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Y. Li et al. / Journal of Organometallic Chemistry 917 (2020) 121274
sensing CN ions has become a very important research line.
Recently, various CN sensors have been developed with diverse
structures, such as organic molecules [24,25], metal complexes
[26,27], nanoparticles [28] etc. Among them, CN sensors based on
metal complexes can show advantages of easy preparation and
environmental compatibility. Importantly, metal complexes can
possess ability of phosphorescent emission which can guarantee
high sensitivity and avoiding interference from background. For the
time being, handful Zn(II) [29], Cu(II) [30], Co(II) [31], Os(II) [32]
and Ni(II) [33] complexes have been prepared to detect CN ions
with fluorescence or absorbance as reporting signal, which cannot
afford the merits associated with phosphorescent reporting signal.
Recently, phosphorescent Ir(III) [18e20] and Ru(II) [34,35] com-
plexes have been employed to sense CN ions based on either
addition reaction of the organic ligands with CN ions or bonding
functional groups, such as -B(Mes)2 [19,20,35]. Clearly, sensing CN
ions by addition reaction may have chance to induce slow
responding speed and high detection limit (DL). Generally, Ru(II)
phosphorescent complexes possess low phosphorescent quantum
yield (FP), which might disfavor ion sensing with emission as
reporting signal.
2.4. Emission and absorption titration
A THF solution of [nBu4N]CN (ca.1 ꢀ 10ꢁ3 M) was added to a THF
solution of the iridium complex (ca. 1 ꢀ 10ꢁ5 M) in a screw-capped
UV or PL cell according to the target [B]: CN ratio via a micro-
syringe. After gentle mixing, the solution in the UV or PL cell was
allowed to stand in the dark for 5 min before measurement. The
detection limit (DL) was determined from the absorption titration
data based on the reported method [38]. The absorption intensity
data at ca. 341 nm were taken to calculate the DL.
3. Results and discussion
3.1. Chemical structure and electronic spectra
Chemical structure of the employed phosphorescent ppy-type
Ir(III) complex IreB is shown in Fig. 1a. It had been synthesized
by our previous method [36]. In IreB, -B(Mes)2 has been intro-
duced to the pyridyl unit in each of the two ppy-type ligands
(Fig. 1a). With sensing purpose, CN ions are supposed to bind with
boron atom in the -B(Mes)2 unit.
So, in this research, a highly phosphorescent ppy-type Ir(III)
complex has been employed to detecting CN ions. It has been
shown that both absorption and phosphorescent signals can show
fast response to the external CN ions in THF solution with low DL.
Critically, the phosphorescent signal of the this phosphorescent
Ir(III) complex sensor can show multi emission-color response,
indicating concentration distinguishing ability. The concerned re-
sults can provide useful information for design new phosphores-
cent CN ion sensors with high performance.
Fig. 1b shows the UVevis absorption and photoluminescence
(PL) spectra of IreB in THF. In the absorption spectrum of IreB, two
kinds of absorption bands can be seen clearly with the strong p-p*
absorption band from the organic ppy-type ligands and the low-
energy weak absorption bands from metal-to-ligand charge
transfer (MLCT) absorption bands (Fig. 1b). The strong red phos-
phorescent at ca. 600 nm in the PL spectrum of IreB has been
confirmed to be induced by the radiative decay of the triplet MLCT
excited states (3MLCT). Importantly, IreB can possess very high
phosphorescent quantum yield (FP) of ca. 0.95, favoring its appli-
cation in ion sensing by enhancing sensitivity.
2. Experimental
3.2. CN ion sensing behavior
2.1. General information
Based on the reported photophysical property of IreB, its
phosphorescent emission is induced by the 3MLCT excited states
from by transferring electron from d-orbital of Ir(III) center to the
pp* orbital of the boron atom in the eB(Mes)2 group [36]. If CN ions
interact with boron atom, it should have a great chance to change
the character of the 3MLCT excited states of IreB and hence alter
emission behavior of IreB. Obviously, response of the phospho-
rescent emission from IreB to the CN ions can act as the reporting
signal for sensing CN ions. In addition, different from its Pt(II) an-
alogs, IreB can possess two eB(Mes)2 groups, which can facilitate
interaction between eB(Mes)2 groups and cyanide ions at low CN
concentration. Obviously, it can lower the detecting limit in sensing
CN ions. Hence, IreB should possess great potential to serve as
novel CN ion sensor.
All commercially available chemicals used were not subjected to
further purification. All solvents for the reactions were dried and
distilled in the proper way. The reactions were checked with thin-
layer chromatography (TLC) materials purchased from Merck & Co.,
Inc. Flash column chromatography and preparative TLC plates were
made from silica gel from Shenghai Qingdao (300e400 mesh).
2.2. Synthesis
Synthesis for IreB was according to the well-established two-
step strategy (Scheme S1 in Supporting Information, SI) [19,36]. The
synthetic detail and spectral data for IreB was provided in SI.
In order to evaluate ion sensing ability of IreB, with the
controlled molar ratio between boron atom and CN ion (B: CN), THF
solution of IreB had been titrated with the THF solution of [nBu4N]
CN employed to record variation of the phosphorescent spectrum
of IreB at different B: CN. It has been found that the red phos-
phorescent emission at ca. 600 nm is quenched quickly with adding
CN ion, while a new yellow emission band at ca. 550 nm gradually
appears and is enhanced (Fig. 2). When B: CN value at 1:1, nearly
85% phosphorescent intensity at ca. 600 nm is quenched (Fig. 2).
Adding more CN ion to maintain B: CNat about 1:4, the newly
appeared yellow emission band reaches the highest intensity
(Fig. 2). It should be noted that another new green-emission band at
520 nm can be detected obviously with B: CNat about 1:6 (Fig. 2). It
means that low CN concentration can induce yellow emission and
green emission can appear at higher CN concentration. The in-
tensity variation for the three emission bands can be clearly
2.3. Physical measurements
1H and 13C NMR spectra were recorded in CDCl3 on a Bruker
Avance 400 MHz spectrometer. Chemical shifts were referenced to
the solvent residual peak at
NMR spectra, respectively. UVevis absorption spectra were
measured on a PerkinElmer Lambda 950 spectrophotometer.
Emission spectra and lifetimes for the obtained complex were
recorded on an Edinburgh Instruments, Ltd., (FLSP 920) fluores-
d C
7.26 ppm for 1H and 77.0 ppm for 13
cence spectrophotometer. Phosphorescent quantum yields (Fp
)
was measured in CH2Cl2 solution against fac-[Ir(ppy)3] (Fp ¼ 0.97)
standard at 293 K [37]. The data of elemental analyses were ob-
tained on
a Flash EA 1112 elemental analyzer. Fast atom
bombardment (FAB) mass spectra were recorded on a Finnigan
MAT SSQ710 system.