TY - JOUR
T1 - Structural phase transition driven by spin-lattice interaction in a quasi-one-dimensional spin system of [1-(4′-iodobenzyl)pyridinium][Ni(mnt) 2]
AU - Ren, X. M.
AU - Akutagawa, T.
AU - Nishihara, S.
AU - Nakamura, T.
AU - Fujita, W.
AU - Awaga, K.
PY - 2005/9/8
Y1 - 2005/9/8
N2 - Crystal structures and magnetic properties were determined for two novel compounds, [1-(4′-iodobenzyl)-pyridinium][M(mnt)2] (mnt 2- = maleonitriledithiolate; M = Ni (1) or Cu (2)). At room temperature, single crystals of 1 and 2 were isostructural, featuring the formation of segregated columnar structures with regular stacks of cations and anions. For crystal 1, a magnetic transition was observed at ∼120 K; furthermore, its magnetic behavior was consistent with that of a regular Heisenberg antiferromagnetic (AFM) chain of S = 1/2 in the high-temperature phase (HT phase) and that of a spin-gap system in the low-temperature phase (LT phase). Such a phenomenon is similar to the spin-Peierls transition. However, the crystal structure of 1 in the LT phase at 100 K revealed that its structural transition is associated with the magnetic transition. Because crystal 2 (S = 0) did not exhibit a structural transition, the structural transition of 1 is driven by spin-lattice interaction.
AB - Crystal structures and magnetic properties were determined for two novel compounds, [1-(4′-iodobenzyl)-pyridinium][M(mnt)2] (mnt 2- = maleonitriledithiolate; M = Ni (1) or Cu (2)). At room temperature, single crystals of 1 and 2 were isostructural, featuring the formation of segregated columnar structures with regular stacks of cations and anions. For crystal 1, a magnetic transition was observed at ∼120 K; furthermore, its magnetic behavior was consistent with that of a regular Heisenberg antiferromagnetic (AFM) chain of S = 1/2 in the high-temperature phase (HT phase) and that of a spin-gap system in the low-temperature phase (LT phase). Such a phenomenon is similar to the spin-Peierls transition. However, the crystal structure of 1 in the LT phase at 100 K revealed that its structural transition is associated with the magnetic transition. Because crystal 2 (S = 0) did not exhibit a structural transition, the structural transition of 1 is driven by spin-lattice interaction.
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U2 - 10.1021/jp051995g
DO - 10.1021/jp051995g
M3 - Article
AN - SCOPUS:25444503757
SN - 1520-6106
VL - 109
SP - 16610
EP - 16615
JO - Journal of Physical Chemistry B
JF - Journal of Physical Chemistry B
IS - 35
ER -