Angewandte
Communications
Chemie
[
8]
urea as a surface-passivation agent. The chemical structure
of the CDs was characterized by transmission electron
microscopy (TEM), X-ray photoelectron spectroscopy
the characteristic absorption bands of CDs and the Eu-HL
complexes in the UV/Vis absorption spectra (Figure S12).
Furthermore, a full-scan XPS plot (Figure S13) confirmed
that the CDs-Eu-HL composite was mainly composed of C, N,
and O. The corresponding high-resolution C 1s, N 1s, and O 1s
XPS spectra revealed the presence of carbonyl, carboxyl, and
amine groups, which was also confirmed by FTIR spectros-
copy. Furthermore, we also observed a weak peak corre-
sponding to Eu 3d (Figure S13a). The high-resolution Eu 3d
XPS spectrum (Figure S14) shows two peaks, corresponding
(
XPS), and Fourier transform infrared spectroscopy (FTIR;
see the Supporting Information, Figures S1–S3). We thus
confirmed the presence of abundant carboxyl and amide
groups on the surface of the as-obtained CDs. These func-
tional groups provide plenty of coordination sites that can
directly chelate Eu ions. The fluorescence spectra of the
CDs reveal optimal excitation and emission wavelengths of
3
+
3
+ [12]
3
49 nm and 448 nm, respectively (Figure S1d). Additionally,
to the 3d5/2 (1134.7 eV) and 3d3/2 (1164.8 eV) states of Eu ,
which further indicated that the surface of the CDs has been
the CDs show excellent fluorescence stability over a broad
pH range (3–11) and under continuous excitation for one
hour (Figure S4).
Interestingly, the fluorescence of the CDs undergoes
a significant red shift from 449 to 491 nm upon an increase in
the solute concentration from 10 to 300 mgmL (Figure S5).
The fluorescence color changes from blue to green, which is
consistent with the corresponding chromaticity coordinates
3
+
successfully functionalized with Eu-HL. The Eu content of
the CDs-Eu-HL composites was determined to be 22.51 wt%
by thermogravimetric analysis (TGA). Similarly, the as-
obtained CDs-Eu-HL composites also display typical excita-
tion-wavelength-dependent fluorescence owing to the pres-
ence of the CDs. As shown in Figure S15, the emission peak is
gradually red-shifted from 443 to 552 nm when the excitation
wavelength is increased from 340 to 500 nm.
ꢀ
1
(
Figure S6). This red shift is best attributed to re-absorption in
view of the spectral overlap between absorption and emission
To study the stimulus response of the nanodevice, we
investigated the energy levels of the ligand HL and depro-
[9]
(
Figure S7), which can occur at small interparticle distances.
ꢀ
3+
This was further confirmed by the fact that the average
lifetime of the fluorescence of the CDs changed from 9.42 to
tonated ligand L in the Gd complexes on the CD platform.
The corresponding energy levels of the triplet excited states
3
7
.72 ns as the concentration was increased (Figure S8 and
( pp*) of the ligand were calculated from the low-temper-
Table S1) because re-absorption processes compete with
ature (77 K) phosphorescence spectra of the corresponding
Gd complexes in a 1:1 methanol/ethanol mixture. Accord-
[10]
3+
radiative transitions and then shorten the lifetime.
Fur-
thermore, the significant shift in wavelength that is described
above is somewhat similar to the excitation-dependent
ing to Latvaꢀs empirical rule, an optimal ligand-to-metal
3
+
3
5
energy transfer process for Ln needs DE = pp*ꢀ D =
J
[
9b,c]
ꢀ1
3+ [13]
fluorescence properties of the as-obtained CDs.
We
2500–4000 cm for Eu . Based on the low-temperature
phosphorescence spectrum of the CDs-Gd-HL nanocompo-
sites, we calculated the energy level of the triplet excited state
believe that these interesting properties of the CDs should
be helpful in anti-counterfeiting. First, printing patterns can
only be observed under a UV lamp when CDs are utilized as
the fluorescent ink (Figure S9). Moreover, when the concen-
tration of the CDs in the ink changes, the fluorescence color
also changes. As shown in Figure S10, the part of the image
printed with an ink with a low CD concentration was
completely invisible in daylight unlike the area printed at
a higher CD concentration, which can make anti-counter-
feiting marks difficult to duplicate.
ꢀ
1
of the ligand HL to be 22026 cm , which is not very suitable
5
3+
ꢀ1
for energy transfer to the D level of Eu (17500 cm ;
0
Figure S16a). However, the energy level of the triplet excited
state of HL can be tuned by deprotonation on the CDs. As
shown in Figure S16b, the corresponding energy level of the
ꢀ
ꢀ1
ligand L in the CDs-Gd-L nanocomposite (20790 cm ) was
ꢀ1
5
3+
located approximately 3290 cm above the D level of Eu .
0
Thus efficient intramolecular energy transfer is possible. Not
surprisingly, we observed the emissions characteristic of the
As the energy levels of the amide-type b-diketone ligand
N-(2-pyridinyl)benzoylacetamide (HL) can be modulated by
3
+
Eu ion in the fluorescence spectrum of the EuL complex,
[
11]
5
7
acid/base vapor, we further designed a stimuli-responsive
nanocomposite that combines the advantages of the CDs and
which were attributed to the D ! F (J = 0–4) transitions
0
J
upon excitation at l = 370 nm (Figure S17).
ex
3
+
3+
Eu complexes by coordination effects. The Eu ions act as
bridges to join the CDs and HL ligands. The successful
supramolecular assembly of Eu-HL on the surface of the CDs
was investigated by FTIR, UV/Vis absorption, and XPS
spectroscopy. As shown in Figure S11, the HL ligands
exhibited characteristic CꢀH in-plane and out-of-plane
To test potential applications of the CDs-Eu-HL nano-
composites, we further studied the fluorescence properties of
the nanocomposites after deposition on filter paper (with no
background UV fluorescence). The paper was first dipped
into an aqueous solution of CDs-Eu-HL and then dried in air.
The broad emission peak at 450 nm was attributed to the CDs,
and the emission peak at 612 nm was assigned to the
bending and stretching vibrations of the pyridine group at
ꢀ
1
3+
1
157 and 908 cm , respectively. The absorption peaks in the
characteristic transitions of Eu ions. Interestingly, the
fluorescence quickly changed from blue to blue-violet upon
ꢀ1
1
435–1547 cm region can also be attributed to n(C=C) and
n(C=N) bands of the pyridine group. Enol-type C=O stretch-
exposure to Et N vapor (Figures 2a and S18). The average bi-
exponential fluorescence lifetime of Eu in the CDs-Eu-HL
is 390.4 ms (Figure 2b and Table S2), which increases remark-
3
3
+
ing vibrations of the b-diketone give rise to the peak at
ꢀ
1
1
652 cm . These peaks can also be found in the spectra of
CDs-Eu-HL and illustrate that Eu-HL is successfully assem-
bled on CDs through supramolecular coordination to form
the smart nanosystem. The CDs-Eu-HL composites display
ably to 562.22 ms after exposure to the Et N vapor and
decreases again to 396.62 ms upon exposure to HCl gas. Good
reversibility was observed even after six cycles (Figure 2c).
3
2
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Angew. Chem. Int. Ed. 2017, 56, 1 – 6
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