A supramolecular ferroelectric realized by collective proton transfer
A supramolecular ferroelectric realized by collective proton transfer
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DOI:
10.1002/anie.200700407
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发表时间:
2007-01-01
影响因子:
16.6
通讯作者:
Tokura, Yoshinori
中科院分区:
文献类型:
--
作者:
Horiuchi, Sachio;Kumai, Reiji;Tokura, Yoshinori
Hydrogen bonds, which bind two or more electronegative atoms as XÀH··· Y, have been utilized to construct molecular assemblies in crystal engineering, supramolecular chemistry, and molecular recognition.[1] The dynamics of proton transfer through hydrogen bonds has attracted extensive interest, because of the crucial role played by proton transfer in many chemical reactions and biological functions, and also because of its potentially diverse applications in electronic and optical devices.[2] In organic molecular solids, proton transfer is often accompanied by a tautomerism of the π-electron configuration, which can be associated with novel functionalities; transformations between the keto and enol forms of molecules have been reported to produce a reversible color change [3] or a dipole inversion.[4] Importantly, such a motion of protons can be correlated even through intermolecular space, if each molecule is restricted in its total number of protons, as is typically found in the case of ice. Squaric acid (H2C4O4)[5] provides a good example of this constraint called the “ice rule”: cooperative proton transfer over the short O··· O bonds (2.55) can reverse the polarity of the hydrogen-bonded molecular sheets. As a consequence, a high dielectric permittivity emerges near the order–disorder phase transition. As in this example, the three-dimensional arrangement of polar molecules is usually antiparallel (antiferroelectric), canceling out the net electric polarization. If the mobile protons were ordered into a polar lattice, they would generate a spontaneous polarization, and their motion could be controlled with an external electric field, as a ferroelectric. Herein, we report the first organic system that exhibits ferroelectricity induced by a cooperative intermolecular proton transfer. KH2PO4 (KDP) is a representative inorganic ferroelectric, in which the electric polarization is reversed by an electric field through a site-to-site proton transfer over very short O··· O bonds (2.50) between the PO4 2À ions.[6] Molecular analogues of KDP are still undeveloped, except for an organic–inorganic hybrid, the salt [dabcoH]+[ReO4] À (dabco= diazabicyclo [2.2. 2] octane).[7] To design genuinely organic ferroelectrics, we have exploited a strongly hydrogen-bonded acid–base system, because some such compounds are known to exhibit novel thermally induced proton migration.[8] The combination of acids and bases with similar proton affinities guarantees that the protons of the hydrogen bonds can easily attach to both molecules.[9] Cocrystals of 2, 5-dihydroxy-p-benzoquinones as the acid and pyridine derivatives as the base (Scheme 1) have recently been tested to fulfill this requirement. For example, it was demonstrated that chloranilic acid (H2ca; Scheme 1, X= Cl) and bromanilic acid (X= Br) produce ferroelectric adducts with phenazine (Phz).[10] In these adducts, however, there is no apparent site-to-site proton transfer and the ferroelectricity is, rather, classified as displacive, as is found for the BaTiO3 or PbTiO3 family. On the other hand, an antiferroelectric phase transition with proton ordering was realized in a proton-transferred monovalent salt of H2ca with a stronger base, 5, 5’-dimethyl-2, 2’-bipyridine (55DMBP; Scheme 1).[11] The new ferroelectric presented herein is derived from the iodine analogue of H2ca, iodanilic acid (H2ia; Scheme 1, X= I), and 55DMBP. This compound is also a proton-transferred 1: 1 salt, as formulated by [H-