Abstract

The spin-crossover (SCO) phenomenon between a high-spin and a low-spin state has attracted much attention in the field of materials science. Among the various kinds of SCO complexes, the triazole-bridged iron(II) polymeric chain system, [Fe(II)(R-trz)3]X2·xH2O (where trz is triazole and X is the anion), exhibiting the SCO phenomenon with thermal hysteresis around room temperature, has been extensively studied from the viewpoint of molecular memory and molecular devices. In connection with this system, we have controlled the SCO phenomenon according to the characteristic properties of counter ions. In the case of X being CnH2n+1SO3−, the spin transition temperature (T1/2) increases with increasing the length (n) of the alkyl chain of the counter ion and saturates above n = 5, which is attributed to the increase in the intermolecular interaction of the alkyl chains of CnH2n+1SO3−, called the fastener effect. The hysteresis width of T1/2 decreases with increasing n, showing the even-odd, also known as parity, effect. In the cases where X is toluenesulfonate (tos: CH3C6H4SO3−) and aminobenzenesulfonate (abs: NH2C6H4SO3−), T1/2 and its hysteresis width vary drastically with the structural isomerism (ortho-, metha-, and para-substitution) of counter ions, which implies the possibility of photoinduced spin transition by means of the photoisomerization of counter ions. From this strategy, we have synthesized [Fe(II)(NH2-trz)3](SP150)2·2H2O (SP150 = N-alkylsulfonated spiropyran) and investigated the SCO phenomenon. Moreover, we have developed [Fe(II)(R-trz)3]@Nafion films exhibiting spin transition around room temperature, where the Nafion membrane behaves as a counter anion as well as a transparent substrate, and investigated the photogenerated high-spin state below 35 K. The lifetime of the photogenerated high-spin state strongly depends on the intensity of irradiated light.

Highlights

  • An octahedrally coordinated transition metal ion, having an electron configuration of 3dn (n = 4–7), exhibits the possibility to change the ground spin state between the low-spin (LS) and high-spin (HS)states

  • In the case when X is toluenesulfonate and aminobenzenesulfonate, T1/2 and its hysteresis width vary drastically with the structural isomerism [24,25], which implies the possibility of photoinduced spin transition by means of the photoisomerization of counter ions

  • We review the effect of the characteristic properties of counter anions on the SCO behavior and the photoinduced SCO phenomenon for [Fe(II)(R-trz)3 ]X2 ·xH2 O (R = H, NH2, etc.; X = anion), which has been mainly contributed by our group

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Summary

Introduction

With increasing the amount of crystal water, the transition temperature lowers and the thermal hysteresis width becomes narrow This can be explained by the water molecules in [Fe(II)(NH2 -trz)3 ](p-tos)2 ·xH2 O having two opposite functions in the SCO phenomenon. The triazole-bridged iron(II) chain system accepts various kinds of counter anions and exhibits a wide variety of spin transitions From this viewpoint, we have developed [Fe(II)(R-trz)3 ] films exhibiting the SCO phenomenon around room temperature and observed the LIESST effect below 30 K, in which Nafion behaves as a counter anion as well as a transparent substrate [21,29]. This condensed phase is stabilized by the attractive interaction between the HS sites and not by the transformation into a metastable structure

Syntheses
Fe K-Edge EXAFS Spectroscopy
Magnetic Susceptibility Measurements
Optical Spectroscopy
Conclusions
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