Rahul Bhowmicka,
Rabiul Alama,
Tarun Mistria,
Kalyan Kumar Dasa,
Atul Katarkarb,
Keya Chaudhurib and
Mahammad Ali*a
aDepartment of Chemistry, Jadavpur University, Kolkata 700 032, India. E-mail: m_ali2062@yahoo.com
bMolecular & Human Genetics Division, CSIR-Indian Institute of Chemical Biology, 4 Raja S.C. Mallick Road, Kolkata-700032, India
First published on 20th January 2016
We report herein the development of a novel, diformyl-p-cresol (DFC)–thiosemicarbazide (TS) based sensor (DFC–TS) that selectively and sensitively recognizes Zn2+ by both UV-Vis and fluorescence methods. The gradual addition of Zn2+ to a solution of the ligand developed a new absorption band at 430 nm, while the bands at 370 and 316 nm gradually decrease generating one well defined isosbestic point at 390 nm exhibiting ∼17 fold turn-on fluorescent enhancement (FE). When we plot absorbance (at 430 nm) vs. [Zn2+] there is a gradual increase in absorption with [Zn2+], becoming saturated at ∼1 equivalent of Zn2+ and then again it increases with the increase in [Zn2+] and ultimately becomes saturated at ∼2 equivalents of added Zn2+. This clearly demonstrates that the Zn2+ binding event to the ligand occurs in two steps, one at a time. Non-linear least-squares computer-fitting of these data gives the parameters: K′f1 = (9.70 ± 5.51) × 105 M−1, n = (1.28 ± 0.05) for the first step and K′f2 = (1.11 ± 0.65) × 105 M−1 and n = (1.01 ± 0.06) for the second step. So far, this study provides the opportunity where we have successfully, for the first time, determined the stepwise formation constants; though they have values of the same order of magnitude. The ground state geometries of DFC–TS, both enol and keto forms and [Zn(DFC–TS)(OAc)], [Zn(DFC–TS)(OAc)]−, and [Zn2(DFC–TS)(OAc)2] were optimized using the Gaussian-03 suit program and bond distances of all species are in reasonable agreement with the reported values.
The mechanistic details of zinc homeostasis are not entirely clear,5 partly due to the difficulty in directly mapping the distribution and tracking the movement of the spectroscopically inert free zinc ions. Therefore, zinc ion-selective fluorescent probes have been the primary tools for the detection and quantification of biological free zinc. The past decade has witnessed the rapid progress in the development of zinc probes,6 which have enabled significant advances in the cell biology of zinc.7
Though the chemistry of thiosemicarbazones (Scheme 1) has been studied for a considerable period of time for their biological properties, the first report on their medicinal applications started to appear in the fifties as drugs against tuberculosis and leprosy.8 In the sixties their antiviral properties were discovered and a huge amount of research was carried out that eventually led to the commercialization of methisazone, Marboran® etc. to treat smallpox9 During this period the first antitumor activity results was published.10 Recently, triapine (3-aminopyridine-2-carboxaldehyde thiosemi-carbazone) has been developed as an anticancer drug for several cancer types.11
Understanding the excited-state proton/hydrogen-atom transfer Excited State Proton Transfer (ESPT) reaction is fundamental in chemistry and biology.12 Taylor reported the first case of excited state biprotonic transfer in 7-azaindole13 and Tahara14 proved that this proton transfer mechanism is a concerted process with the initial formation of a dimer in solution. Villani15 recently proved that the trans-formation of the Watson–Crick (WC) DNA base pairs to their tautomers is achieved via a concerted double-hydrogen transfer process beginning with a hydrogen atom of a purinic base. The ESIPT reaction in green fluorescent protein (GFP) has also attracted much interest,16 because it is a major tool in many areas of the life science. ESIPT molecules have attracted attention for various applications including chemical sensors,17 luminescent materials18 and functional polymers.19 A distinctive feature for the ESIPT molecules is that their fluorescence is well separated from their absorption maxima (>100 nm). This resulting unusually large Stokes shift is an obvious advantage over other normal fluorophores, such as fluorescein, rhodamine or coumarin, as they can avoid self-absorption and thus the inner filter effect in fluorescence analysis.
