Xiaoding Lou‡
ab,
Chris Wai Tung Leung‡b,
Chao Donga,
Yuning Hongb,
Sijie Chenb,
Engui Zhaob,
Jacky Wing Yip Lamb and
Ben Zhong Tang*bcd
aKey Laboratory for Large-Format Battery Materials and System, Ministry of Education, School of Chemistry and Chemical Engineering, Huazhong University of Science and Technology, Wuhan 430074, China
bDepartment of Chemistry, Institute for Advanced Study, Division of Biomedical Engineering, Division of Life Science, State Key Laboratory of Molecular Neuroscience, and Institute of Molecular Functional Materials, The Hong Kong University of Science and Technology (HKUST), Clear Water Bay, Kowloon, Hong Kong, China. E-mail: tangbenz@ust.hk
cGuangdong Innovative Research Team, SCUT-HKUST Joint Research Laboratory, State Key Laboratory of Luminescent Materials and Devices, South China University of Technology, Guangzhou 510640, China
dHKUST Shenzhen Research Institute, Nanshan, Shenzhen 518057, China
First published on 16th July 2014
In this work, tetraphenylethene (TPE) equipped with thymine, TPE–T, was synthesized and used as a fluorescence biosensor for differentiating ssDNA from dsDNA. TPE–T is a “turn-on” fluorescence probe once it forms hydrogen bonds with single-stranded adenine-containing oligonucleotides with high sensitivity and specificity. The working mechanism of TPE–T and its potential in cell imaging are investigated in detail.
On the other hand, fluorescent probes of detecting single-stranded DNA (ssDNA) are still scarce compared to a huge number of dsDNA probe. We have previously discovered a group of fluorogens which are nonemissive when molecularly dissolved but highly fluorescent when aggregate are potentially used as ssDNA fluorescence probes.26 We coined this phenomenon as aggregation-induced emission (AIE) with the mechanism of the restriction of intramolecular rotations (RIR).27 In the past decade, the AIE fluorogens have been successfully employed in a variety of biological applications28 such as DNA sensing (G-quadruplex, dsDNA), protein sensing (Human serum albumin, insulin, Caspase-3/7, Acetylcholinesterase), small molecule sensing (cysteine, glucose), and long-term cell tracking etc. The fluorescence signals of AIE fluorogens will be turned on upon the binding to biomacromolecules by RIR.29
TPE–T is soluble and thus non-emissive in ethanol. The fluorescence spectrum exhibits as nearly a flat line parallel to the abscissa when the volume fraction of water (fw) is lower than 60% (Fig. S4†). When a large amount of water is added, the resulting mixture becomes intensely luminescent with blue emission peaked at 450 nm. The emission intensity of TPE–T in the solution with fw of 99% is about 400 times higher than that in pure ethanol. This characteristic curve shown in Fig. 1B indicates that TPE–T is a typical AIE active fluorogen with an fw threshold of 68%, above which the dye molecules aggregate and the emission is turned on. Solution of TPE–T in ethanol–water mixture with fw of 64% was then used as a detection medium.
Using this detection system, dsDNA and ssDNA differentiation was investigated, and the sequences of ssDNA are listed in Table 1. In order to check the stability of dsDNA, UV-vis spectra has been conducted. Fig. S5† showed the UV-vis spectra of calf thymus DNA (30 μg mL−1) in ethanol–water mixture (36:
64, v/v) at different incubation time. It was found that calf thymus DNA was stable in the test system for at least 60 minutes, which is sufficient for our detection. The fluorescence signals of TPE–T to dsDNA and ssDNA in the detection medium were shown in Fig. 1A. The solution of TPE–T in pure ethanol is almost non-emissive. The presence of adenine-containing ssDNA (AA) triggers the fluorescence of the dye whereas dsDNA (calf thymus DNA) cannot turn on the fluorescence of TPE–T in the detection medium. Increasing the concentration of dsDNA gave similar experimental results (Fig. S6†). Formations of hydrogen bond between TPE–T and adenine induce the RIR of the phenyl groups thus lead to the enhancement of the fluorescence. To verify this hypothesis, Hoechst 33342, a conventional nucleic acid dye, was chosen for evaluation by staining DNA through groove binding. Since the groove does not exist in single-stranded DNA, the fluorescence of Hoechst 33342 cannot be turned on. Different from TPE–T, Hoechst 33342 exhibits fluorescence enhancement in the presence of dsDNA rather than ssDNA (Fig. S7†), which implies that TPE–T is not a groove binder of DNA.
