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Partial in Situ Reduction of Copper(II) Resulting in One-Pot Formation of 2D Neutral and 3D Cationic Copper(I) Iodide–Pyrazine Coordination Polymers: Structure and Emissive Properties
Author(s) -
Iurie L. Malaestean,
Victor Kravtsov,
Janusz Lipkowski,
Elena Cariati,
Stefania Righetto,
Daniele Marinotto,
Alessandra Forni,
Marina S. Fonarı
Publication year - 2017
Publication title -
inorganic chemistry
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.348
H-Index - 233
eISSN - 1520-510X
pISSN - 0020-1669
DOI - 10.1021/acs.inorgchem.7b00290
Subject(s) - chemistry , pyrazine , copper , denticity , phosphorescence , iodide , singlet state , crystallography , ligand (biochemistry) , cationic polymerization , photochemistry , inorganic chemistry , fluorescence , stereochemistry , polymer chemistry , crystal structure , organic chemistry , biochemistry , physics , receptor , quantum mechanics , nuclear physics , excited state
On the way to copper(I) iodide coordination polymers with specific luminescent properties, the in situ reduction of Cu(II) in the presence of KI and bidentate N-heteroatomic ligand, either pyrazine (pyz) or 4,4'-bipyridine (bpy), resulted in one two-dimensional and two three-dimensional new coordination networks. Starting from Cu(NO 3 ) 2 ·3H 2 O in the presence of pyz, successive precipitation of known yellow [(Cu I I) 2 (pyz)] n , new orange [Cu I I(pyz)] n , and new dark blue {[Cu I (pyz) 2 ]·I 5 } n polymeric solids was observed. Starting from the same salt in the presence of bpy resulted in the successive precipitation of known yellow [(Cu I I) 2 (bpy)] n and new brown {[Cu II (NO 3 )(bpy) 2 ]·I 3 ·(dmf·H 2 O)} n coordination polymers. By using either Cu(CH 3 COO) 2 ·H 2 O or Cu(BF 4 ) 2 as starting materials, both known forms, yellow [(Cu I I) 2 (bpy)] n and orange [Cu I I(bpy)] n , precipitated successively. The new solids were characterized by IR spectroscopy and X-ray analysis. [Cu I I(pyz)] n represents the missing member in the row of two-dimensional coordination networks with general formula [Cu I X(pyz)] n (X = Cl, Br, I). Its steady state and time-resolved characterization together with DFT and TDDFT calculations revealed that the emission at room temperature is mainly delayed fluorescence originating from mixed singlet metal-to-ligand charge transfer and halide-to-ligand charge transfer states, while that at 77 K is phosphorescence, associated with the small singlet-triplet energy differences (ΔE = 70 meV).

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