Center for Biomedical Photonics & College of Physics and Optoelectronic Engineering, Key Laboratory of Optoelectronic Devices and Systems of Ministry of Education and Guangdong Province, Shenzhen University, Shenzhen 518071, China
Prof. Dr. Wei Yan
Center for Biomedical Photonics & College of Physics and Optoelectronic Engineering, Key Laboratory of Optoelectronic Devices and Systems of Ministry of Education and Guangdong Province, Shenzhen University, Shenzhen 518071, China
Many kinds of nanoparticles and organic dyes as fluorescent probes have been used in the stimulated emission depletion (STED) nanoscopy. Due to high toxicity, photobleaching and non-water solubility, these fluorescent probes are hard to apply in living cell imaging. Here, we report a new fluorescence carbon dots (FNCDs) with high photoluminescence quantum yield (56%), low toxicity, anti-photobleaching and good water-solubility that suitable for live-cell imaging can be obtained by doping fluorine element. Moreover, the FNCDs can stain the nucleolus and tunneling nanotubes (TNTs) in the living cell. More importantly, for STED nanoscopy imaging, the FNCDs effectively depleted background signals and improved imaging resolution. Furthermore, the lateral resolution of single FNCDs size under the STED nanoscopy is up to 22.1 nm for FNCDs deposited on a glass slide was obtained. And because of their good water dispersibility, the higher resolution of single FNCDs size in the nucleolus of a living cell can be up to 19.7 nm. After the image optimization steps, the fine fluorescence images of TNTs diameter with ca. 75 nm resolution is obtained living cell, yielding a threefold enhancement compared with that in confocal imaging. Additionally, the FNCDs show excellent photobleaching resistance after 1,000 scan cycles in the STED model. All results show that FNCDs have significant potential for application in STED nanoscopy.
Super-resolution optical imaging is crucial to the study of cellular processes. Current super-resolution fluorescence microscopy is restricted by the need of special fluorophores or sophisticated optical systems, or long acquisition and computational times. In this work, we present a deep-learning-based super-resolution technique of confocal microscopy. We devise a two-channel attention network (TCAN), which takes advantage of both spatial representations and frequency contents to learn a more precise mapping from low-resolution images to high-resolution ones. This scheme is robust against changes in the pixel size and the imaging setup, enabling the optimal model to generalize to different fluorescence microscopy modalities unseen in the training set. Our algorithm is validated on diverse biological structures and dual-color confocal images of actin-microtubules, improving the resolution from ~ 230 nm to ~ 110 nm. Last but not least, we demonstrate live-cell super-resolution imaging by revealing the detailed structures and dynamic instability of microtubules.
Flexible organic materials that exhibit dynamic ultralong room temperature phosphorescence (DURTP) via photoactivation have attracted increasing research interest for their fascinating functions of reversibly writing-reading-erasing graphic information in the form of a long afterglow. However, due to the existence of a nonnegligible activation threshold for the initial exposure dose, the display mode of these materials has thus far been limited to binary patterns. By resorting to halogen element doping of carbon dots (CDs) to enhance intersystem crossing and reduce the activation threshold, we were able to produce, for the first time, a transparent, flexible, and fully programmable DURTP composite film with a reliable grayscale display capacity. Examples of promising applications in UV photography and highly confidential steganography were constructed, partially demonstrating the broad future applications of this material as a programmable platform with a high optical information density.
Stimulated emission depletion (STED) microscopy is a powerful super-resolution microscopy technique that has achieved significant results in breaking the resolution limit and relevant applications. In principle, STED super resolution is obtained by stimulated emission partially inhibiting the spontaneous emission in the periphery of a diffraction-limited area. However, very high depletion laser power is generally necessary for the enhancement of imaging resolution, which is harmful to live biological specimens due to its high phototoxicity and photo-bleaching effects. Therefore, further improving the STED resolution at a lower depletion power level has recently attracted increasing interest from researchers in various fields. In this work, a phasor plot approach combined with fluorescence lifetime imaging microscopy (FLIM) is used to resolve the abovementioned problem based on a long- and short-lifetime criterion. Firstly, the time-resolved data obtained by STED-FLIM is converted to the frequency domain via a phasor approach. Next, partial data is extracted according to the information on the phase and amplitude for resolution improvement. Then, fluorescent microspheres (100 nm in diameter) are observed under different depletion powers, resulting in a series of improved resolution through phasor plots. Finally, this method is applied to image human Nup153 in fixed HeLa cells, providing a 86 nm higher resolution than that in traditional STED imaging at a depletion power of 20 mW.
Two probes, AIE-1 and AIE-2, were synthesized to investigate the effect of substitutional functional group on aggregation (aggregation-caused quenching (ACQ) or aggregation-induced emission (AIE)) and intramolecular charge transfer (ICT) behavior as well as on the cell imaging aspect. The yellow-color non-substituted probe AIE-1 showed weak charge-transfer absorption and an emission band at 377 nm and 432 nm, whereas the yellowish-orange color substituted probe AIE-2 showed a strong charge-transfer absorption and an emission band at 424 nm and 477 nm in THF solvent. The UV-Vis studies of AIE-1 and AIE-2 in THF and THF with different water fractions showed huge absorption changes in AIE-2 with high water fractions due to its strong aggregation behavior, but no such noticeable absorption changes were observed for AIE-1. Interestingly, the fluorescence intensity of AIE-1 at 432 nm gradually decreased with increasing water fractions and became almost non-emissive at 90% water. However, the monomer-type emission of AIE-2 at 477 nm was shifted to 584 nm with a 6-fold increase in fluorescence intensity in THF-H2O (1:9, v/v) solvent mixtures due to the restriction of intramolecular rotation on aggregation in high water fractions. This result indicates that the probe AIE-1 shows ACQ and probe AIE-2 shows AIE behaviors in THF-H2O solvent mixtures. Furthermore, the emission spectra of AIE-1 and AIE-2 were carried out in different solvent and with different concentrations to see the solvent- or concentration-dependent aggregation behavior. Scanning electron microscope (SEM) and dynamic light scattering (DLS) experiments were also conducted to assess the morphology and particle size of two probes before and after aggregation. Both of the probes, AIE-1 and AIE-2, showed less toxicity on HeLa cells and were suitable for cell imaging studies. Density functional theory (DFT) calculation was also carried out to confirm the ICT process from an electron-rich indole moiety to an electron-deficient cyano-phenyl ring of AIE-1 or AIE-2.