Yu-Shuang Guo1, Mei Zhao1, Qiong Wang1, Yu-Qin Chen1, Dian-Shun Guo1. 1. College of Chemistry, Chemical Engineering and Materials Science, Collaborative Innovation Center of Functionalized Probes for Chemical Imaging in Universities of Shandong, Shandong Normal University, Jinan 250014, P. R. China.
Abstract
A challenge in the design of optical and redox-active receptors is how to combine a specific recognition center with an efficient responsive system to facilely achieve multifeature detection in biological and environmental analyses. Herein, a novel ferrocene-rhodamine receptor conjugated with a pyridine bridge was designed and synthesized. This receptor can sensitively sense Hg2+ in aqueous media via chromogenic, fluorogenic, and electrochemical multisignal outputs with a low detection limit and fast response time. Moreover, it can be qualified as a fluorescent probe for effectively monitoring Hg2+ in living cells. A plausible recognition mode was proposed and rationalized with theoretical calculations.
A challenge in the design of optical and redox-active receptors is how to combine a specific recognition center with an efficient responsive system to facilely achieve multifeature detection in biological and n class="Species">environmental analyses. Herein, a novel ferrocene-rhodamine receptor conjugated with a pyridine bridge was designed and synthesized. This receptor can sensitively sense Hg2+ in aqueous media via chromogenic, fluorogenic, and electrochemical multisignal outputs with a low detection limit and fast response time. Moreover, it can be qualified as a fluorescent probe for effectively monitoring Hg2+ in living cells. A plausible recognition mode was proposed and rationalized with theoretical calculations.
Mercury
is one of the most hazardous heavy n class="Chemical">metals because of its
detrimental and accumulated features.[1,2] It is extensively
distributed in water, soil, and atmosphere systems through natural
phenomena and different human activities, resulting in serious public
health and ecological environment problems.[3−5] Once inside
the human body, Hg(II) tends to accumulate in vital organs and impairs
human health even at low concentrations due to its strong affinity
to thiols from enzymes and proteins.[6−9] For example, Hg(II) can cause the serious
Minamata disease.[10] Therefore, it is significant
to develop new strategies for efficiently monitoring Hg2+ ions in aqueous media and biological systems.
Presently, many
techniques have been developed for the detection
of Hg2+, involving liquid chromatography, atomic absorption
spectrometry, solid-phase microextraction, high-performance plasma
emission spectroscopy, etc. These techniques generally require the
tedious sample preparation and expensive equipment.[11−15] By comparison, fluorescent or electrochemical probes
are more popular methods used to survey n class="Species">Hg2+ ions in view
of their high sensitivity and specificity. However, most of them were
built by a singly optical or electrochemical responsive model with
some limitations for the practical usages.[16−22] As of now, there is a paucity of optical and redox-active receptors
designed via a multiple signal model to expand the application scope.
Thus, it is essential to develop multimodel-responsive receptors for
the efficient analysis of Hg2+ in water and living cells.
A key challenge in the design of multimodel-responsive receptors
is how to combine a specific recognition center with a signal output
system aimed to facilely achieve validly multifeature detection. In
recent years, a number of fluorescent probes involving n class="Chemical">rhodamine dyes
have been documented for sensing Hg2+ by the optical response
based on their spiral skeleton and distinctive photochemical features.[23−29] However, a few ferrocene–rhodamine receptors have been reported
for the multifeature detection of Hg2+ ions.[30−33] Herein, we present a multimodel-responsive ferrocene–rhodamine
receptor FR-P (Scheme ) that can efficiently monitor Hg2+ ions in water with a low detection limit (4.14 × 10–7 M) and fast response time (<5 min). Especially, it can be qualified
for testing Hg2+ in living cells. Our strategy is to couple
rhodamine fluorophore with an eminent electrochemical probe so as
to construct a multimodel receptor that combines the ferrocenecarboxamide
function and the rhodamine B spirolactam scaffold with 2,6-pyridinediyl
moiety as a linkage and part of the recognition center.
Scheme 1
Synthesis
of Multiple Model Receptor FR-P
Results and Discussion
Synthesis and Characterization
of FR-P
The pyridine-bridged n class="Chemical">ferrocene–rhodamine B
receptor FR-P, as depicted in Scheme , was facilely synthesized
via two steps.