Abbreviation | Sequence |
---|---|
AA | 5′AAAAAAAAAAAAAAAAAAAAA3′ |
TT | 5′TTTTTTTTTTTTTTTTTTTTT3′ |
CC | 5′CCCCCCCCCCCCCCCCCCCCC3′ |
GG | 5′GGGGGGGGGGGGGGGGGGGGGG3′ |
AT | 5′ATATATATATATATATATATA3′ |
AC | 5′ACACACACACACACACACACA3′ |
AG | 5′AGAGAGAGAGAGAGAGAGAGA3′ |
TC | 5′TCTCTCTCTCTCTCTCTCTCT3′ |
TG | 5′TGTGTGTGTGTGTGTGTGTGT3′ |
A2T | 5′ATTATATTATATTATATTATA3′ |
A4T | 5′ATTTTATTTTATTTTATTTTA3′ |
A9T | 5′ATTTTTTTTTATTTTTTTTTA3′ |
R1 | 5′AATCCGTCGAGCAGAGTT3′ |
R2 | 5′GGC ATG AAC CGG AGT CCC ATC CTC3′ |
R3 | 5′AAT TTC ATA TTG GCT TCA ATC CAA AAT3′ |
To investigate the fluorescence response of TPE–T toward ssDNA, titration experiments were performed by adding different sequences of ssDNA into solution of TPE–T in ethanol–water mixture (36:
64, v/v; 10 μM) (Fig. S8–16†). In the presence of AA, an emission peak with a maximum at 450 nm appears as a result of TPE–T can form hydrogen bond with adenine causing the RIR of the phenyl groups. There were detectable fluorescent signals observed at concentrations of AA as low as 100 nM, and the fluorescence intensity increased with increasing AA concentration (Fig. 1B). In the AA concentration ranged of 1.3–1.9 μM, the plot of fluorescence increment at 450 nm as a function of AA concentration was in a linear regression with a correlation coefficient of 0.9928. Beside sensitivity, the specificity of TPE–T towards adenine-rich ssDNA was also investigated. As shown in Fig. 2, nearly no change was observed when adding the ssDNA without adenine, even at the ssDNA concentrations of 2 μM. At such a high ssDNA concentration, the emission intensity of TPE–T increased nearly 40-fold with the aid of adenine-rich ssDNA (AT, AC, AG), which demonstrated that it has high specificity to adenine-containing ssDNA.
In addition, the control experiments were carried out by using solutions of nucleobase-containing molecules, such as dTTP, dATP, dCTP, dGTP. As shown in Fig. S17–20,† even at the high concentration of 20 μM, the emission intensity exhibited very weak signals. The signals from the mixtures of TPE–T with dTTP, dCTP and dGTP were match to the hypothesis due to the absence of hydrogen bond formation. Interestingly, weak fluorescence signals were given even TPE–T was mixed with adenine-containing species. It shows that TPE–T could not detect the presence of adenine solely by the formation of hydrogen bond as dATP was too small to trigger RIR. To obtain more evidence, six ssDNA with different sequences were studied (Fig. S8, 9, 14, 21–23†). Among these, from TT, A9T, A4T, A2T, AT, to AA, the percentage of adenine increased gradually. As shown in Fig. 3B, the emission intensity of TPE–T remains almost unchanged in the presence of TT but increases along with the increase of the percentage of adenine in different ssDNA. These results proved that the restriction of intramolecular rotation of the phenyl groups on TPE–T is crucial for this detection system.
When 2 μM of AA was added in this detection system, the emission intensity enhanced about 25-fold, almost the same as in the case with AT as shown in Fig. 3A. The binding stoichiometry of TPE–T with AA and AT were then determined for rationalizing this similarity. Binding analysis was performed using the method of continuous variations (Job plot) as shown in Fig. S24.† Take AT as an example, the total concentration of TPE–T and AT was kept constant at 10.0 μM. A maximum and constant relative intensity occurs at [AT]/([AT] + [TPE–T]) = 0.1, which establishes the formation of a 1:
9 complex of AT and TPE–T and is responsible for the observed fluorescence signals. These data indicate that the formation of the complex, and the binding stoichiometry agrees well with the known adenine–thymine base pair. Interestingly, the plots of AA with TPE–T was also peaked at 0.1, giving a 1
:
9 binding ratio for AA to TPE–T. Since the presence of the steric hindrance between TPE–T bound ssDNA, no significant signal enhancement difference was observed between TPE–T and AA or AT.
To study whether the TPE–T based fluorescent probe developed here was applicable to real systems, three random ssDNA sequences (R1, R2, R3) were analyzed using our detecting system (Table 1). The experimental results showed that this sensing system can also sense the random ssDNA. Take a random ssDNA (R2) as an example, a linear correlation existed between the fluorescence intensity and the concentration of R2 within the range from 0 to 2.0 × 10−6 M (Fig. 4). The TPE–T bound to R2 through hydrogen bond indeed shows a distinct difference in fluorescence emission intensity, which exhibits more than 4-fold higher brightness than the TPE–T probe alone. The change in fluorescence emission intensity (I/I0) in three random ssDNA sequences (R1 = 3.4; R2 = 4.3; R3 = 5.6) is in accordance with our previous studies, which further proved that such a sensing system still worked well in real systems.
In addition to this, we have also explored the biological applications of TPE–T. We found that TPE–T can work as a fluorescent visualizer for intracellular imaging. As depicted in Fig. S25,† TPE–T selectively stained the cytoplasmic regions of living HeLa cells. Bright blue fluorescence was observed from the fixed HeLa cells, presumably because the dead HeLa cells with compromised membrane open the access for the dye molecules to enter the protoplasm, which represents an indicator of cell death.
Footnotes |
† Electronic supplementary information (ESI) available: Details of the experimental procedure; UV-vis spectra 1H NMR spectra; mass spectra. See DOI: 10.1039/c4ra05765a |
‡ These authors contributed equally to this work. |
This journal is © The Royal Society of Chemistry 2014 |