TY - JOUR
T1 - Dynamics of Chiral Cations in Two-Dimensional CuX4and PbX4Perovskites (X = Cl and Br)
AU - Takahashi, Masaki
AU - Hoshino, Norihisa
AU - Sambe, Kohei
AU - Takeda, Takashi
AU - Akutagawa, Tomoyuki
N1 - Funding Information:
This work was supported by a Grant-in-Aid for Scientific Research on KAKENHI Kibankenkyu (A) (JP19H00886), JST CREST (Grant No. JPMJCR18I4) and "Dynamic Alliance for Open Innovation Bridging Human, Environment and Materials" from MEXT.
Funding Information:
This work was supported by a Grant-in-Aid for Scientific Research on KAKENHI Kibankenkyu (A) (JP19H00886), JST CREST (Grant No. JPMJCR18I4), and “Dynamic Alliance for Open Innovation Bridging Human, Environment and Materials” from MEXT.
Publisher Copyright:
© 2020 American Chemical Society.
PY - 2020/8/17
Y1 - 2020/8/17
N2 - Chiral organic ammonium cations ((R)-2-methylphenethylammonium (R-MPhA) and (R)-3,7-dimethyloctylammonium (R-DMOA)) cations were combined with [MX4]2- anions (M = Cu and Pb, X = Cl and Br) to form two-dimensional (2D) perovskites: (R-MPhA)2CuCl4 (1a), (R-MPhA)2CuBr4 (1b), (R-DMOA)2CuCl4 (2a), (R-DMOA)2CuBr4 (2b), (R-DMOA)2PbCl4 (2c), and (R-DMOA)2PbBr4 (2d). The point shearing of the MX4 octahedron formed 2D perovskite layers, which were sandwiched by the bilayer molecular assembly of chiral organic ammonium cations. We found that the flexible and polar organic R-MPhA and R-DMOA cations in the 2D perovskites played an important role in the phase transition behavior and dielectric responses. Salts 2a-2d showed similar solid-solid (S1-S2) phase transitions, for which the temperatures decreased in the order of CuCl4 (2a) > PbCl4 (2c) > CuBr4 (2b) > PbBr4 (2d). The occupation volume of one R-DMOA per MX4 octahedron determined the dynamic crystalline space for the motional freedom of chiral ammonium in the 2D perovskite layer. Although thermally activated dielectric fluctuations were observed in salts 2a, 2b, and 2c, only an order-disorder-type dielectric phase transition was observed in salt 2d. Interband optical transitions were observed in the CuCl4 and CuBr4 2D perovskites, whereas sharp exciton absorptions were observed in the 2D PbCl4 and PbBr4 layers in perovskite salts 2c and 2d.
AB - Chiral organic ammonium cations ((R)-2-methylphenethylammonium (R-MPhA) and (R)-3,7-dimethyloctylammonium (R-DMOA)) cations were combined with [MX4]2- anions (M = Cu and Pb, X = Cl and Br) to form two-dimensional (2D) perovskites: (R-MPhA)2CuCl4 (1a), (R-MPhA)2CuBr4 (1b), (R-DMOA)2CuCl4 (2a), (R-DMOA)2CuBr4 (2b), (R-DMOA)2PbCl4 (2c), and (R-DMOA)2PbBr4 (2d). The point shearing of the MX4 octahedron formed 2D perovskite layers, which were sandwiched by the bilayer molecular assembly of chiral organic ammonium cations. We found that the flexible and polar organic R-MPhA and R-DMOA cations in the 2D perovskites played an important role in the phase transition behavior and dielectric responses. Salts 2a-2d showed similar solid-solid (S1-S2) phase transitions, for which the temperatures decreased in the order of CuCl4 (2a) > PbCl4 (2c) > CuBr4 (2b) > PbBr4 (2d). The occupation volume of one R-DMOA per MX4 octahedron determined the dynamic crystalline space for the motional freedom of chiral ammonium in the 2D perovskite layer. Although thermally activated dielectric fluctuations were observed in salts 2a, 2b, and 2c, only an order-disorder-type dielectric phase transition was observed in salt 2d. Interband optical transitions were observed in the CuCl4 and CuBr4 2D perovskites, whereas sharp exciton absorptions were observed in the 2D PbCl4 and PbBr4 layers in perovskite salts 2c and 2d.
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U2 - 10.1021/acs.inorgchem.0c01404
DO - 10.1021/acs.inorgchem.0c01404
M3 - Article
C2 - 32594741
AN - SCOPUS:85088088018
SN - 0020-1669
VL - 59
SP - 11606
EP - 11615
JO - Inorganic Chemistry
JF - Inorganic Chemistry
IS - 16
ER -