First, the treatment of rhodamine B chloride with excess 2,6-pyridinediamine
and triethylamine in dichloromethane generated rhodamine B spirolactam I in 52% yield; then, it reacted with ferrocenylformyl chloride
in dichloromethane with triethylamine as a base to produce FR-P in 58% yield. Its chemical structure was fully characterized
by Fourier transform infrared (FT-IR), 1H nuclear magnetic
resonance (NMR), and 13C NMR spectroscopy and high-resolution
mass spectrometry (HR-MS) techniques (Figures S1–S4, Supporting Information).
The structure
of FR-P was further identified by X-ray
diffraction analysis (Tables S1 and S2,
Supporting Information). In the solid state, n class="Chemical">FR-P crystallizes in the P21/c space group with one-molecule solvent containing ca. 69%
CH2Cl2 and 31% MeOH. As shown in Figure , the typical rhodamine B spirolactam
is connected with a ferrocenecarboxamide function by a 2,6-pyridinediyl
linkage. The spirolactam plane is almost vertical to the xanthene
ring and approximately coplanar with the pyridine ring, generating
dihedral angles of 83.4(2)° and 13.5(2)°. On the other hand,
the amide plane of ferrocenecarboxamide is practically coplanar with
its connected cyclopentadienyl ring and 2,6-pyridinediyl ring, forming
dihedral angles of 21.3(3)° and 8.0(4)°, which play a main
role in the electrochemical response. The C5H5 ring of the ferrocenyl group is rotationally disordered over two
positions. Notably, FR-P possesses a ferrocenecarboxamide
function as the electrochemical probe and a rhodamine B scaffold as
the optical probe that are smartly conjugated with a pyridine bridge
to create a multimodel-responsive receptor. Its recognition properties
were fully evaluated with UV–vis, fluorescence, and electrochemistry
techniques as well as theoretical calculations.
Figure 1
Crystal structure of FR-P with one-molecule
solvent containing 31% MeOH and 69% CH2Cl2,
showing the atom-numbering scheme. Displacement ellipsoids are drawn
at the 30% probability level. Hydrogen atoms are omitted for clarity.
Crystal structure of FR-P with one-molecule
solvent containing 31% n class="Chemical">MeOH and 69% CH2Cl2,
showing the atom-numbering scheme. Displacement ellipsoids are drawn
at the 30% probability level. Hydrogen atoms are omitted for clarity.
UV–Vis and Fluorescence
Evaluations
of FR-P
The UV–vis and fluorescence assays were conducted
in an optimized H2O/n class="Chemical">dimethylformamide (DMF) (9:1, v/v)
solution. FR-P (50 μM) shows one absorption
peak at 311 nm in the UV–vis spectrum (Figure S5, Supporting Information), assigned to the ferrocenyl
function. However, no absorption peaks in the visible region above
450 nm were found, confirming that FR-P exists
as a spirolactam form in solution. This corresponds to the chemical
shift at δ = 66.1 ppm in its 13C NMR and belonged
to the tertiary carbon. Next, its UV–vis absorption behaviors
were studied in the presence of different metal ions including
Na+, K+, Cs+, Mg2+, Ca2+, Pb2+, Zn2+, Cd2+, Hg2+, Cu2+, Ag+, Co2+, Ni2+, Nd3+, La3+, Ce3+, and
Eu3+ (Figure ). Gratifyingly, we found that by only adding Hg2+, FR-P can generate a new maximum absorption peak
at 567 nm, showing that its spirolactam ring opened and delocalized
into the xanthene moiety. In this case, an apparent color change in
the solution emerged from yellowish to pink (Figure , top), indicating that FR-P can be applied for the “naked-eye” detection
of Hg2+. However, upon the addition of other metal ions
to the FR-P solution, no corresponding variations
in both color and absorption spectra were observed.
Figure 2
UV–vis absorbance
of FR-P (50
μM) in H2O/DMF (9:1, v/v) at room temperature upon
the addition of various metal ions (250 μM).
