献明 张;明良 童;Meng Lian Gong;Hung Kay Lee;Li Luo;King Fai Li;叶翔 童;小明 陈
China Association for Science and Technology;Sun Yat-Sen University;Chinese University of Hong Kong;Guangdong University of Technology;Hong Kong Baptist University
发表时间:2002-7-15
期 刊:Chemistry - A European Journal
语 言:English
U R L: http://www.scopus.com/inward/record.url?scp=0037101663&partnerID=8YFLogxK
Four copper complexes with hydroxylated bipyridyl-like ligands, namely [Cu2(ophen)2] (1), [Cu4(ophen)4(tp)] (2), [Cu4(obpy)4(tp)] (3), and [Cu4(obpy)4(dpdc)] · 2H2O (4), (Hophen = 2-hydroxy-1,10-phenanthroline, Hobpy = 6-hydroxy-2,2′-bipyridine, tp = terephthalate, dpdc = diphenyl-4,4′-dicarboxylate) have been synthesized hydrothermally. X-ray single-crystal structural analyses of these complexes reveal that 1,10-phenanthroline (phen) or 2,2′-bipyridine (bpy) ligands are hydroxylated into ophen or obpy during the reaction, which provides structural evidence for the long-time argued Gillard mechanism. The dinuclear copper(I) complex 1 has three supramolecular isomers in the solid state, in which short copper - copper distances (2.66 - 2.68 Å) indicate weak metal-metal bonding interactions. Each of the mixed-valence copper(I,II) complexes 2-4 consists of a pair of [Cu2(ophen)2]+ or [Cu2(obpy)2]+ fragments bridged by a dicarboxylate ligand into a neutral tetranuclear dumbbell structure. Dinuclear 1 is an intermediate in the formation of 2 and can be converted into 2 in the presence of additional copper(II) salt and tp ligands under hydrothermal conditions. In addition to the ophen-centered π→π* excited-state emission, 1 shows strong emissions at ambient temperature, which may be tentatively assigned as an admixture of copper-centered d →s,p and MLCT excited states.
化合物
工程与材料科学
Scopus度量
年份 | CiteScore | SJR | SNIP |
---|---|---|---|
1996 | |||
1997 | |||
1998 | |||
1999 | 2.904 | 1.602 | |
2000 | 2.985 | 1.525 | |
2001 | 2.872 | 1.514 | |
2002 | 2.58 | 1.426 | |
2003 | 2.365 | 1.437 | |
2004 | 2.442 | 1.471 | |
2005 | 2.78 | 1.474 | |
2006 | 3.108 | 1.552 | |
2007 | 3.449 | 1.591 | |
2008 | 3.135 | 1.497 | |
2009 | 2.753 | 1.504 | |
2010 | 2.791 | 1.344 | |
2011 | 8.8 | 2.902 | 1.358 |
2012 | 9.3 | 2.935 | 1.295 |
2013 | 9.6 | 2.643 | 1.244 |
2014 | 9.8 | 2.526 | 1.219 |
2015 | 9.5 | 2.461 | 1.205 |
2016 | 9.3 | 2.352 | 1.085 |
2017 | 9.1 | 2.265 | 1.035 |
2018 | 8.7 | 1.842 | 0.98 |
2019 | 9 | 1.681 | 1.01 |
2020 | 8.3 |
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