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Conducting Layered Organic-inorganic Halides Containing 〈110〉-Oriented Perovskite Sheets

David B. MitziIBM T. J. Watson Research Center, Post Office Box 218, Yorktown Heights, NY 10598, USAS. WangDepartment of Chemistry and Texas Center for Superconductivity, University of Houston, Houston, TX 77204-5641, USAC. FeildIBM T. J. Watson Research Center, Post Office Box 218, Yorktown Heights, NY 10598, USACatherine A. ChessIBM T. J. Watson Research Center, Post Office Box 218, Yorktown Heights, NY 10598, USAArnold M. GuloyDepartment of Chemistry and Texas Center for Superconductivity, University of Houston, Houston, TX 77204-5641, USA
1995en
ABI

Annotatsiya

Single crystals of the layered organic-inorganic perovskites, [NH(2)C(I=NH(2)](2)(CH(3)NH(3))m SnmI3m+2, were prepared by an aqueous solution growth technique. In contrast to the recently discovered family, (C(4)H(9)NH(3))(2)(CH(3)NH(3))n-1SnnI3n+1, which consists of (100)-terminated perovskite layers, structure determination reveals an unusual structural class with sets of m <110>-oriented CH(3)NH(3)SnI(3) perovskite sheets separated by iodoformamidinium cations. Whereas the m = 2 compound is semiconducting with a band gap of 0.33 +/- 0.05 electron volt, increasing m leads to more metallic character. The ability to control perovskite sheet orientation through the choice of organic cation demonstrates the flexibility provided by organic-inorganic perovskites and adds an important handle for tailoring and understanding lower dimensional transport in layered perovskites.

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