In the present article we are going to disclose a simple and easily synthesizable DFC–TS based turn-on colori- and fluorimetric dual sensor for Zn2+.The promise of this new ligand as a quantitative probe for Zn2+ is demonstrated by its use in the estimation of affinities towards Zn2+ through absorption and fluorescence changes occurring mainly due to ESIPT blocked Chelation Enhanced Fluorescence (CHEF) effect. Most striking feature of this study is that it enables us, for the first time, the direct determination of stepwise formation constants (K′f1 and K′f2); though they are of same order of magnitude and otherwise, very difficult to determine by any suitable analytical techniques. In addition, the ligand displays ESIPT behavior with large Stokes shift (>155 nm) that can avoid self-absorption and thus the inner filter effect in fluorescence analysis.
:
1 Zn2+ complex and 2.19 (s, 3H, methyl), 2.52 (2-H, NH), 7.31 (s, 2H, azomethine), 8.31 (s, 2-H, aromatic), 6.43 (s, 4H, NH2) for 1
:
2 Zn2+ complex, (please see Fig. S2 and S3†). ESI-MS+ (m/z): 372.9884, (DFC–TS + Zn2+) (1
:
1), 514.9107 ([Zn2(DFC–TS)(OAc)(H2O)]+) (please see Fig. S8 and S9†).
:
1 DMSO
:
H2O) was prepared and pH was adjusted to 7.2 by using HCl and NaOH. 2.5 ml of this buffer solution was pipetted out into a cuvette to which 20 μM of the probe was added and Zn2+ ion was added incrementally starting from 0 to 46 μM in a regular interval of volume and UV-Vis and fluorescence spectra were recorded for each solution. Path lengths of the cells used for absorption and emission studies were 1 cm. Fluorescence measurements were performed using 2 nm × 2 nm slit width.
For competition assays 1.0 × 10−3 M Na2H2EDTA solution was prepared in water. 2.5 ml of the buffered solution was pipetted out into a cuvette to which 20 μM of the DFC–TS was added and Zn2+ ion was added in 1
:
1 and 1
:
2 mole ratio separately and then Na2H2EDTA solution was added incrementally starting from 0 to 44 μM in a regular interval of volume and UV-Vis and fluorescence spectra were recorded for each solution.
| Kcomp = [M–L2][L1]/[M–L1][L2]; Kcomp = KL2/KL1 |
Emission spectra were recorded by excitation at 430 nm. Both excitation and emission slit widths were 2 nm. The equilibrium competition constant (Kfi-comp) (i = 1 and 2 for 1
:
1 and 1
:
2 L
:
M mole ratios respectively) were calculated based on the titration curve.
:
water = 1
:
9 (v/v))] in the culture medium, allowed to incubate for 30 min at 37 °C. After incubation, cells were washed twice with phosphate-buffered saline (PBS). Bright field and fluorescence images of HepG2 cells were taken by a fluorescence microscope (Leica DM3000, Germany) with an objective lens of 40× magnification. Fluorescence images of HepG2 cells were taken separately from another set of experiment where cells incubated with 10 μM DFC–TS + 10 μM Zn2+ for 30 min. Similarly, in another set of experiment, cells were incubated with 10 μM DFC–TS + 10 μM Zn2+ for 30 min followed by addition of 100 μM EDTA for another 30 min and fluorescence images were taken. HepG2 cells showed almost complete quenching of fluorescence due to removal of Zn2+ from the DFC–TS–Zn2+ complex.
