J. Jiang et al.
Journal of Solid State Chemistry 283 (2020) 121153
Fig. 3. Competitive experiments of ZnAPA in sensing Hg2þ ions with the
interference of other metal ions (100 μM), the baby blue and organic columns
represent in the presence and absence of Hg2þ ions, respectively. (For inter-
pretation of the references to colour in this figure legend, the reader is referred
to the Web version of this article.)
sample in the solid state (Fig. S6), which can be attributed to the metal to
ligand charge transfer. By taking advantage of the ligand-based fluores-
cence of ZnAPA and the attached active sites for guest metal ions, this
material can be used for fluorescent detection of Hg2þ ions. To investi-
gate the ability of ZnAPA to detect a trace quantity of Hg2þ ions, the
suspension state fluorescence experiment was performed. Fig. 2a pre-
sents the fluorescence response of ZnAPA suspension solution (1 mg in 5
mL H2O) with different amounts of Hg2þ ions. With the increasing con-
centration of Hg2þ ions, the intensity of emission at 405 nm for ZnAPA
dramatically decreases; whereas at 100 μM, the intensity decreased by
75%. After that, the emission intensity decreases and the peak shows
slightly red-shift with the Hg2þ concentration raises. The emission of
ZnAPA was completely quenched when concentration of Hg2þ reach
~400 μM. Obviously, in the range of 0–100 μM, the fluorescence in-
tensity of ZnAPA and the concentration of Hg2þ ions delivers a good
linear relationship and the fitted curve follows an equation with a cor-
relation coefficient R2 ¼ 0.9926 and can be described as
I ¼ -69.81 CHg2þ þ 8819
I represent the fluorescence intensity of ZnAPA and C Hg2þ indicates
the concentration of Hg2þ ions. The limit of detection (LOD) can be
calculated using: LOD ¼ 3δ/S, where δ and S indicate the standard de-
viations for blank solutions of fluorescence intensity and the slope of the
fitted curve, respectively. Accordingly, the LOD value of ZnAPA towards
Fig. 2. (a) Fluorescence spectra of ZnAPA (1 mg) in water solution (5 mL) with
increasing amounts of Hg2þ (0, 5, 10, 15, 20, 25, 30, 35, 40, 45, 50, 60, 70, 80,
90, 100, 120, 150, 180, 200, 250, 300, and 400
μM, respectively); (b) the
relationship of peak fluorescence intensity of ZnAPA and concentration of Hg2þ
ions in aqueous solution.
Hg2þ was determined to be 0.1243
reported probes [33,42,43].
μM, which is comparable to many
powder sample of ZnAPA was treated at different temperatures and
characterized by XRD measurement. From the obtained powder XRD
patterns (Fig. S3), ZnAPA was thermal stable after heat treating at 200 ꢀC
in air atmosphere. Moreover, the TG analysis experiments were per-
formed. As can be seen in the TG curve (Fig. S2), ZnAPA undergoes two
steps of weight loses in nitrogen atmosphere: the first mass loss stage, in
the range of 220–300 ꢀC corresponds to the loss of coordinated water
molecule; the second step occurred at 410–800 ꢀC is attributed to the
gradually collapse of the framework. This implies that the main crystal
framework can withstand the high temperature of 410 ꢀC, demonstrating
its good thermostability.
In order to investigate whether ZnAPA acts as a highly selective
fluorescent molecular probe for Hg2þ ion, interference experiment was
performed (Fig. 3). Some possible heavy metal ions in real wastewater
samples were selected, and added consecutively into the suspensions of
ZnAPA, respectively. Clearly, in presence of different kinds of metal ions,
including Agþ, Kþ, Naþ, Liþ, Cd2þ, Ca2þ, Mg2þ, Ni2þ, Zn2þ, Al3þ, and
Cr3þ, no significant fluorescence changes of ZnAPA were detected.
However, after adding Hg2þ ions into the ZnAPA solutions containing
these interfering metal ions, the fluorescence of ZnAPA quenched
immediately. Such results indicate that the Hg2þ induced fluorescence
response was unchanged in the environment of 1 equiv of other inter-
fering metal ions, suggesting that ZnAPA was a high selective probe for
Hg2þ recognition. In general, there are several factors could have con-
tributions to the high selectivity for Hg2þ, such as the suitable pore size of
the framework, the soft acidity, the conjugation of benzene, and the large
radius of the Hg2þ ions [30,31].
The excitation and emission spectra of the free ligand H2APA and as-
synthesized MOFs in the solid state were measured under room condi-
tions and shown in Fig. S5. Upon excitation at 316 nm, the ligand H2APA
exhibits a broad band centered at 416 nm, which is assigned to the π*-π
transition. Compared to free ligand, the emission of ZnAPA shows a
slightly red-shifted emission of the H2APA ligands around at 424 nm.
Interestingly, the compound ZnAPA in aqueous solution exhibits the
maximum emission at 405 nm and a blue shift of 19 nm compared to the
The mechanism of the Hg2þ-induced fluorescence quenching for
ZnAPA was further investigated. In theory, Hg2þ ions could readily
3