Spin-State Patterns in Surface-Grafted Beads of Iron(II) Complexes
Spin-State Patterns in Surface-Grafted Beads of Iron(II) Complexes
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DOI:
10.1002/anie.200905062
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发表时间:
2010-01-01
影响因子:
16.6
通讯作者:
Grohmann, Andreas
中科院分区:
文献类型:
--
作者:
Alam, Mohammad S.;Stocker, Michael;Grohmann, Andreas
Novel strategies for the design of functional materials are in increasing demand, as the down-scaling of lithographic processes (the top-down approach) will soon encounter the fundamental physical limits of miniaturization.[1] One of the fascinating perspectives of molecular electronics [2, 3] is information storage at the single-molecule level, on the basis of arrays of molecular switches.[4] Spin-crossover (SCO) compounds hold considerable potential in this context.[5, 6] SCO can occur in octahedral transition-metal complexes in which the metal ion has ad 4 to d7 electron configuration.[7, 8] The transition may be stimulated externally, by a change in temperature or pressure, or by irradiation.[7, 8] SCO is entropydriven and, in the solid state, is influenced strongly by intermolecular interactions, such as hydrogen bonding or π–π stacking. Such interactions give rise to cooperativity between SCO complexes within the ensemble. High cooperativity can cause the change in spin state to be accompanied by hysteresis, which confers bistability on the system and thus a memory effect.[5, 7] A viable reading/writing procedure, that is, a means of reproducible actuation on the single-molecule level, is a formidable challenge that has yet to be met, but in this way SCO compounds could serve in devices of unsurpassable storage density. In principle, reliable information storage could be achieved even in the absence of hysteresis, provided the energy difference between low-spin state and high-spin state of the complexes within the SCO ensemble is sufficiently large (on the order of several kT). A large number of spin-crossover systems are known,[7] with complexes of iron (II) the most numerous, both in solution and in the solid state. Usually, ferrous iron is in a quasi-octahedral N6 coordination environment, and switching occurs between a low-spin (LS, 1A1g/t2g 6, S= 0) and a high-spin state (HS, 5T2g/t2g 4eg 2, S= 2).