Figure 3
Color changes of FR-P (50 μM) in
H2O/DMF (9:1, v/v) under visible (top) and UV (365 nm,
bottom) light in the presence of various metal ions (250 μM),
where 1–17 stand for Na+, K+, Cs+, Mg2+, Ca2+, Pb2+, Zn2+, Cd2+, Hg2+, Cu2+, Ag+, Co2+, Ni2+, Nd3+, La3+, Ce3+, and Eu3+, respectively.
UV–vis absorbance
of FR-P (50
μM) inn class="Chemical">H2O/DMF (9:1, v/v) at room temperature upon
the addition of various metal ions (250 μM).
Color changes of FR-P (50 μM) inn class="Chemical">H2O/DMF (9:1, v/v) under visible (top) and UV (365 nm,
bottom) light in the presence of various metal ions (250 μM),
where 1–17 stand for Na+, K+, Cs+, Mg2+, Ca2+, Pb2+, Zn2+, Cd2+, Hg2+, Cu2+, Ag+, Co2+, Ni2+, Nd3+, La3+, Ce3+, and Eu3+, respectively.
Through the sequential titration of FR-P with n class="Species">Hg2+ ions (Figure ), the absorption peak at 567 nm gradually
increased.
This shows that FR-P possesses a strong
binding affinity to Hg2+ ions with high specificity. In
addition, Job’s plot analyses (Figure S6, Supporting Information) confirm that a 1:1 complex formed between FR-P and Hg2+ in solution with a coordination
constant of 2.8 × 105 M–1, calculated
according to the nonlinear fitting of the titration profile.[34] Significantly, the quick responsive time (<5
min) of FR-P toward Hg2+ was
obtained from the UV–vis absorption spectrum tests in various
time intervals (Figure S7, Supporting Information).
Figure 4
UV–vis
absorbance of FR-P (50
μM) in H2O/DMF (9:1, v/v) at room temperature upon
the titration of Hg2+ (50–900 μM). Inset:
absorbance at 567 nm as a function of Hg2+ concentration.
UV–vis
absorbance of FR-P (50
μM) inn class="Chemical">H2O/DMF (9:1, v/v) at room temperature upon
the titration of Hg2+ (50–900 μM). Inset:
absorbance at 567 nm as a function of Hg2+ concentration.
Moreover, the fluorescence and sensing properties
of FR-P were studied in a n class="Chemical">H2O/DMF
(9:1, v/v) solution.
Free FR-P (25 μM) displays no distinct
fluorescence in the range from 576 to 800 nm excited at 563 nm (Φf = 0.014, vs rhodamine B) (Figure S8, Supporting Information),[35−37] also proving that the spirolactam
structure existed in solution. Upon the addition of Hg2+ ions, FR-P yields a remarkable fluorescence-on
response at 590 nm (Φf = 0.029, vs rhodamine B) with
a color change to pink, verifying that the spirolactam ring of FR-P was opened upon sensing Hg2+.
In the identical conditions, the other metal ions failed to engender
any vital effect on the emission spectra of FR-P (Figure S9, Supporting Information),
which is similar to the UV–vis results. This shows the high
specificity of FR-P toward Hg2+. To evaluate the sensitivity of FR-P to
Hg2+, fluorescence titration assays were further performed
(Figure ). Upon addition
of 10 equiv of Hg2+, the fluorescence intensity of FR-P increased up to ca. 130-fold at 590 nm,
which confirms that FR-P also owns a high
sensitivity for Hg2+ ions.
Figure 5
Fluorescence emission spectra of FR-P (25 μM) in H2O/DMF (9:1,
v/v) at room temperature
upon addition of Hg2+ (25–450 μM). Inset:
fluorescence emission variations at 590 nm with the incremental addition
of Hg2+. λex = 563 nm.
Fluorescence emission spectra of FR-P (25 μM) inn class="Chemical">H2O/DMF (9:1,
v/v) at room temperature
upon addition of Hg2+ (25–450 μM). Inset:
fluorescence emission variations at 590 nm with the incremental addition
of Hg2+. λex = 563 nm.
To examine the practical ability of FR-P as a fluorescent probe, competition experiments were also
performed.
