TY - JOUR
T1 - Structural and magnetic investigations for the doping effect of nonmagnetic impurity on the spin-Peierls-like transition in a quasi-one-dimensional magnet
T2 - 1-(4′-nitrobenzyl)pyridinium bis(maleonitriledithiolato)nickelate
AU - Ren, X. M.
AU - Akutagawa, T.
AU - Noro, S.
AU - Nishihara, S.
AU - Nakamura, T.
AU - Yoshida, Y.
AU - Inoue, K.
PY - 2006/4/20
Y1 - 2006/4/20
N2 - A nonmagnetic compound, [NO2BzPy][Au(mnt)2] (NO 2BzPy+ = 1-(4′-nitrobenzyl)pyridinium; mnt 2 = maleonitriledithiolate), was synthesized and characterized structurally, which is isostructural with [NO2BzPy][Ni(mnt) 2] that is a quasi-one-dimensional magnet and possesses a spin-Peierls-like transition with J = 192 K in the gapless state and spin energy gap = 738 K in the dimerization state, respectively. Further, ten nonmagnetic impurity doped compounds with a formula [NO2BzPy][Au xNi1-x(mnth)2 (x = 0.01-0.73) were prepared and investigated by crystal structural determinations and magnetic susceptibility measurements. The nonmagnetic doping causes the suppression of the spin transition with an average rate of 221(12) K/percentage of dopant concentration. From the plots of χm-T, the transition collapse (the characteristic of the transition is the sudden drop of χm upon cooling, and the disappearance of this characteristic is considered as the criterion for the transition collapse) is estimated at around x> 0.27. In heavier doped system x = 0.49, the spin gap vanishes and a gapless phase is achieved again.
AB - A nonmagnetic compound, [NO2BzPy][Au(mnt)2] (NO 2BzPy+ = 1-(4′-nitrobenzyl)pyridinium; mnt 2 = maleonitriledithiolate), was synthesized and characterized structurally, which is isostructural with [NO2BzPy][Ni(mnt) 2] that is a quasi-one-dimensional magnet and possesses a spin-Peierls-like transition with J = 192 K in the gapless state and spin energy gap = 738 K in the dimerization state, respectively. Further, ten nonmagnetic impurity doped compounds with a formula [NO2BzPy][Au xNi1-x(mnth)2 (x = 0.01-0.73) were prepared and investigated by crystal structural determinations and magnetic susceptibility measurements. The nonmagnetic doping causes the suppression of the spin transition with an average rate of 221(12) K/percentage of dopant concentration. From the plots of χm-T, the transition collapse (the characteristic of the transition is the sudden drop of χm upon cooling, and the disappearance of this characteristic is considered as the criterion for the transition collapse) is estimated at around x> 0.27. In heavier doped system x = 0.49, the spin gap vanishes and a gapless phase is achieved again.
UR - http://www.scopus.com/inward/record.url?scp=33646457202&partnerID=8YFLogxK
U2 - 10.1021/jp0556106
DO - 10.1021/jp0556106
M3 - 文章
AN - SCOPUS:33646457202
SN - 1520-6106
VL - 110
SP - 7671
EP - 7677
JO - Journal of Physical Chemistry B
JF - Journal of Physical Chemistry B
IS - 15
ER -