The electronic absorption spectral properties of DFC–TS were investigated in 9
:
1 DMSO–H2O at pH 7.2 HEPES buffer. The absorption spectrum of DFC–TS presents two important transitions with intense absorption bands at 316 and 370 nm. As Scheme 2 describes, there is an equilibrium between the two configurations, enol and keto tautomers of DFC–TS due to ESIPT. The band at 370 nm is assigned to the transition to quinoid (keto) form. On gradual addition of Zn2+, the absorption bands of DFC–TS at 370 and 316 nm decrease gradually; however, a new peak appears at 430 nm thereby generating one well defined isosbestic point at 390 nm indicating a clean transformation of free ligand to its metal bound state (Fig. 1, S10 and S11†). This clearly indicates the chelation of Zn2+ by the multidentate ligand moiety giving [[Zn(DFC–TS)]+ and [Zn2(DFC–TS)]+]. The spectral change (decrease in absorbance at 370 nm and increase at 430 nm) clearly indicate that the addition of Zn2+ ion induces the decrease in concentration of free ligand both in keto and enol forms. Here the nitrogen atom of the azomethine group takes part in the coordination with Zn2+ and the formation of complexes Zn–DFC–TS and Zn2–DFC–TS inhibit the ESIPT (Scheme 2).
The cation binding affinities of sensor toward Zn2+ was investigated by UV-Vis absorption studies and when a change in absorbance at 430 nm was plotted against [Zn2+], there is a gradual increase in absorbance with [Zn2+], gets saturated at ∼1 equivalent of Zn2+ and then it again increases with the increase in [Zn2+] and finally get saturated at ∼2 equivalent of added Zn2+ (inset (b), Fig. 1). This clearly demonstrates that the Zn2+ binding event to the ligand occurs in two steps, one at a time. Non-linear least-squares fit of the data to eqn (1)
| y = (a + b × c × xn)/(1 + c × xn),21 | (1) |
| Formation constant | Spectrophotometrically | Fluorometrically |
|---|---|---|
| K′f1 | (9.7 ± 5.51) × 105 M−1 | (7.17 ± 0.2) × 104 M−1 [(1.14 ± 0.47) × 105 M−1; λex = 430 nm] |
| K′f2 | (1.11 ± 0.65) × 105 M−1 | — |
| K′f1 (competition) | (2.28 ± 0.32) × 105 M−1 | (1.38 ± 0.29) × 105 M−1 |
| K′f2 (competition) | (1.64 ± 0.17) × 105 M−1 | (7.2 ± 2.3) × 104 M−1 |
We have also attempted to determine the formation constants by competition method by reacting the in situ generated complexes like [Zn(DFC–TS)] and [Zn2(DFC–TS)] with Na2H2EDTA and equilibrium competition constants (K′f1 and K′f2) were calculated from the plots of (Amax − A)/Amax as a function of H2EDTA2− concentration by adopting displacement model. The evaluated apparent formation constants are: K′f1 = (2.28 ± 0.32) × 105 M−1 and K′f2 = (1.64 ± 0.17) × 105 M−1 and corresponding formation constants Kf1 and Kf2 were calculated from the relation Kfi = K′EDTA/K′fi where K′EDTA = KEDTA × α4 = 2.55 × 1013 and α4 = K1K2K3K4/([H+]4 + K1[H+]3 + K1K2[H+]2 + K1K2K3[H+] + K1K2K3K4) = 7.98 × 10−4 at pH 7.20 with K1 = 1.02 × 10−2, K2 = 2.14 × 10−3; K3 = 6.92 × 10−7 and K4 = 5.50 × 10−11 and KZn-EDTA = 3.2 × 1016.31 So the calculated values are Kfi = 1.55 × 108 and Kf2 = 1.11 × 108. The apparent formation constant values (K′f1 = (2.28 ± 0.32) × 105 M−1 and K′f2 = (1.64 ± 0.17) × 105 M−1) are found to be very close to the values obtained by non-linear fitting of absorption data as a function of [Zn2+] (Fig. S12†).
The composition of the complex was determined by Job's method and it was revealed that an overall composition is 2
:
1 with respect to the Zn2+ ion.