As discussed above, n class="Chemical">FR-P only senses Hg2+, while the other metal ions give a negligibly perceptible
effect (Figure , purplish-red
bars). Next, the fluorescence response of FR-P was measured separately when 250 μM of various interfering
metal ions (Na+, K+, Cs+, Mg2+, Ca2+, Pb2+, Zn2+, Cd2+, Cu2+, Ag+, Co2+, Ni2+, Nd3+, La3+, Ce3+, and
Eu3+) and 125 μM Hg2+ ions (Figure , green bars) were added. No
remarkable variations in the fluorescence emission were found by the
addition of most competitive ions, while only Cd2+, Cu2+, and Eu3+ ions partially quenched the fluorescence
owing to the spin–orbit coupling effect.[38,39]
Figure 6
Fluorescence
intensity of FR-P (25 μM) in H2O/DMF
(9:1, v/v) at 590 nm after the addition of Hg2+ (125 μM)
or other metal ions (250 μM) (purplish-red
bars) and the mixture of various interfering metal ions (250 μM)
with Hg2+ (125 μM) (green bars). λex = 563 nm.
Fluorescence
intensity of FR-P (25 μM) inn class="Chemical">H2O/DMF
(9:1, v/v) at 590 nm after the addition of Hg2+ (125 μM)
or other metal ions (250 μM) (purplish-red
bars) and the mixture of various interfering metal ions (250 μM)
with Hg2+ (125 μM) (green bars). λex = 563 nm.
Electrochemistry
Evaluation of FR-P
In view of FR-P having a redox-active n class="Chemical">ferrocenyl
function, cyclic voltammetry (CV) and differential pulse voltammetry
(DPV) techniques were applied to study its electrochemistry and sensing
properties. We found that FR-P displays
a one-electron quasi-reversible redox peak at E1/2 = 0.670 V with Ipa/Ipc = 1.04, assigned to the ferrocene/ferrocenium
(Fc/Fc+) redox couple. Upon the addition of 1.0 equiv of
Hg2+, the original CV wave of FR-P shifts negatively, forming a new CV wave at E1/2 = 0.625 V with ΔE1/2 =
−50 mV (Figure S11, Supporting Information).
Alternatively, the DPV assays show a similar shift with ΔE = −70 mV, confirming that FR-P can be used as an electrochemical sensor for the detection
of Hg2+ (Figure ). For comparison, the DPV of FR-P was also tested with 1.0 equiv of H+, demonstrating only
a slight shift of Fc/Fc+ with ΔE = −20 mV. Thus, the negative shift can be mainly ascribed
to FR-P binding Hg2+, which increases
the electron density on the ferrocenyl group.[40]
Figure 7
DPV
assays of FR-P (0.5 mM) in MeCN/CH2Cl2 (9:1, v/v) with 0.1 M n-Bu4NClO4 as a supporting electrolyte upon the addition
of 1.0 equiv of Hg(ClO4)2 and 1.0 equiv of HClO4.
DPV
assays of n class="Chemical">FR-P (0.5 mM) in MeCN/CH2Cl2 (9:1, v/v) with 0.1 M n-Bu4NClO4 as a supporting electrolyte upon the addition
of 1.0 equiv of Hg(ClO4)2 and 1.0 equiv of HClO4.
Studies
on the Sensing Mode of FR-P to Hg2+
As of now,
two plausible modes have been documented
for the rhodamine-based probes sensing n class="Species">Hg2+ in the literature:
one is that the probe specifically coordinates Hg2+,[41−44] and the other is that the probe decomposes with the selective catalysis
of Hg2+.[45−48] To verify how FR-P senses Hg2+, we have designed and carried out a few supplementary studies including
HR-MS, FR-IR, and theoretical calculations.
