Yinghui
Wang
ab,
Yanqi
Huang
c,
Bin
Li
*a,
Liming
Zhang
a,
Hang
Song
a,
Hong
Jiang
a and
Jie
Gao
a
aKey Laboratory of Excited State Processes, Changchun Institute of Optics, Fine Mechanics and Physics, Chinese Academy of Sciences, Changchun, 130033, P. R. China
bGraduate School of the Chinese Academy of Sciences, Chinese Academy of Sciences, Beijing, 100039, P. R. China
cSchool of Materials Science and Engineering, Shandong University, Jinan, 250061, P. R. China. E-mail: lib020@nenu.edu.cn; Fax: +86-431-86176935
First published on 27th September 2011
A novel fluorescent chemosensor based on rhodamine derivative (Rh1) has been designed and synthesized for detection of Hg2+ ions, which exhibits high sensitivity and selectivity over other metal ions in aqueous solution and living cells. Moreover, this “Off–On”-type fluorescent sensor could successfully mimic a molecular level keypad lock in the presence of Cu2+ ions. Stimulated by the two chemical inputs (Hg2+ and Cu2+), Rh1 undergoes transformation of the structure between spirocyclic and ring-opened spirocyclic, which results in the change of fluorescence. Significantly, the outputs of the system depend on not only the proper combination but also on the correct order of the input signals, which is the most important feature of the keypad lock system. Only a specific sequence of inputs, i.e. the correct password, results in strong fluorescence emission at 555 nm which can be used to “open” this molecular keypad lock. Therefore, this molecular keypad lock has the potential for application in security devices, which could be used to authorize a user, to verify authentication of a product, or to initiate a higher process.
To mimic various electronic devices, numerous chemical systems responding to a large variety of activating input signals (e.g., light, electrical, magnetic, and chemical) have been developed.1k,6 Among these chemical systems, the most important one is fluorescent chemosensors with high selectivity and sensitivity for a specific analyte, such as heavy metal ions, anions, and pH. In particular, a fluorescent chemosensor for heavy metal ions not only can be used to detect the presence of the heavy metal ions (such as Hg2+ ions) in aqueous solution and living cells, but also to integrate these heavy metal ions as chemical-driven molecular machines in future molecular computing. Therefore, there is an urgent need to develop innovative and convenient fluorescent chemosensors for heavy metal ions (such as Hg2+ ions) because of the dual important application of a single molecule.
For fluorescent chemosensors, suitable fluorescence indicators that are sensitive to heavy metal ions (such as Hg2+ ions) concentrations and exhibit changes in fluorescence intensity have been used as molecular recognition materials. Among the numerous indicators, rhodamine derivatives are an excellent candidate due to their high fluorescence sensitivity to heavy metal ions, in addition to the excellent spectroscopic properties of large molar extinction coefficients, high fluorescence quantum yields and visible wavelength excitation. They can change their geometric structures among two states as a result of stimuli. Typically, in the absence of metal ions, the molecules prefer their spirolactam ring-closed geometry,7 which shows little absorption and fluorescence, whereas upon the addition of specific metal ions, the chelation or reaction of metal ions with sensor molecules will simultaneously open the spirolactam ring, which gives rise to a strong fluorescence emission.8 Simultaneously, they display a strong color development against the colorless blank during the sensing event, which is an important feature that would facilitate “naked-eye” detection. Therefore, many molecular switches and logic gates using rhodamine derivatives as indicator have been proposed.9 However, up to now, there has been no report on molecular keypad locks based on rhodamine derivatives as far as we know.
Herein, we intend to report the synthesis and characterization of a novel fluorescent chemosensor to detect Hg2+ both in aqueous solution and in living cells with rhodamine derivative 1 (Rh1) as fluorescent indicator. Moreover, Rh1 has been identified to respond as On and Off state of fluorescence depending upon the sequence of addition of Hg2+ and Cu2+ ions into the solution. Based on this property, a molecular keypad lock based on rhodamine derivative Rh1 was constructed whose fluorescence is in the On state in response to a specific sequence of chemical inputs (Hg2+ and Cu2+ ions).
Scheme 1 Synthesis procedure of Rh1. |
As mentioned above, we speculated the S, N, O binding sites might be sensitive towards the Hg2+ ion, thus we tested the effect of Hg2+ ions on the fluorescence behavior of Rh1. The fluorescence spectra were recorded upon excitation at 500 nm at room temperature with the gradual addition of small amounts of Hg2+ ions (0–10 equiv, 0–100 μM) into Rh1 solution, and shown in Fig. 1a. In the absence of Hg2+, as expected, the Rh1 solution exhibited very weak fluorescence in the range from 510 nm to 650 nm. Upon the addition of increasing concentrations of Hg2+, a new emission band peaking at 555 nm appeared and developed, which can be ascribed to the delocalized xanthene moiety of rhodamine group.12 The fluorescence response of Rh1 to other metal ions under the same condition was also investigated. As illustrated in Fig. 1b, no significant spectral changes of Rh1 were observed in the presence of K+, Na+, Ca2+, Mg2+, Ba2+, Zn2+, Cd2+, Cu2+ and Pb2+ (1 mM), indicating that Rh1 could recognize Hg2+ from other metal ions even those that exist in high concentrations.
