Author Affiliations
Abstract
1 Department of Gastroenterology, The First Hospital of Jilin University, Changchun 130021, P. R. China
2 Department of Urology, The First Hospital of Jilin University, Changchun 130021 P. R. China
3 Department of Biomedical Engineering, School of Basic Medical Sciences, Central South University, Changsha 410013, P. R. China
Photodynamic therapy (PDT) is a new and rapidly developing treatment modality for clinical cancer therapy. Semiconductor polymer dots (Pdots) doped with photosensitizers have been successfully applied to PDT, and have made progress in the field of tumor therapy. However, the problems of severe photosensitivity and limited tissue penetration depth are needed to be solved during the implementation process of PDT. Here we developed the Pdots doped with photosensitizer molecule Chlorin e6 (Ce6) and photochromic molecule 1,2-bis(2,4-dimethyl-5-phenyl-3-thiophene)-3,3,4,5-hexafluoro-1-cyclopentene (BTE) to construct a photoswitchable nanoplatform for PDT. The Ce6-BTE-doped Pdots were in the green region, and the tissue penetration depth was increased compared with most Pdots in the blue region. The reversible conversion of BTE under different light irradiation was utilized to regulate the photodynamic effect and solve the problem of photosensitivity. The prepared Ce6-BTE-doped Pdots had small size, excellent optical property, efficient ROS generation and good photoswitchable ability. The cellular uptake, cytotoxicity, and photodynamic effect of the Pdots were detected in human colon tumor cells. The experiments in vitro indicated that Ce6-BTE-doped Pdots could exert excellent photodynamic effect in ON state and reduce photosensitivity in OFF state. These results demonstrated that this nanoplatform holds the potential to be used in clinical PDT.Photodynamic therapy (PDT) is a new and rapidly developing treatment modality for clinical cancer therapy. Semiconductor polymer dots (Pdots) doped with photosensitizers have been successfully applied to PDT, and have made progress in the field of tumor therapy. However, the problems of severe photosensitivity and limited tissue penetration depth are needed to be solved during the implementation process of PDT. Here we developed the Pdots doped with photosensitizer molecule Chlorin e6 (Ce6) and photochromic molecule 1,2-bis(2,4-dimethyl-5-phenyl-3-thiophene)-3,3,4,5-hexafluoro-1-cyclopentene (BTE) to construct a photoswitchable nanoplatform for PDT. The Ce6-BTE-doped Pdots were in the green region, and the tissue penetration depth was increased compared with most Pdots in the blue region. The reversible conversion of BTE under different light irradiation was utilized to regulate the photodynamic effect and solve the problem of photosensitivity. The prepared Ce6-BTE-doped Pdots had small size, excellent optical property, efficient ROS generation and good photoswitchable ability. The cellular uptake, cytotoxicity, and photodynamic effect of the Pdots were detected in human colon tumor cells. The experiments in vitro indicated that Ce6-BTE-doped Pdots could exert excellent photodynamic effect in ON state and reduce photosensitivity in OFF state. These results demonstrated that this nanoplatform holds the potential to be used in clinical PDT.
Photodynamic therapy semiconductor polymer dots photosensitizer tumor therapy 
Journal of Innovative Optical Health Sciences
2022, 15(6): 2240007
Huan Wang 1,2,3Lu Guo 1,2,3Wu Zhao 1,2,3Guangcan Chen 1,2,3[ ... ]Lingjuan Zhao 1,2,3
Author Affiliations
Abstract
1 Key Laboratory of Semiconductor Materials Science, Institute of Semiconductors, Chinese Academy of Sciences, Beijing 100083, China
2 Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing 100049, China
3 Beijing Key Laboratory of Low Dimensional Semiconductor Materials and Devices, Beijing 100083, China
We report a distributed-Bragg-reflectors-based 4 × 40 GHz mode-locked laser diode (MLLD) array monolithically integrated with a multimode interference (MMI) combiner. The laser produces 2.98 ps pulses with a time-bandwidth product of 0.39. The peak wavelength of the MLLD array can be tuned by 8.4 nm while maintaining a good mode-locked state. The four mode-locked channels could work simultaneously with the peak wavelength interval around 3 nm.
