P. Rana, R. Gaur, B. Kaushik et al.
Journal of Catalysis 401 (2021) 297–308
ture of 150ꢀC to determine the specific surface area, pore volume
and pore size distribution. Metal content of the catalyst was mea-
sured on Perkin Elmer Avio 200 ICP-OES System. Magnetization of
the nanoparticles were confirmed by using a vibrating sample
magnetometer (EV-9, Microsense, ADE) in the range of ꢁ10000
Oe to 10,000 Oe. The cyclic voltammetry (CV) curve was recorded
on an Autolab Potentiostat Galvanostat (AUT204 Netherlands). The
measurement was performed utilizing a three-electrode system
with ITO coated glass electrode as the working electrode, platinum
(Pt) as the counter electrode, and silver-silver chloride (Ag/AgCl) as
the reference electrode in PBS solution of pH 7.0 containing 5 mM
of [Fe(CN)6]3-/4-. The optimization studies and control experiments
were carried out using an Agilent gas chromatograph (6850 GC)
having a HP-5MS capillary column (stationary phase: 5% phenyl
methyl siloxane; column length: 30 m; internal diameter:
(TRPL) spectroscopy; which showed the steady-state emission
spectra excited at 355 nm, the Ir@PyBz@ASMNPs showed strong
emission peaks at 430 nm (Fig. 2a). Such observed emission of
Ir@PyBz@ASMNPs is due to effective electron transfer process
and inhibited recombination of electrons and holes. Such observed
phenomenon; eventually promotes electron transfer and reduces
the photogenerated electron–hole recombination rate via inhibi-
tion of charge carrier recombination [39,42,43]. In addition; Time
resolved photoluminescence (TRPL) spectroscopy carried out for
Ir@PyBz@ASMNPs photocatalyst; confirms ligand–metal charge
transfer lifetimes which showed an average fluorescence decay
lifetimes (save) of 13.6 ns. Observed fluorescence decay lifetimes
(save) could be well attributed to the emergence of a non-
radiative pathway from Ir(ppy)3 organometallic complexes well
supported over heterogeneous system (Fig. 2b) [44] suggesting
that photo generated charge carriers survived longer on its surface.
The generated sites might be working as a bridge to facilitate the
faster electron transfer and enhancing the charge density on Ir cen-
tre thus reducing the photocarrier transfer barrier and enabling the
photocatalytic activity. On another note; since Ir(ppy)3 based
organometallic complexes, are good organic phosphorescent mate-
rials system and well known for absorbance due to the large
amount of spin–orbit coupling induced by the heavy metal ion
0.25 mm; film thickness: 0.25
lm) and a quadrupole mass filter
equipped 5975C mass selective detector (MSD) using helium as a
carrier gas. 1H NMR (400 MHz) and 13C NMR (100 MHz) spectra
were recorded on a JEOL JNM-EXCP 400 unless otherwise noted
and data are reported in terms of chemical shift related to CDCl3
(7.26 ppm) or with tetramethylsilane (TMS, d 0.00 ppm) as the
internal standard, abbreviation used to indicate the multiplicity
(s = singlet, d = doublet, t = triplet, q = quartet, m = multiplet,
dd = doublet of doublet, dt = doublet of triplet, ddd = doublet of
doublet of doublet), coupling constant (Hz), integration. Thin-
layer chromatography (TLC) was performed by utilizing Merck sil-
ica gel plates 60 F254 to check the course of reactions and visual-
ized under UV light. Light Source. 12 W Philips white LEDs, Quantity
of Light Source: Two
[44–46]. The PL excitation
ꢁ
emission map of the Ir@PyB-
z@ASMNPs is presented in Fig. 2c where Ir based photocatalyst
exhibited an excitation-dependent emission since the position of
the emission peak widely shifts over a wide range of excitation
wavelengths [44–46]. The crystallographic properties and struc-
tures of the MNPs and Ir@PyBz@ASMNPs photoredox nanocatalyst
were also characterized by X-ray diffraction (XRD). The XRD pat-
tern of the fabricated Ir@PyBz@ASMPs photoredox nanocatalyst
exhibited consistency with the peaks of Fe3O4 (Fig. S4a) along with
the emergence of a new strong diffraction peak at 12.9ꢀcorrespond-
ing to the IrPC moiety (Fig. S4b) [44,47]. X-ray photoelectron spec-