We have also spectroscopically determined the acid dissociation constants of the free ligand (DFC–TS) and its Zn2+ complex with slightly excess over two equivalents of Zn2+ ions by monitoring the absorption of free ligand at 430 nm as a function of pH spanning between 2.0 and 12.0 using the eqn (2)
| A = (AAH [H+] + AA−Ka)/(Ka + [H+]),32,33 | (2) |
:
1 DMSO–water, v/v) compared to the free 4-methylphenol (19.1 and 10.2 in DMSO and pure water respectively).35
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Fig. 2 Determination of acid dissociation constant of (a) DFC–TS (free) and (b) DFC–TS in presence of 2.1 equivalents of Zn2+ in 9 : 1 DMSO–water (v/v) at 25 °C. | ||
The emission spectra of DFC–TS and its fluorescence titration with Zn2+ were recorded in DMSO–H2O (9
:
1, v/v, pH 7.20, HEPES buffer) (Fig. 3) at λex = 390 nm. The binding between the free DFC–TS and Zn2+ leads to chelation enhanced fluorescence (CHEF) effect causing ∼17 fold fluorescence intensity enhancement due to increased structural rigidity of the formed complexes (Fig. 3).36 On excitation at 390 nm, the isosbestic point in absorption spectra, there is gradual increase in fluorescence intensity (FI) at λem = 500 nm, with the increase in [Zn2+] upto 1
:
1 mole ratio, after that on increasing [Zn2+] there is a blue shift in λem from 500 to 490 nm (Fig. 3). This observation clearly indicates the stepwise uptake of Zn2+ ions in the ligand framework. The linear dependence of FI as function of [Zn2+] upto 1
:
1 mole ratio was analyzed with the help of eqn (1) in the form y = a + b × c × x, under the conditions 1 ≫ c × x and n = 1. It is interesting to note that linear least-squares analysis of fluorescence titration data gives K′f (7.17 ± 0.20) × 104 M−1. In addition, at λex = 430 nm there is a gradual blue shift of λem from 520 nm for pure ligand to 500 nm on complexation with Zn2+ and may be a consequence of slight involvement of Intramolecular Charge Transfer (ICT).37 It is interesting to note that non-linear least-squares analysis of fluorescence titration data gives K′f (1.14 ± 0.47) × 105 M−1 and n = (1.03 ± 0.04) and it is obvious that on gradual addition of Zn2+ fluorescence intensity at λem 500 nm increases and gets saturated at ∼DFC–TS
:
Zn2+ = 1
:
1 when exited at 430 nm (Fig. S13†). On further addition of Zn2+ there is no visible increase/decrease in fluorescence intensity.
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Fig. 3 Fluorescence titration of DFC–TS (20 μM) with Zn2+ (0–48 μM) in DMSO–H2O (9 : 1, v/v, pH 7.20, 10 mM HEPES buffer), λex = 390 nm, R2 = 0.99. | ||
Again, when we added Na2H2EDTA to an in situ generated [Zn(DFC–TS)] (1
:
1 L
:
M) and [Zn2(DFC–TS)] (1
:
2 L
:
M) complexes the observations are same as in case of absorption titration i.e. there is a gradual decrease in absorbance with the increase in Na2H2EDTA concentration (Fig. 4 and S14†). However, here the phase separation (2
:
1 and 1
:
1 complexes) is quite distinct thereby facilitating the determination of Kf1 and Kf2 unambiguously which were evaluated to be Kf1 = 1.03 × 108 and Kf2 = 0.92 × 108. These values are in good agreement to those obtained by absorption titration data.
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Fig. 4 (a) Plot of FI as a function of [Na2H2EDTA ] for the competitive displacement of Zn2+ from [Zn2(DFC–TS)] ensemble (20 μM with respect to DFC–TS) by Na2H2EDTA (0–44 μM) in DMSO-H2O (9 : 1, v/v) at pH 7.2 (HEPES buffer) and (b) non-linear fitting of data using eqn (1). | ||
The stoichiometries of the Zn2+ complexes of DFC–TS as delineated by UV-VIS and fluorescence titrations were further confirmed by ESI-MS+ (m/z) mass spectrometry. The prominent ESI-MS+ peak of the pure ligand at 311.1094, 316.0230 and 333.0256 corresponds to [DFC–TS + H+], [DFC–TS + Li+] and, [DFC–TS + Na+], respectively. The mass spectrum of the isolated [Zn(DFC–TS)]+ complex at m/z = 372.9884 corresponds to [Zn(DFC–TS)]+ indicating a 1
:
1 complexation in the initial stage. However the presence of a very small peak for 1
:
2 complex [Zn2(DFC–TS)(OAc)(H2O)]+ in solution is also apparent (Fig. S8†). When we prepared the solid product by reacting DFC–TS and Zn2+ in 1
:
2 mole ratio the a prominent ESI-MS+ peak appears at 514.9107 (m/z) that indicating the presence of complex species [Zn2(DFC–TS)(OAc)(H2O)]+ in solution. However no peaks appear for 1
:
1 complex.