140.5960 Semiconductor lasers 140.4050 Mode-locked lasers 
Chinese Optics Letters
2019, 17(11): 111402
Author Affiliations
Abstract
1 Key Laboratory of Semiconductor Materials Science, Institute of Semiconductors, Chinese Academy of Science, Beijing 100083, China
2 Tsinghua National Laboratory for Information Science and Technology, State Key Laboratory of Integrated Optoelectronics, Department of Electronic Engineering, Tsinghua University, Beijing 100084, China
We experimentally demonstrate all-optical clock recovery for 100 Gb/s return-to-zero on–off keying signals based on a monolithic dual-mode distributed Bragg reflector (DBR) laser, which can realize both mode spacing and wavelength tuning. By using a coherent injection locking scheme, a 100 GHz optical clock can be recovered with a timing jitter of 530 fs, which is derived by an optical sampling oscilloscope from both the phase noise and the power fluctuation. Furthermore, for degraded injection signals with an optical signal-to-noise ratio as low as 4.1 dB and a 25 km long distance transmission, good-quality optical clocks are all successfully recovered.
070.6020 Continuous optical signal processing 140.3520 Lasers, injection-locked 
Chinese Optics Letters
2016, 14(3): 030604
Author Affiliations
Abstract
Key Laboratory of Semiconductor Materials Science, Institute of Semiconductors, Chinese Academy of Sciences, Beijing 100086, China
We report a direct, modulated bandwidth enhancement in a amplified feedback laser (AFL), both experimentally and numerically. By means of fabricated devices, an enhanced 3 dB bandwidth of 27 GHz with an in-band flatness of ±3 dB is experimentally confirmed at 13 °C. It is numerically confirmed that the modulated bandwidth of the AFL can be enhanced to two times its original bandwidth, with more controlled flexibility to realize a flat, small-signal response.
140.5960 Semiconductor lasers 130.3120 Integrated optics devices 060.4510 Optical communications 
Chinese Optics Letters
2015, 13(5): 051401
作者单位
摘要
中国科学院半导体研究所 材料重点实验室,北京 100086
报道并制备一种脊波导结构的大功率1.5 μm分布反馈(DFB)激光器。为了获取最大的激光器出光功率,采用上下限制层非对称的波导结构。通过模拟仿真发现,当下限制层选择为450 nm时,该激光器具有最小的内部损耗系数,同时还能保证一阶模(m=1)在量子阱区具有最小的限制因子。实际制备的管芯的损耗系数为9.78 cm-1,这与仿真中计算的损耗系数9.3 cm-1较为符合。600 mA直流电流下,制备的法布里-帕罗(F-P)腔激光器最大功率大于114 mW;255 mA直流电流下,制备的单波长DFB激光器具有45 dB的边模抑制比,40 mW输出功率,和小于400 kHz的光谱线宽。
激光器 分布反馈激光器 高功率 非对称波导盖层 
中国激光
2015, 42(s1): s102012
作者单位
摘要
上海大学 精密机械工程系,上海200072
数字全息拼接技术旨在实现较大物体的检测或在同样的测量面积下获得更高的空间分辨力,实现方法是采集被测物体多个子孔径的数字全息图,且保持相邻子孔径之间有一定的重叠区。分别精密再现各个子孔径的数字全息图,然后将各孔径的位相信息进行拼接,以获得全孔径的位相分布。分别处理了反射型分辨力板(子孔径数为2×4)和透射性微透镜阵列(子孔径数为4×4)两个样本的全息图,并给出了消除测量光束和参考光束非等光程所引入的误差的方法。
数字全息技术 位相拼接 误差抑制 digital holography phase stitching error restraining 
光学仪器
2011, 33(4): 55

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