Fig. 1 (a) Emission spectra of Rh1 (10 μM) in the presence of increasing concentration of Hg2+ in buffered (NaAc-HAc, pH = 7) water/CH3CN (1:1, v/v). λex = 500 nm. (b) Normalized fluorescence response I/I0 of Rh1 (10 μM) in the presence of various metal ions (1 × 10−3 M). λex = 500 nm and λem = 555 nm. Inset shows fluorescence change upon addition of Hg2+, Zn2+, Cd2+, Cu2+ , Pb2+ and blank (5 equiv). (c) Job's plot for determining the stoichiometry of Rh1 and Hg2+ ions (the total concentration of Rh1 and Hg2+ ions was 10 μM). |
To understand the recognition abilities of Rh1 towards Hg2+ ions, a Job's plot analysis was conducted to determine the binding stoichiometry of the Rh1-Hg2+ complex, by maintaining the total Rh1 and Hg2+ ions constant (10 μM) and changing the mole fraction of Hg2+ from 0 to 1. From the Job's plot shown in Fig. 1c, we can observe that the significant increase in fluorescence intensity of Rh1 resulted from the complexation with Hg2+. The fluorescence intensity went through a maximum at a molar fraction of about 0.5 of Hg2+, indicating that a 1:1 stoichiometry was the most possible one for the binding mode of Hg2+ and Rh1.
The association constant for Rh1 binding to Hg2+ was determined from the absorption titration data. Upon gradual addition of Hg2+ into the solution, a new absorption peaking around 527 nm emerged with increasing intensity which corresponds to the appearance of a pink color, suggesting the formation of the ring-opened tautomer of Rh1 upon Hg2+ binding (Fig. 2a and b). Since Rh1 binds with Hg2+ to form a complex with a complexing ratio of 1:1, the equilibrium can thus be described as follows:
Fig. 2 (a) Absorption spectra of Rh1 (10 μM) in the presence of increasing concentration of Hg2+ in buffered (NaAc-HAc, pH = 7) water/CH3CN (1:1, v/v). (b) Color changes of Rh1 (10 μM) upon addition of different amounts of Hg2+. (c) Absorbance as a function of [Hg2+] calculated from eqn (3): ■, data points experimentally obtained. |
(1) |
(2) |
(3) |
From the above discussion, it is apparent that the absorbance of Rh1 has a distinct functional relationship with the Hg2+ concentration, and the association constant Ks, which provides the basis for the detection of the Ks value. The fitted curve to incorporate experimental data for Hg2+ is presented in Fig. 2c, which gave an association constant Ks value of 8.42 × 104 M−1 for Rh1 binding to Hg2+. The strong binding ability of Rh1 towards Hg2+ could be ascribed to the introduction of the S atom.
In view of the good sensing performances of Rh1 to Hg2+ in aqueous solution, fluorescence imaging experiments were carried out in living cells on a Olympus fluorescence microscope to further demonstrate the practical applicability of Rh1 in living cells. As shown in Fig. 3b, after staining Rat Schwann cells with Rh1 (10 μM) for 10 min, they displayed no detectable fluorescence signal in living cells. Upon addition of 50 μM Hg2+ ions, the fluorescence intensity increases dramatically to show a clear red intracellular fluorescence (Fig. 3d). The results indicate that Rh1 can provide a fluorescence enhancement with excellent cell-permeability and biocompatibility for tracing the Hg2+ ion in cells, specifically and rapidly. Therefore, Rh1 could be considered for application for in vitro imaging of Hg2+ ion in living cells and potentially in vivo.
Fig. 3 Fluorescence images of Hg2+ ions in Rat Schwann cells with Rh1 (10 μM). Bright-field transmission image (a, c) and fluorescence image (b, d) of Rat Schwann cells incubated with 0 μM and 50 μM of Hg2+ ions for 30 min, respectively (excited with green light). |
In the experiment of testing the selectivity of Rh1, an interesting phenomenon attracted our attentions. There was no obvious color change in the presence of interfering effect metal ions, such as K+, Na+, Ca2+, Mg2+, Ba2+, Zn2+, Cd2+, and Pb2+ as shown in Fig. 4. However, the solution of Rh1 exhibits an obvious pink color with the addition of Cu2+, thus almost no fluorescence change is observed (insert in Fig 1b). Therefore, we investigated the detailed response of Rh1 to Cu2+ ion.