troscopy (XPS) was carried out to investigate the surface chemical
nature of Ir in Ir@PyBz@ASMNPs. As shown in Fig. 3a, the Ir binding
energy spectra displayed two emission peaks at 60.2 eV (Ir 4f7/2
level) and 63.3 eV (Ir 4f5/2 level) respectively, which is in agree-
ment with the XPS spectra of Ir 4f region reported in literature
and can be attributed to Ir (+3) [15–17,48]. Survey scan and
detailed XPS spectra of the elements manifest the presence of Fe
2p, Si 2p, C 1 s, N 1 s and O 1 s in the final Ir@PyBz@ASMNPs
(Fig. S5). The transmission electron microscopy (TEM) analysis
was carried out to record images of MNPs, SMNPs and Ir@PyB-
z@ASMNPs (Fig. 3b-d). From the TEM image of MNPs (Fig. 3b), it
is evident that MNPs have an average diameter of 13 nm. The inset
of Fig. 3b spectacles the selected area electron diffraction pattern
(SAED) of MNPs. The bright diffraction rings and white spots points
towards the highly crystalline nature of the synthesized magnetic
nanoparticles. TEM image of SMNPs reveals a silica coating of
about 6 nm in thickness over the MNPs (Fig. 3c). Furthermore,
TEM images of MNPs and SMNPs nanoparticles show the spherical
morphology of the nanoparticles. In addition, the TEM image in
Fig. 3d indicates that Ir@PyBz@ASMNPs have some irregular spher-
ical nanoparticles in the range of 23–26 nm.
3. Results and discussion
3.1. Characterization of the photoredox nanocatalyst
Characterization of the structure of iridium photoredox
nanocatalyst, Ir@PyBz@ASMNPs was verified by employing various
physico-chemical techniques. Fourier transform infrared (FT-IR)
was carried out to identify the functional groups present at each
stage during the synthesis of the catalyst (Fig. S2, see SI for details).
The observed photocatalytic result can be correlated with the opti-
cal properties of Ir@PyBz@ASMNP photocatalyst; such as UV–Vis
diffuse reflectance spectrum, photoluminescence, time resolved
photoluminescence (TRPL) analysis and Excitation-emission color
map are plotted in Fig. S3 and Fig. 2 a, b, c respectively. Primarily;
UV–Vis spectrum of homogeneous iridium photocatalyst displays
an intense absorption peak at 280 nm in the range of 250 nm to
350 nm in MeOH, shows intense absorption from ligand
p – p*
and MLCT transitions Fig. S3. The * absorption (singlet–singlet
p– p
ligand-centered) band for both (homo and hetero) Ir organometal-
lic complex falls in the range 250–320 nm which is an intense
ultraviolet band, and closely resembles the spectrum of the free
ppy ligand associated with Ir metal center [38,39]. Clear evidence
for significant mixing of the singlet and triplet excited states is
seen in both the absorption and emission spectra of Ir@PyB-
z@ASMNPs photo-catalysts. On another note, the weaker absorp-
tion band 375 nm that extend to the visible region of low energy
is conventionally assigned to metal-to-ligand charge-transfer tran-
sitions (3MLCT) (Fig. S3). Both 1MLCT and 3MLCT bands are typi-
cally well observed in both homogeneous and heterogeneous Ir-
organometallic based complex system. Such absorption spectrum
of Ir@PyBz@ASMNPs were well matched and nearly the same as
that for Ir(ppy)3 complexes as reported previously [37,40–42].
Furthermore; the separation of photogenerated electrons and
holes in Ir@PyBz@ASMNPs generated system was investigated
through photoluminescence and time resolved photoluminescence
Likewise, the SEM images of Ir@PyBz@ASMNPs also reveal that
the iridium based photoredox nanocatalyst retains the spherical
shape (Fig. S6). The qualitative analysis of elements (Fe, Si, C, N,
O and Ir) was performed by energy-dispersive X-ray Spectroscopy
(EDS) and energy dispersive X-ray Fluorescence (ED-XRF) (Fig. S7)
while quantitative determination of iridium metal content in the
Ir@PyBz@ASMNPs was accomplished by ICP-OES and was found
to be 0.1207 mmol gꢁ1. The magnetization properties of the MNPs,
SMNPs and Ir@PyBz@ASMNPs were recorded by using vibrating-
sample magnetometer (VSM) at room temperature (300 K)
(Fig. S8). The saturation magnetization, Ms value of the Ir@PyB-
301