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2391
both free ligands and it was found that the strongest
emission peak for H2PYDC is located at ca. 370 nm
(lex ¼ 276 nm), whereas for H2HPHT it is at ca. 455 nm
(lex ¼ 370 nm) [19]. The strongest emission peak of
compound 1 (415 nm) is very close to the free ligand
(370 nm). In addition, a series of lead(II) b-diketonates
compounds showing typical intraligand (IL) phosphores-
cence has been reported [20a]. Therefore, this emission
band might be attributed to the intraligand (IL) emission
from the PYDC ligand [20]. The bathochromic shift and
enhancement of PYDC ligand in compound 1 compared to
free ligand may be attributed to the coordination bond
between the ligand and Pb(II), which increases the rigidity
of the ligand and reduces the loss of energy by radiationless
decay of the intraligand emission excited state [21]. The
emission wavelength of compound 2 occurs at a much
lower energy of 602 nm, which is much longer than that of
the free ligand (455 nm). The low-energy emissions
associated with large Stokes shifts have been commonly
observed for other s2–metal complexes, which can be
assigned to a metal-centered transition involving the s and
p metal orbital as proposed by Vogler [18b,c]. Thus the
emission band of 2 can be assigned to a metal-centered s-
p transition. In addition, the dinuclear Pb2O2 cluster in the
[Pb(HPHT)]n. These data can be obtained free of charge
Cambridge Crystallographic Data Center, 12 Union Road,
Cambridge CB2 1EZ, UK; fax: (+44) 1223-336-033; or
e-mail: deposit@ccdc.cam.ac.uk.
Acknowledgments
This work was financially supported by NSFC
(90206040, 20325106, 20521101 and 20333070), NSF of
Fujian Province (2005HZ01-1, E0520003), The Distin-
guished Oversea Scholar Project and One Hundred Talent
Project from CAS.
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