C O M M U N I C A T I O N S
Table 1. Luminescence Lifetimes for the Complexes Studied
ytterbium and the steric demands of the amide substituentssthe
residual hydration probably results from outer sphere effects. We
then studied the interaction between the terbium and ytterbium ions
for a solution of 1 in D2O. Direct excitation of the terbium
absorption band at 488 nm resulted in the observation of ytterbium-
centered emission at 980 nm. Stray light was rejected using a cutoff
filter in front of the monochromator to remove signals below 850
nm and obviate the possibility of 2λ artifacts appearing close to
980 nm. The decay of the emission band at 980 nm fitted to a
lifetime identical to that measured for the ytterbium complex in
D2O when excited at 337 nm. The fitted time-resolved decay is
shown as an inset to Figure 1. It is reasonable to infer energy
transfer from the terbium center, since neither ytterbium nor the
ligand-centered chromophore have any absorption bands at 488 nm.
To our knowledge this represents the first report of lanthanide-
centered near-IR emission sensitized by a lanthanide ion. We are
currently investigating the use of different pairs of lanthanide ions
and more complex arrays with a view to performing a thorough
study of the energy transfer processes involved.
compd
Lna
λex/nm
λem/nm
τH
O/µ
s
τD
O/µs
q
2
2
6
7
1
1
Tb
Tb
Yb
Yb
266
266
337
488
545
545
980
980
860
1140
1.83
1180
1840
4.22
4.22
1.3
1.4
0.2
a Lanthanide ion under examination.
Acknowledgment. The authors wish to acknowledge support
from the University of Manchester and EPSRC (GR/M82608).
Figure 1. Fitted luminescence decays for ligand-sensitized (main graph)
and terbium-sensitized emission (inset) from ytterbium in compound 1
dissolved in D2O. Both fit to a lifetime of 4.2 µs. The observed decay (blue)
and fitted curve (red), superimpose almost exactly, as can be seen from the
residual (dark green). The detector response (black) is also shown.
Supporting Information Available: Synthetic routes to 1 and its
precursors; experimental procedures for luminescence spectroscopy and
deconvolution; energy level diagram showing excited states for terbium
and ytterbium. This material is available free of charge via the Internet
intensities of the emission maxima, with the strongest transition at
545 nm, when probed directly (λex ) 366 nm) or through the aryl
chromophore of the aminobenzyl group (λex ) 266 nm). This
suggests that the binding site is the same in both cases. Furthermore,
the luminescence lifetimes obtained for 6 and 7 (Table 1) give
similar hydration numbers, showing that the metal environment is
almost certainly the same in both cases. Having thus ascertained
that the terbium remains in a DO3A-like binding site through the
course of the synthesis of 7, it is reasonable to assume that the
complex is kinetically robust. Reaction of 7 with ytterbium
trifluoromethanesulfonate yielded the trinuclear complex 1. Ytter-
bium has been shown to reduce the luminescence intensity of
terbium in kinetically unstable systems.13 In our system the metals
are held in close proximity with one another throughout the
experiment, and the luminescence from the ytterbium center can
be studied without difficulty. Excitation at 337 nm using a nitrogen
laser gave rise to emission from both metal centers. The emission
from the terbium center was reduced in intensity relative to the
terbium-centered luminescence in 7, and a new emission at 980
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