Table 1 Photophysical parameters of copper complexes at room
temperature in MeCy
tunability, and ease of synthesis. The ease of synthetic modifi-
cation afforded by these complexes provides an opportunity to
expand the available emission colors and to facilitate a more
detailed study of the photophysical states contributing to their
luminescence properties.
a,b
Complex
lem/nm
FPL
t/msc
1
2
3
521
546
525
509
535
563
461
0.23
0.22
0.13
0.13
0.11
0.18
0.24
3.17(5)
3.1(2)
2.5(1)
This work was supported by an NSF Center for Chemical
Innovation (CHE-0802907). Luminescence measurements
were carried out in the laboratory of T. M. Swager with
assistance from T. L. Andrews. K. J. L. gratefully acknowledges
a fellowship from the MIT Energy Initiative.
4
2.5(1)
5d
6
2.71(2)
1.70(1)
11.7(6)
7
a
Uncertainty in quantum yield measurements is estimated to be ꢂ0.05.
b l = 390 nm. c
ex
d
lex = 337 nm. In C5H10
.
Notes and references
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Fig.
5 (A) HOMO of 2 as calculated by DFT. Energy =
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most extensively studied monomeric copper emitters.7
The electronic structure of 2 was explored using Density
Functional Theory (DFT) calculations at the B3LYP/
6-31+G* level of theory. The computed highest occupied
molecular orbital (HOMO) is localized primarily on the
diphenylamide ligand with substantial nitrogen pp and C–C
p character (Fig. 5). There is a small contribution from a Cu
d-orbital that is p-antibonding with respect to the amide
p-orbital. The HOMO is nearly identical to those calculated
for a related class of complexes9 and indicates that tuning of
the ground state energy is possible through ortho- or para-
substitution of the amide phenyl rings. The calculated lowest
unoccupied molecular orbital (LUMO) is localized on the
triphenylphosphine ligands and has C–C p* character. While
these computational results imply a ligand-to-ligand-charge-
transfer (LLCT) excitation, computational and experimental
studies on related systems suggest that amide ligand-centered
(LC) excited states may also play an important role.10,12
Further studies aimed at understanding the photophysics
and electronic structure of these luminescent copper(I) amido-
phosphines are underway for comparison to a recent detailed
photophysical study on the dicopperphosphinoamide complex
[Cu(PNP-tBu)]2 (PNP-tBu = bis[(2-diisopropylphosphino-4-
tert-butyl)phenyl]amide).13
8 S. B. Harkins and J. C. Peters, J. Am. Chem. Soc., 2005, 127,
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11 Yamamoto and co-workers had previously formulated a series of
Cu(I) bisphosphinoamidates as three-coordinate. No structural
data were presented. One of these complexes was observed to be
luminescent: T. Yamamoto, Y. Ehara, M. Kubota and
A. Yamamoto, Bull. Chem. Soc. Jpn., 1980, 53, 1299–1302.
12 S. B. Harkins, N. P. Mankad, A. J. Miller, R. K. Szilagyi and
J. C. Peters, J. Am. Chem. Soc., 2008, 130, 3478–3485.
13 J. C. Deaton, S. C. Switalski, D. Y. Kondakov, R. H. Young,
T. D. Pawlik, D. J. Giesen, S. B. Harkins, A. J. M. Miller,
S. F. Mickenberg and J. C. Peters, 2010, manuscript submitted
for publication.
In conclusion, we have described a series of three-coordinate
copper(I) diarylamidophosphine complexes that combine efficient
luminescence in solution at room temperature, spectroscopic
ꢁc
This journal is The Royal Society of Chemistry 2010
3692 | Chem. Commun., 2010, 46, 3690–3692