J. Li et al.
Materials Research Bulletin 135 (2021) 111135
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The 1516 cmꢀ
band is ascribed to C C vibration of naphthalene ring
–
–
–
[44]. For OS (Fig. 2b), two bands at 1199/1067 cmꢀ 1 are characteristic
absorptions of SO3ˉ [45]. In Fig. 2c, the 1384 cmꢀ 1 band of NO3ˉ proves
successful synthesis of NO3-LYH [46]. In Fig. 2d, the NO3ˉ band at 1384
cm-1 becomes unobservable, suggesting substitution of NO3‾ by HNˉ and
OS in the HN/OS-LYH. The SO3‾ vibrations observed at 1171/1049 cm-1
signify the presence of OS in the composite. The absorption bands at
1596/1401 cmꢀ 1 can be assigned to ꢀ COOˉ, for which the red shift of
the wavelengths relative to the 1665/1467 cm-1 of ꢀ COOH results
from the deprotonation. The hydrogen bonding interactions of ꢀ COOˉ
with layer ꢀ OH groups also decrease in vibration frequency.
SEM observations were employed for the NO3-LYH and HN/OS-LYH
as shown in Fig. 3. The NO3-LYH precursor (Fig. 3a,a’) exhibits plate-like
morphology with a nearly regular hexagon shape, and some crystals
grow into columnar or flower-like aggregates. The HN/OS-LYH (Fig. 3b,
b’) basically maintains the morphology of NO3-LYH. The coincidence of
morphology of the HN/OS-LYH composite with the NO3-LYH precursor
means a topotactic intercalation process of the organics into the LYH
interlayers.
Fig. 5. Emission spectra of HN/OS-LYH colloid mixed with various metal ions
(λex =355 nm). For measurements, 3 ml of composite colloid mixed with 1 ml of
aqueous solutions containing metal ions in a 1000 ppm concentration. The
‘None’ case is a control experiment, for which 3 ml of composite colloid was
mixed with 1 ml of pure water.
3.2. Luminescence performance of HN/OS-LYH in solid state and
delaminated state
Emission spectra of HN-Na salt and HN/OS-LYH in solid state were
depicted in Fig. 4A. For HN-Na, at the 394 nm excitation (λex ¼394 nm,
with the excitation spectra shown in Fig. S1a), a green emission is
observed at 545 nm (see Fig. 4A-a). For HN/OS-LYH (Fig. 4A-b and
Fig. S1b, λex ¼415 nm), though it is still a green emission, the peak
position appears at 505 nm, with a 40 nm blue-shift, and the lumines-
cence intensity is much enhanced in comparison to HN-Na. It is noted
that in the testing, the solid dosage of HN-Na and HN/OS-LYH composite
is equal, which means a much less HN amount in the HN/OS-LYH. Inter-
molecular aggregation of HN can be prevented by the LYH layers and
interlayered OS [47], thus causing the increased luminescence intensity.
Meanwhile, OS and LYH layers together induce the blue shift of emission
wavelength. The same green color range but different emission position
of the two samples is depicted in the CIE 1931 chromaticity diagram
(Fig. 4A’).
Fig. 6. Fluorescence intensity (525 nm) of HN/OS-LYH colloidal suspension
with the addition of Fe3+ and other metal ions (λex =355 nm). The luminous
intensity of Fe3+ is too low to be displayed.
Luminescence behavior of HN-Na solution and HN/OS-LYH colloid
in FM were investigated. The HN/OS -LYH colloid displays a blue
emission at 480 nm (Fig. 4B-b), forming striking contrast to the green
luminescence (505 nm) of the composite in solid state (Fig. 4A-b) as well
as the green emission (515 nm) of free HNˉ in FM solution (Fig. 4B-a).
This marked blue shift identifies the role of LYH host layers and inter-
layered OS. Moreover, the delamination of the HN/OS-LYH offers much
free space for HNˉ surrounding positively-charged LYH layers (loose
contact), giving the opportunity of OS to play its role in terms of lumi-
nescence regulation. Also, the delamination process may also promote
the appearance of blue emission. The blue shift phenomenon was re-
ported in DDS–AQS/LDH [48]. As we know surfactants may reduce
aggregation of chromophores [49]. Here the OS acts as a diluter for the
luminous organic anions (here is HN) and thus prevents them from ag-
gregation which may reduce the fluorescence [47,50,51]. The CIE 1931
chromaticity diagram and inserted photos in Fig. 4B’ present the
transition from green to blue color of the two samples, coinciding with
the emission spectrum. Here we see the CIE1931 chromaticity dia-
grams enable a clearer view of the emitted color of related samples.
The chromaticity diagram mainly divides three color areas, that is,
red, blue and green. In the present work, in solid state, although
the emissions of HN-Na (545 nm) and the HN/OS-LYH composite
(505 nm) both belong to green luminescence, their emission
wavelengths are different (with 40 nm change), for which the
corresponding position can be displayed in the chromaticity dia-
gram. Moreover, the green emission (515 nm) of the HN-Na solu-
tion and the blue emission (480 nm) of the exfoliated HN/OS-LYH
can be well distinguished and observed in the chromaticity
diagram. Based on integrating sphere technique [52], the PL
quantum yield of the HN/OS-LYH composite was determined to be
23.20 %, which is much larger than that (4.86 %) of the HNA-Na
[39]. The increased quantum yield of the composite demonstrates
the significant function of the LYH layers for improvement of the
luminescence performance of HN.
3.3. Ion recognition of HN/OS-LYH composite
Luminescence performance was studied for HN/OS-LYH mixed with
aqueous solutions containing metal ions at certain concentrations. As
shown in Fig. 5, red shift of emission from 480 nm to 525 nm is found
after addition of aqueous solutions of metal ions, which may be because
of the H2O entrance. To detect the effect of solvents, emission spectra of
HN-Na in H2O, FM and their mixtures were measured (Fig. S2). In pure
FM, water and different proportional FM+H2O, emission wavelengths of
515, 530, and 515ꢀ 530 nm were observed. As shown in Fig. 5, fluo-
rescence intensity varied in the cases with various types of metal ions.
The fluorescence was remarkably quenched by Fe3+, forming sharp
contrast to other metal ions. This may originate from the interactions
between Fe3+ and HN/OS-LYH composite. As known Fe3+ may coordi-
nate with the hydroxyl and carboxylate groups of HN, and radiative
transition can be disrupted, which causes the quenching of fluorescence.
The highly effective recognition capability towards Fe3+ verifies an
admirable fluorescent sensoring. The high selectivity may be due to
strong affinity of Fe3+ with HN. Meanwhile, paramagnetic Fe3+ has
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