The coordination modes were further supported by 1H-NMR studies. 1H-NMR peaks appear at 7.68, 8.31 and 11.45 ppm, correspond to azomethine proton (a), aromatic proton (b) and phenolic proton (c) and also peaks at 8.07 and 8.16 correspond to NH2 proton. The appearance of two separate peaks for NH2 proton may be due to the presence of two NH2 groups in two different chemical environments. The appearance of OH proton signal at >10.0 ppm signifies the presence of H-bonding. This peak intensity decreases significantly for [Zn(DFC–TS)]+ (1) and vanishes completely in case of dinuclear complex (2) indicating that phenolate group in DFC–TS participates in complexation with Zn2+ but in solution there is certain extent of free ligand in the case of complex 1. The 1H-NMR peak of azomethine proton (a) shifted to high field region (lower ppm, 6.93 for complex 1 and 7.31 for complex 2) reflecting the fact that the azomethine nitrogen participated in complexation. The aromatic protons remain almost invariant in the three species. Similar is the case for methyl proton. The coordination through sulphur atom to the Zn2+ is confirmed by IR spectra, where free ligand gives IR strectching frequency centered at 1110 cm−1 for C
S bond (normal range 1050–1200 cm−1) (Fig. 5) which on complexation splits into two peaks appearing at 1110 and 1090 cm−1. The shifting to smaller frequency clearly points out the lowering in electron density around the C–S bond and corresponds to the existence of thiolate ion.
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| Fig. 5 IR spectra of DFC–TS ligand (shown in black), (Zn–DFC–TS) complex (shown in green), (Zn2–DFC–TS) complex (shown in red) in solid KBr-pellets. | ||
The detection of Zn2+ was not perturbed by biologically abundant Na+, K+, Ca2+, Mg2+, Al3+ etc. metal ions. Several transition metal ions, namely Cr3+, Mn2+, Fe2+, Fe3+, Co2+, Ni2+, Cu2+, and heavy metal ions like Cd2+, Pb2+, and Hg2+, also caused no interference (Fig. 6). The sensor was found to bind Zn2+ reversibly as tested by reacting with excess EDTA in intra-cellular conditions and also with EDTA in extra-cellular conditions. Moreover, no significant change in emission spectra was observed even on excess addition of the above mentioned interfering metal ions.
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| Fig. 6 Fluorescence and histogram plots to indicate the selectivity of DFC–TS toward Zn2+ over other biologically relevant metal ions, λex = 430 nm. | ||
For practical application, the appropriate pH conditions for successful operation of the sensor were evaluated. The probe DFC–TS fluoresces rather very weakly between pH 2 and 8 while Zn–DFC–TS complexes fluoresce extensively between pH 5 and 8 in 10 mM HEPES buffer, clearly indicating that this pH range is suitable for fluorescence studies for the complexation with Zn2+ (Fig. 7). The fluorescence of free ligand DFC–TS increases enormously beyond pH 10.0 and may be due to the acid dissociation of the thioamide proton.