First, a binding
mode between FR-P and n class="Species">Hg2+ was
initially confirmed by the HR-MS analysis based on a typical peak
at m/z 982.2125 corresponding to
a 1:1 complex of FR-P with Hg2+, [FR-P·Hg(II) + Cl]+ (Figure S12, Supporting Information). Next, FR-IR
spectra of FR-P and its Hg(II) complex were
measured to understand the coordination mode (Figure S13). In the FR-IR spectrum of FR-P, the stretching frequency of the spirolactam C=O
bond appears at 1696 cm–1, while it shifts to 1647
cm–1 in that of its Hg(II) complex. Simultaneously,
the pyridine C=N peak moves from 1605 to 1584 cm–1. This implied that the spirolactam ring opens with Hg2+ binding to FR-P.[49,50] Thus, we deduce that the pyridine N atom and two amide O atoms of FR-P possibly coordinate Hg2+ to yield
a chelating complex assisted with the solvent molecule (Figure A).
Figure 8
Plausible binding mode
of FR-P to Hg2+ (A) and the DFT-optimized
structure of complex [FR-P·Hg(II)·DMF]2+ (B), calculated
with the B3LYP/LANL2DZ basis set.
Plausible binding mode
of FR-P to n class="Species">Hg2+ (A) and the DFT-optimized
structure of complex [FR-P·Hg(II)·DMF]2+ (B), calculated
with the B3LYP/LANL2DZ basis set.
To rationalize the mode of FR-P binding
n class="Species">Hg2+, as depicted in Figure A, structures of FR-P and
its Hg(II) complex (Figure S14, Supporting
Information) were optimized with the density functional theory (DFT)
calculations via the Gaussian 09W program. Figure B demonstrates an optimized structure of
complex [FR-P·Hg(II)·DMF]2+ generated with a multibonding mode between FR-P and Hg2+. In this complex, one Hg2+ ion bonds with two amide O atoms and one pyridine N atom
of FR-P together with one amide O atom of
DMF, creating close contacts of dHg–O1 = 2.278 Å, dHg–O2 = 2.227
Å, dHg–N2 = 2.383 Å,
and dHg–O3 = 2.306 Å, as well
as bond angles of N2–Hg–O3 = 154.1° and O1–Hg–O2
= 153.5°. The opening of the spirolactam ring caused a significant
electronic delocalization that can be identified by the variation
of the N3–C4 distance in FR-P and
its Hg(II) complex, which is shortened from 1.401 to 1.310 Å
upon coordinating Hg2+. The addition of Hg2+ opened the spirolactam ring and extended its conjugate system.
The molecular orbitals of FR-P and its
n class="Chemical">Hg(II) complex were also optimized (Table S3, Supporting Information). As shown in Figure , the highest occupied molecular orbital
(HOMO) of FR-P is largely located on the
xanthene unit of rhodamine, while the lowest unoccupied molecular
orbital (LUMO) is mainly distributed over the pyridine ring and the
ferrocenecarboxamide function, with a LUMO–HOMO gap of 3.94
eV (Figure A). For
[FR-P·Hg(II)·DMF]2+, its HOMO is also located on the xanthene ring; however, the LUMO
is diffused over the pyridine and amide groups, with a lower energy
gap of 2.79 eV (Figure B), confirming that [FR-P·Hg(II)·DMF]2+ is more stable than FR-P.
Figure 9
HOMO–LUMO
distributions of FR-P (A) and [FR-P·Hg(II)·DMF]2+ (B), calculated
by the 6-31G** basis set for C, H, N, and
O atoms and the LANL2DZ basis set for Fe and Hg atoms.
HOMO–LUMO
distributions of n class="Chemical">FR-P (A) and [FR-P·Hg(II)·DMF]2+ (B), calculated
by the 6-31G** basis set for C, H, N, and
O atoms and the LANL2DZ basis set for Fe and Hg atoms.
Bioimaging Evaluations of FR-P
After
extensive evaluations, we found that FR-P has high sensitivity, good selectivity, and fast response time for
monitoring n class="Species">Hg2+ in aqueous media. Encouraged by these advantages,
we continue to examine the potential applications of FR-P in fluorescence imaging of Hg2+ in living
cells. The evaluation of FR-P to survey
intracellular Hg2+ in HeLa cells was assessed by fluorescence
imaging studies. As shown in Figure , the HeLa cell lines incubated with FR-P (50 μM) at 37 °C for 30 min show no fluorescence
(Figure a), confirming
that the spirolactam scaffold of FR-P is
stable enough to tolerate the HeLa cell lines. However, when adding
Hg2+ ions (100 μM) to the preincubated HeLa cells
for less than 10 min, strong fluorescence appears (Figure d). These results imply that FR-P can be qualified as a fluorescence imaging
probe for the survey of intracellular Hg2+ ions in living
cells.
