Inorganic Chemistry
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Figure 2a, only the C, O, Si, P, Cu, and I elements are detected
in the XPS survey, indicating the high purity of the OIHC
coating. In the C 1s XPS spectrum (Figure 2b), the main peak
at 284.8 eV is consistent with the dominant phenyl
contribution.43 The minor peak at around 286 eV should
have originated from the adventitious atmospheric organic
pollutants. The O 1s and Si 2p spectra (Figure 2c,d) possess
highly symmetric peaks at 532.9 and 103.6 eV, respectively,
indicating a uniform Si−O−Si major constitution and
coinciding with the SiO2 sol−gel configuration with silicon-
(IV) species.43 The P 2p signal at 131.1 eV is in agreement
with the reported P atom corresponding to the phosphine
ligand coordinated to Cu atoms (Figure 2e).55 As for the Cu
and I elements, both Cu 2p3/2 at 933.0 eV and I 3d5/2 at 619.4
eV are consistent with the Cu4I4 XPS data from the literature
(933.00 and 619.72 eV, respectively), demonstrating the
existence of Cu4I4 (Figure 2f,g).43 Notably, the atomic
percentages of P, Cu, and I are 0.3%, 0.25%, and 0.2%,
respectively (Table S2), indicating that the P/Cu/I ratio is
approximatively 1/1/1.
coatings on the quartz substrates are transparent (inset of
Figure 3b). Because the Cu4I4 core is incorporated in the
hybrid coatings, the optical properties of 1 are similar
compared to that of other Cu4I4-based hybrid structures.
Density of states (DOS) calculations of 0D-Cu4I4(F-tpp)4
(Figure 3d) demonstrate similarities and differences in the
atomic state distributions compared to other Cu4I4-based
hybrid structures, indicating that the optical properties of the
Cu4I4-based hybrid coatings can be systematically tuned by
changing either the inorganic species or organic ligands.44,45,45
The photoluminescence (PL) spectrum of compound 1 is
shown in Figure 4a. The yellow emission peak at 580 nm has a
full width at half-maximum (fwhm) of around 110 nm. A 40
nm blue shift was observed compared to its precursor Cu4I4-
dpes (Figure S6). Compound 1 shows a large Stokes shift of
∼325 nm, exhibiting a large energy-level difference between
the absorption excitation state and PL emission state.
Compared to the emission of 0D-Cu4I4(F-tpp)4, compound
1 shows a red shift of around 30 nm (Figure S7). The internal
quantum yield of 1 was measured to be 8.5% under 300 nm
excitation, which is relatively lower compared to those of other
Cu4I4-based compounds.44 The Commission Internationale de
l’Eclairage (CIE) chromaticity coordinates (Figure 4b) for the
emission were calculated to be (0.49, 0.50), indicating that the
emission of compound 1 is orange-yellow light.
In the OIHC material obtained, there are two types of
inorganic species: CuI and silica. The two types of inorganic
cores are interconnected by the organic species, forming a
cross-linked network (Figure 1c). PXRD analyses have been
carried out, and the results show that the as-made network is
totally amorphous structure (Figure 3a). No peak for CuI has
As shown in previous studies for Cu4I4-based clusters,
thermochromic luminescence of compound 1 is revealed by
immersion of 1 in liquid nitrogen.54 Under the same UV
excitation, the orange-yellow emission becomes a sharp-yellow
emission (inset of Figure S8). The emission spectrum of
compound 1 at 77 K has been collected (Figure S8), which
shows that the emission intensity increases and the emission
band becomes narrower at lowered temperatures. Also, blue
shifts in the emission energies have been observed as the
temperature is decreased. About a 20 nm blue shift in its
emission spectrum was observed by lowering the temperature
from room temperature to 77 K. This can be explained by the
reduced structural torsion and increased localization of the
excited state on the Cu4I4L4 cluster.56 Figure S9 displays the
luminescence decay of 1 at room temperature, and it shows
that compound 1 has a long lifetime of approximately 2.35 μs
by monoexponential fitting. This is in accordance with the
lifetime values of other luminescent Cu4I4-based organic−
inorganic hybrid materials.45
The sol−gel coating materials are luminescent under UV
excitation (inset of Figure 4a) and can be coated onto the
various kinds of substrates by a spin-coating technique. The
detailed coating preparation procedure is described in the
that the quartz substrates are completely transparent under
nature light. Upon 254 nm UV-light irradiation, the quartzes
exhibit intense yellow-light signals (Figure 4c). The scanning
electron microscopy (SEM) image shows the formation of a
uniform, homogeneous, crack-free, and highly adherent
protective film on the rectangular quartz substrate coated
with hybrid coatings (Figure S5). The coatings can also be
coated on metallic surfaces, as shown in the inset of Figure 4b.
The luminescent coatings show good air and moisture stability.
After the coated quartz was exposed to open air for 1 month,
no noticeable change in the luminescent intensity is observed.
After the coated quartz was heated at 45 °C overnight, the
surface morphology and luminescence intensity of the coatings
show negligible changes (Figure S10). However, the coatings
Figure 3. (a) PXRD patterns of compound 1. (b) FT-IR spectrum of
compound 1. (c) UV−vis absorption spectrum of coatings on quartz.
Inset: Photograph of the quartz coated with the hybrid material. (d)
DOS plot of 0D-Cu4I4(F-tpp)4.
been observed in the PXRD pattern, indicating full
incorporation of the inorganic component in the network
structure. Fourier transform infrared (FT-IR) spectroscopy
shows that the sample exhibited a strong absorption peak at
792 cm−1, corresponding to the absorption peaks of the Si−
O−Si stretching and Si−O−Si bending vibrations, respectively
(Figure 3b). The absorption peaks of the stretching vibrations
of −CH3 and −CH2− in the range of 3000−2800 cm−1 as well
as the CC stretching vibration of a double bond at 1640
cm−1 demonstrate the successful reaction of Cu4I4-dpes with
TEOS via a sol−gel method.
Optical diffuse-reflectance spectra were collected at room
temperature. The dried sample of the OIHC material is
colorless, and the absorption spectrum shows that the OIHC
material exhibits no absorption in the visible-light region. The
C
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