Tetragonal Diiodotetrapyridinedicopper(I): Structure, Luminescence, and Computational Modeling

We report on a new crystal modification of (CuIPy 2 ) n (Py = pyridine), a compound first reported by White et al. In contrast to White’s orthorhombic structure, which is comprised of rhomboid iodide-bridged dimers, Cu 2 I 2 Py 4 , our new tetragonal crystal structure in space group P 4 1 2 1 2 is d...

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Veröffentlicht in:Journal of inorganic and organometallic polymers and materials 2017-11, Vol.27 (Suppl 1), p.90-100
Hauptverfasser: Kelly, Andrew W., Handy, Joseph V., Nicholas, Aaron D., Barnes, Francis H., Patterson, Howard H., Wojtas, Lukasz, Pike, Robert D.
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container_end_page 100
container_issue Suppl 1
container_start_page 90
container_title Journal of inorganic and organometallic polymers and materials
container_volume 27
creator Kelly, Andrew W.
Handy, Joseph V.
Nicholas, Aaron D.
Barnes, Francis H.
Patterson, Howard H.
Wojtas, Lukasz
Pike, Robert D.
description We report on a new crystal modification of (CuIPy 2 ) n (Py = pyridine), a compound first reported by White et al. In contrast to White’s orthorhombic structure, which is comprised of rhomboid iodide-bridged dimers, Cu 2 I 2 Py 4 , our new tetragonal crystal structure in space group P 4 1 2 1 2 is disordered and can be interpreted as either iodide-bridged dimers or helical chains. To determine the structure type, variable temperature X-ray diffraction and luminescence measurements were carried out. The photoluminescence spectrum shows a distinct cluster-centered transition at high excitation energies which is consistent with the dimer structure. DFT and TD-DFT calculations were performed to explain the difference between the emission spectrum at high energies compared to low energies. Furthermore, correlation of the luminescence spectrum with the X-ray results as temperature is varied demonstrates that the cluster-centered luminescence band in Cu 2 I 2 Py 4 arises from close Cu⋯Cu distances which vary with temperature. A low temperature X-ray crystallographic redetermination of the cubane tetrameric Cu 4 I 4 Py 4 is also presented. Both Cu 2 I 2 Py 4 and Cu 4 I 4 Py 4 structures show distortion of the Cu n I n core cluster at low temperature resulting in reduced Cu⋯Cu distances, but with I⋯I distances roughly unchanged.
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In contrast to White’s orthorhombic structure, which is comprised of rhomboid iodide-bridged dimers, Cu 2 I 2 Py 4 , our new tetragonal crystal structure in space group P 4 1 2 1 2 is disordered and can be interpreted as either iodide-bridged dimers or helical chains. To determine the structure type, variable temperature X-ray diffraction and luminescence measurements were carried out. The photoluminescence spectrum shows a distinct cluster-centered transition at high excitation energies which is consistent with the dimer structure. DFT and TD-DFT calculations were performed to explain the difference between the emission spectrum at high energies compared to low energies. Furthermore, correlation of the luminescence spectrum with the X-ray results as temperature is varied demonstrates that the cluster-centered luminescence band in Cu 2 I 2 Py 4 arises from close Cu⋯Cu distances which vary with temperature. A low temperature X-ray crystallographic redetermination of the cubane tetrameric Cu 4 I 4 Py 4 is also presented. 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In contrast to White’s orthorhombic structure, which is comprised of rhomboid iodide-bridged dimers, Cu 2 I 2 Py 4 , our new tetragonal crystal structure in space group P 4 1 2 1 2 is disordered and can be interpreted as either iodide-bridged dimers or helical chains. To determine the structure type, variable temperature X-ray diffraction and luminescence measurements were carried out. The photoluminescence spectrum shows a distinct cluster-centered transition at high excitation energies which is consistent with the dimer structure. DFT and TD-DFT calculations were performed to explain the difference between the emission spectrum at high energies compared to low energies. Furthermore, correlation of the luminescence spectrum with the X-ray results as temperature is varied demonstrates that the cluster-centered luminescence band in Cu 2 I 2 Py 4 arises from close Cu⋯Cu distances which vary with temperature. A low temperature X-ray crystallographic redetermination of the cubane tetrameric Cu 4 I 4 Py 4 is also presented. 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In contrast to White’s orthorhombic structure, which is comprised of rhomboid iodide-bridged dimers, Cu 2 I 2 Py 4 , our new tetragonal crystal structure in space group P 4 1 2 1 2 is disordered and can be interpreted as either iodide-bridged dimers or helical chains. To determine the structure type, variable temperature X-ray diffraction and luminescence measurements were carried out. The photoluminescence spectrum shows a distinct cluster-centered transition at high excitation energies which is consistent with the dimer structure. DFT and TD-DFT calculations were performed to explain the difference between the emission spectrum at high energies compared to low energies. Furthermore, correlation of the luminescence spectrum with the X-ray results as temperature is varied demonstrates that the cluster-centered luminescence band in Cu 2 I 2 Py 4 arises from close Cu⋯Cu distances which vary with temperature. A low temperature X-ray crystallographic redetermination of the cubane tetrameric Cu 4 I 4 Py 4 is also presented. Both Cu 2 I 2 Py 4 and Cu 4 I 4 Py 4 structures show distortion of the Cu n I n core cluster at low temperature resulting in reduced Cu⋯Cu distances, but with I⋯I distances roughly unchanged.</abstract><cop>New York</cop><pub>Springer US</pub><doi>10.1007/s10904-017-0584-y</doi><tpages>11</tpages><oa>free_for_read</oa></addata></record>
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subjects Chemistry
Chemistry and Materials Science
Clusters
Crystal structure
Crystallography
Cubane
Diffraction
Dimers
Inorganic Chemistry
Luminescence
Molecular structure
Organic Chemistry
Photoluminescence
Polymer Sciences
title Tetragonal Diiodotetrapyridinedicopper(I): Structure, Luminescence, and Computational Modeling
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