Figure 10
Bioimaging assays of FR-P in HeLa cells.
Images of HeLa cells treated with FR-P (50
μM) for 30 min (a–c) and then incubated with Hg2+ (100 μM) for 10 min (d–f) ((b, e) bright-field image;
(c, f) overlay images of (a, b) and (d, e)). Fluorescence signals
were collected at 570–650 nm for the red channel (λex = 561 nm).
Bioimaging assays of FR-P inn class="CellLine">HeLa cells.
Images of HeLa cells treated with FR-P (50
μM) for 30 min (a–c) and then incubated with Hg2+ (100 μM) for 10 min (d–f) ((b, e) bright-field image;
(c, f) overlay images of (a, b) and (d, e)). Fluorescence signals
were collected at 570–650 nm for the red channel (λex = 561 nm).
Conclusions
A novel optical and redox-active ferrocene–n class="Chemical">rhodamine receptor
linked by a pyridine moiety has been successfully designed and prepared
for the multifeature detection of Hg2+ in water and living
cells. The pyridine ring plays a key role in both creating the recognition
center and regulating the responsive system. This receptor features
a high selectivity, a low detection limit (4.14 × 10–7 M), and a fast response time (<5 min) to Hg2+. Moreover,
theoretical calculations are applied to understand and rationalize
the sensing mode.
Experimental Section
Materials and Instruments
All starting
materials and solvents were commercially available and utilized without
further purification. Stock solutions of FR-P and all n class="Chemical">metal salts were prepared in DMF and distilled water, respectively. 1H NMR and 13C NMR spectra were obtained using BRUKER
ADVANCE 300/400 spectrometers (CDCl3, TMS as an internal
standard). FT-IR spectra (KBr pellets) were recorded in the range
of 400–4000 cm–1 with a PerkinElmer 1600
FT-IR spectrometer. Electrospray ionization mass spectra (ESI-MS)
were obtained using a maXis UHR-TOF system. Melting points were measured
using a Yanaco MP-500 micromelting point instrument and uncorrected.
UV–vis spectra were recorded using a TU-1900 UV–vis
spectrometer. Fluorescence spectra were measured using an RF-6000
Shimadzu fluorescence spectrometer. Electrochemical analyses were
carried out using a CHI660 electrochemical analyzer.
Synthesis of FR-P
To a solution of
rhodamine B spirolactam I (prepared as the known procedure,[51] 0.320 g, 0.6 mmol) and Et3N (1.0
mL) in anhydrous n class="Chemical">CH2Cl2 (10.0 mL) was added
dropwise a solution of ferrocenylformyl chloride (0.298 g, 1.2 mmol)
in anhydrous CH2Cl2 (10.0 mL) at 0–5
°C. The resulting mixture was stirred at room temperature for
12 h. After the completion of the reaction the resultant solution
was added to ice water, and the organic phase was washed with saturated
NaHCO3 and brine and then dried over anhydrous MgSO4. The volatile was removed under reduced pressure, and the
residue was subjected to column chromatography on silica gel (ethyl
acetate/hexane = 1:2, Rf = 0.5), providing
0.260 g (yield 58%) FR-P as an orange solid;
m.p. 224–226 °C. FT-IR (cm–1): vmax 1697 (C=O), 1605 (C=N). 1H NMR (400 MHz, CDCl3, TMS): δ 8.27 (d, J = 7.8 Hz, 1H), 8.02–8.00 (m, 1H), 7.92 (s, 1H),
7.75 (d, J = 7.7 Hz, 1H), 7.58 (d, J = 8.1 Hz, 1H), 7.55–7.50 (m, 2H), 7.18–7.16 (m, 1H),
6.48 (d, J = 2.6, 2H), 6.42 (s, 1H), 6.41 (s, 1H),
6.16 (dd, J = 8.9, 2.6 Hz, 2H), 4.95 (s, 2H), 4.52
(s, 2H), 4.31 (s, 5H), 3.28 (q, J = 7.0 Hz, 8H),
1.10 (t, J = 7.0 Hz, 12H). 13C NMR (100
MHz, CDCl3, TMS): δ 168.5, 167.9, 153.8, 153.3, 148.6,
139.5, 133.8, 130.7, 128.3, 124.4, 123.1, 110.3, 109.0, 107.0, 96.8,
71.2, 70.0, 68.1, 66.1, 53.3, 44.2, 12.7. HR-MS: m/z [M]+: calcd. for C44H43FeN5O3: 745.2715; found: 746.2786 ([M+H]+).