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Fig. 7 pH depence of FI of the free ligand, DFC–TS and [Zn2(DFC–TS)]+ with DFC–TS : Zn = 1 : 2.15 in 10 mM HEPES buffer in 9 : 1 DMSO : H2O (v/v) solvent system, λex = 430 nm. | ||
The intracellular Zn2+ imaging behaviour of DFC–TS was studied on HepG2 cells with the aid of fluorescence microscopy which displayed intensive fluorescence when cells pre-incubated with DFC–TS were exposed to Zn2+ ion (10.0 μM), (Fig. 8) which, however, strongly suppressed when Na2H2EDTA (100 μM) was added (Fig. 8). Therefore, DFC–TS renders a confirmatory evidence of the intracellular monitoring of Zn2+ without interference by biologically abundant other metal ions. We have also determined quantum yields of the ligand, [Zn2(DFC–TS)] complex, which showed higher quantum yield for Zn2+complex (0.143) than the pure ligand (0.0074).
We have also optimized the geometry of complex 1 as an anionic species where sulphide (S−) from C–SH (enolic form) coordinates to the metal center, other coordinating atoms remain unchanged. It is to be mentioned here that neutral species is more stable than the anionic species as indicated by the HOMO → LUMO energy gap (Fig. 10). The complex 2 is a dinuclear neutral species where one DFC–TS with N2S2O donor set of atoms and 4 oxygen atoms from two acetate groups involved in bonding. The phenoxo-O atom acts as a bridge between two metal centers along with two bridging acetate groups to hold the Zn2+ atoms firmly resulting distorted TBP geometries around them. The idea of such geometry as a dinuclear complex comes from our previous structural studies with analogous ligand. The bond distances and bond angles (Table S1 and S2 in ESI†) around the metal center(s) are very similar to those found in analogous complexes. In 1 and 2 all the calculated Zn–N/Zn–O distances fall in the range 2.054–2.319 Å and comparable to the reported values in the analogous complexes.36,38
Time dependent density functional theory (TDDFT)23–25 with B3LYP density functional was applied to study the low-lying excited states of the complex in DMSO using the optimized geometry of the ground (S0) state. The vertical excitation energies of the lowest 20 singlet states are also computed here. The UV-Vis spectra computed from TDDFT calculations in DMSO show two important peaks in the range 250–600 nm (see Fig. S6 and S7†) for DFC–TS. For complex 1, the band around 370 nm is dominated by the HOMO → LUMO excitations, while the band around ∼320 nm is mainly due to HOMO−1 → LUMO, HOMO−1 → LUMO+1 and HOMO → LUMO+1 transition. The corresponding experimental absorption bands appear at 370 nm and 317 nm respectively. In case of [Zn(DFC–TS)(OAc)] the absorption band around ∼420 nm is dominated by the HOMO → LUMO excitations, while the band around ∼340 nm it is mainly due to HOMO−1 → LUMO, and HOMO → LUMO+1 transitions. The absorption band at ∼300 nm arises mainly due to HOMO−3 → LUMO transition. The corresponding experimental absorption bands appear at 430 nm and 300 nm. Similarly, in case of [Zn2(DFC–TS)(OAc)2] the absorption bands at∼ 420 nm is dominated by the HOMO → LUMO excitations, while the band around ∼340 nm is mainly due toHOMO−1 → LUMO, and HOMO → LUMO+1 transitions. The TDDFT calculation on the mono- and dinuclear complexes reveal that there is no basic differences in the pattern of absorptions spectra of these species which is also evidenced from the experimental spectra where the λmax (absorption) remains almost unaltered for these two species but absorption continues to increase on adding Zn2+ beyond 1
:
1 mole ration, until it gets saturated at 2
:
1 mole ratio with respect to Zn2+. The details of the vertical excitation energies, oscillator strengths, and nature of excitations are shown in Table S3 (ESI†). HOMO–LUMO diagrams of all the optimized species along with the energy gaps are depicted in Fig. 10.
A list of 2,6-diformyl-p-cresol based Schiff base ligands36,39–43 that showed Zn2+ sensing is given in Scheme 3.
A quick inspection of these studies reveal that all these are turn on Zn2+ sensor with moderate LOD and find application towards intracellular Zn2+ monitoring.36,39–43
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c5ra25653d |
| This journal is © The Royal Society of Chemistry 2016 |