2合成并表征了亚苯基亚氨基)吡啶鎓和mnt〜2 =顺丁烯二腈。该化合物在大约267 K和325 K处经历了两个结构相变。这三个相依次标记为α(267 K以下),β(267和325 K之间)和γ(325 K以上)。 [Ni(mnt)2]〜-阴离子形成不规则堆叠,相邻Ni Ni距离为两个值。阳离子在β相中沿结晶a轴方向排列成直线且规则。在从β到a相的跃迁中,不对称单元从一个阴离子阳离子对转换为两个阴离子阳离子对。这导致平行于阴离子堆的结晶轴长度加倍。这也导致不规则阴离子堆显示出三个不等价的相邻Ni Ni距离,并使直阳离子排列不规则。 β和γ相是同构的,表现出非常相似的堆积结构。阴离子堆随着温度的升高而略有收缩,所有的晶体学轴显示从β相到γ相的少量还原。观察到的两个磁性相变是由这些各种结构相变驱动的。 β相和α相之间的跃迁中出现一个〜8 K的热滞回线。但是,这在β相和γ相之间的过渡中是不存在的。在β相和γ相之间的相变上出现电介质异常,但在β相和α相之间没有出现。

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