Fig. 4 Change in color of Rh1 (10 μM) in buffered (NaAc-HAc, pH = 7) water/CH3CN (1:1, v/v) with metal ions: blank, K+, Na+, Ca2+, Mg2+, Ba2+, Zn2+, Cd2+, Cu2+ and Pb2+ (1 × 10−3 M, from left to right). |
Unlike the varying tendency of fluorescence emission, upon addition of small amounts of Cu2+, the absorbance was significantly enhanced with a new peak appearing at 527 nm (Fig. 5a), whereas the absorption spectra of free Rh1 exhibited only a very weak band above 500 nm, which was ascribed to the spirolactam form of Rh1. Upon the addition of 5 equiv of Cu2+, the new peak was enhanced up to log ε = 5.25, accompanied with an obvious color change from colorless to pink simultaneously (Fig. 5b). The Job's plot analysis in Fig. 5c was conducted to determine the binding stoichiometry of the Rh1-Cu2+ complex. It was observed that a maximum absorption was reached when the molar fraction of Cu2+ ions was about 0.5, confirming that a 1:1 stoichiometry is most possible for the binding mode of Cu2+ and Rh1. The association constant for Rh1 binding to Cu2+ was also determined from the absorption titration data. Since Rh1 bound with Cu2+ to form a complex with a complexing ratio of 1:1, the data still can be fitted by eqn (3). Fig. 6 shows the fitted curve to incorporate the experimental data for Cu2+, which gives an association constant Ks value of 1.98 × 104 M−1 for Rh1 binding to Cu2+. Upon addition of small amounts Cu2+, the enhancement in absorbance clearly suggested the formation of the delocalized xanthane moiety of the rhodamine group, along with a distinct color change from colorless to pink. However, the fluorescence of the open-ring form of Rh1 was quenched by Cu2+, which could be explained based on the well-known paramagnetic effect of the Cu(II) d9 system.14
Fig. 5 (a) Absorption spectra of Rh1 (10 μM) in the presence of increasing concentration of Cu2+ in buffered (NaAc-HAc, pH = 7) water/CH3CN (1:1, v/v). (b) Color changes of Rh1 (10 μM) upon addition of different amounts of Cu2+. (c) Job's plot for determining the stoichiometry of Rh1 and Cu2+ ions (the total concentration of Rh1 and Cu2+ ions was 10 μM). |
Fig. 6 Absorbance as a function of [Cu2+] calculated from eqn (3): ■, data points experimentally obtained. |
Since the Ks values of Rh1-Hg2+ and Rh1-Cu2+ are comparable, Hg2+ and Cu2+ would compete against each other to coordinate with Rh1 when they were coexist in a system, resulting in a transformation between Rh1-Hg2+ and Rh1-Cu2+ with fluorescence. Based on this, we investigated the different fluorescence state “ON and OFF” of Rh1 with changing the addition sequence, using Hg2+ (2 equiv.) and Cu2+ (10 equiv.) as inputs (Fig. 7). When the first input is Hg2+, the fluorescence emission at 555 nm significantly enhanced. Although the sequential addition of Cu2+ led to a relative decline of the fluorescence intensity, it was still in the “On” state. On reversal of the input sequence, i.e. for Cu2+ as the first input and Hg2+ as the second one, it caused the fluorescence intensity far below its initial maximum, i.e. “Off” state. The two input signals of Hg2+ and Cu2+ were defined as In 1 and In 2, respectively. These inputs can be encoded with binary digits applying positive logic conventions (off = 0, on = 1). If we regard fluorescence intensity of 75 as the threshold values, Output = 0 when its corresponding spectral value was lower than 75; Output = 1 when its corresponding spectral value was higher than 75.
Fig. 7 Fluorescence emission output of Rh1 with different input sequences: (1) Hg2+ as the first input followed by Cu2+ as the second one; (2) Cu2+ as the first input followed by Hg2+ as the second one. |
As discussed above, Fig. 8 presents the outputs in the fluorescence channel, obtained for different addition sequences. Only in input sequence of Hg2+ and Cu2+, the fluorescent intensity was higher than the threshold value (Output = 1), resulting in strong fluorescence. However, changing the sequence of the inputs, it could not initiate a strong fluorescence at 555 nm (Output = 0). Therefore, according to this sequence-dependent phenomenon, a molecular keypad lock was constructed.
Fig. 8 Fluorescence output resulting from different input sequences: (a) In 1 (Hg2+ first) and In 2 (Cu2+ second); b) In 2 (Cu2+ first) and In 1 (Hg2+ second). |
To simplify the input sequence as password of the molecular keypad lock, inputs Hg2+ and Cu2+ were designated as “K” and “E”, respectively. When the input signal “K” was added first and followed by “E”, the emission at 555 nm was in the “On” state, and it created a secret password “KEY” (Y defines On state). Inverting the addition sequence of inputs, i.e. the first input is “E” and the second input is “K”, gave an obvious fluorescence quenching (Off, designated as the character “N”). Thus, the wrong password “EKN” failed to open the lock. Therefore, only the authorized user who knows the exact password “KEY” can open the lock, which is a new approach for protecting information at the molecular scale (Fig. 9). Due to the fact that the use of numerical digits (0–9) and letters (A–Z) as PIN numbers in a two-digit password allows a total of more than 700 different combinations,5j it added to the complexity of cracking the keypad lock, and improved remarkably the security of the molecular device.
Fig. 9 Fluorescent keypad to access a secret password at 555 nm with different input sequences. |
This journal is © The Royal Society of Chemistry 2011 |