Crystal Structure Determination
Orange
single crystals were developed through slow evaporation of a solution
of FR-P inn class="Chemical">CH2Cl2/MeOH
(1:1, v/v) at 0–4 °C. The selected single crystal of FR-P was mounted on the glass fiber. The intensity
data were measured at 293 K on an Agilent SuperNova CCD-based diffractometer
(Cu Kα radiation, λ = 1.54184 Å).[52] Empirical absorption corrections were used with SCALE3
ABSPACK. The structure was solved by direct methods and difference
Fourier syntheses and refined by the full-matrix least-squares technique
on F2 with SHELXS-97[53] and SHELXL-97.[54] All nonhydrogen atoms were refined using anisotropic
displacement parameters. Hydrogen atoms linked to refined atoms were
placed in geometrically idealized positions and refined by a riding
model with C–H = 0.93, 0.97, and 0.96 Å for aromatic,
methylene, and methyl H, respectively, Uiso(H) = 1.5Ueq(C) for methyl H, and Uiso(H) = 1.2Ueq(C)
for all other H atoms. Crystallographic data for FR-P have been deposited with the Cambridge Crystallography Data
Centre (CCDC No. 1978652).
UV–Vis/Fluorescence
and Electrochemistry
Tests
A stock solution of FR-P (0.5
mM) was prepared inn class="Chemical">DMF, and the stock solutions of all metal salts
(5.0 mM) were prepared in distilled water. The solution of FR-P was then diluted to 50 and 25 μM with H2O/DMF (9:1, v/v) solvents for UV–vis and fluorescence
studies, respectively. For fluorescence tests, the excitation was
provided at 563 nm, while the emission was collected from 576 to 800
nm. The fluorescence intensity at 590 nm was used to assess the performance
of the proposed assay strategy. Both excitation and emission slits
applied in the assays are 5 nm. Cyclic voltammetry (CV) and differential
pulse voltammetry (DPV) experiments were carried out using a solution
of FR-P (0.5 mM) in MeCN/CH2Cl2 (9:1, v/v) with 0.1 M n-Bu4NClO4 as the supporting electrolyte and Hg/Hg2Cl2 as the reference electrode, along with platinum working and
auxiliary electrodes. DPV measurements were performed with a 50 ms
pulse width and a scan rate of 100 mV s–1.
Cell Culture and Fluorescence Imaging
HeLa cells were
cultured in Dulbecco’s modified Eagle’s
medium (n class="Chemical">DMEM) along with 10% fetal bovine serum, 100 U/mL penicillin,
and 100 μg/mL streptomycin and incubated at 37 °C in a
humidified atmosphere of 5% CO2 and 95% air. The sample
was excited at 561 nm, and the emission spectrum collection ranges
from 570 to 650 nm.
Before the experiments, HeLa cells were
washed with n class="Chemical">phosphate-buffered saline (PBS) buffer and then incubated
with 50 μM FR-P in PBS/DMF (2:1, v/v)
at 37 °C for 30 min. At last, 100 μM Hg2+ was
added for the amplification reaction. The process was carried out
at 37 °C for 10 min. Cell imaging was then performed after washing
cells with PBS.
Theoretical Calculations
All ground-state
optimizations were performed with the density functional theory (DFT)
using the Gaussian 09W program. All geometry optimizations were made
with tight convergence criteria in the gas phase by utilizing the
B3LYP level, with the 6-31G** basis set for C, H, N, and O atoms and
the LANL2DZ basis set for Fe and n class="Chemical">Hg atoms.[55,56]