Author Affiliations
Abstract
1 Alferov University, Khlopina 8/3, St. Petersburg 194021, Russia
2 Department of Physics and Engineering, ITMO University, Lomonosova 9, St. Petersburg 197101, Russia
3 Institute of Automation and Control Processes (IACP), Far Eastern Branch of Russian Academy of Sciences, Ulitsa Radio 5, Vladivostok 690041, Primorsky Krai, Russia
4 Peter the Great St. Petersburg Polytechnic University, Polytechnicheskaya 29, St. Petersburg 195251, Russia
5 Skolkovo Institute of Science and Technology, Nobel 3, Moscow 121205, Russia
6 Qingdao Innovation and Development Center, Harbin Engineering University, Qingdao 266000, China
Halide perovskite light-emitting electrochemical cells are a novel type of the perovskite optoelectronic devices that differs from the perovskite light-emitting diodes by a simple monolayered architecture. Here, we develop a perovskite electrochemical cell both for light emission and detection, where the active layer consists of a composite material made of halide perovskite microcrystals, polymer support matrix, and added mobile ions. The perovskite electrochemical cell of CsPbBr3:PEO:LiTFSI composition, emitting light at the wavelength of 523 nm, yields the luminance more than 7000 cd/m2 and electroluminescence efficiency of 1.3×105 lm/W. The device fabricated on a silicon substrate with transparent single-walled carbon nanotube film as a top contact exhibits 40% lower Joule heating compared to the perovskite optoelectronic devices fabricated on conventional ITO/glass substrates. Moreover, the device operates as a photodetector with a sensitivity up to 0.75 A/W, specific detectivity of 8.56×1011 Jones, and linear dynamic range of 48 dB. The technological potential of such a device is proven by demonstration of 24-pixel indicator display as well as by successful device miniaturization by creation of electroluminescent images with the smallest features less than 50 μm.
composite inorganic halide perovskite silicon single walled carbon nanotubes light-emitting electrochemical cell photodetector indicator display 
Opto-Electronic Advances
2023, 6(9): 220154
作者单位
摘要
上海交通大学电子信息与电气工程学院 薄膜与微细技术教育部重点实验室, 上海200240
利用半导体性单壁碳纳米管(SWCNT)的高吸收系数、优异的光电特性和高载流子迁移率等特点,本文构筑了基于半导体SWCNT(sc-SWCNT)/富勒烯(C60)异质结的透明全碳宽光谱的场效应晶体管光电探测器。该器件的大部分结构均由碳基材料组成,全碳异质结作为导电沟道材料,金属性SWCNT作为源漏电极,氧化石墨烯(GO)作为介质层,在可见光波段的透光率均高于80%。电学测试结果表明:该光电探测器表现出了较强的栅控能力,实现了从405~1064 nm的可见光-近红外宽光谱响应,在5 mW/cm2的940 nm激光照射下,该器件光电响应率可以达到18.55 A/W,比探测率达到5.35×1011 Jones,同时,表现出了优异的循环稳定性。
单壁碳纳米管 富勒烯 全碳异质结 高透明度 场效应晶体管光电探测器 single-walled carbon nanotubes Fullerene all-carbon heterojunctions high transparency field-effect transistor photodetector 
中国光学
2023, 16(5): 1243
陈文彬 1冯吉军 1,*廖洋 2夏新成 1[ ... ]赵新洛 3,**
作者单位
摘要
1 上海理工大学光电信息与计算机工程学院上海市现代光学系统重点实验室,上海 200093
2 中国科学院上海光学精密机械研究所强场激光物理国家重点实验室,上海 201800
3 上海大学低维碳与器件物理研究所物理系,上海 200444
利用重复频率为1 kHz的钛蓝宝石飞秒激光烧蚀悬浮在甲醇中的单壁碳纳米管制备碳炔。利用表面增强拉曼光谱仪和紫外可见吸收光谱仪对样品溶液进行光谱表征,并用高效液相色谱仪对样品进行分离,确认有碳炔(CnH2n=6,8,10,12,14,16)生成,其中的主要产物是C8H2。对制备碳炔的最佳激光功率与最佳加工时间进行了研究,结果显示:当激光单脉冲能量为0.52 mJ、加工时间为1.5 h时,可以获得最高的碳炔产率。对碳炔的合成机制进行了较深入的解释。激光功率密度存在饱和阈值,该饱和阈值与C2自由基的碎裂程度有关,激光功率密度超过饱和阈值后会打破C2自由的“反向” 第四键,进而影响C2自由基合成碳炔。因此,随着激光单脉冲能量增大,碳炔的产率呈现先增加后降低的现象。本研究可为碳炔的大规模制备提供重要参考。
激光技术 碳炔 飞秒激光烧蚀 激光功率密度饱和阈值 单壁碳纳米管 
中国激光
2023, 50(20): 2002404
作者单位
摘要
1 上海科技大学 物质科学与技术学院, 上海 201210
2 中国科学院苏州纳米技术与纳米仿生研究所 先进材料部, 江苏 苏州 215123
半导体型单壁碳纳米管在分散与分离过程中长度会被截短。在100nm以下的超短管的存在会增加管间搭接电阻和载流子的散射几率, 从而导致器件性能的下降。开发了一种有机体系的硅胶吸附技术。利用硅胶颗粒表面的硅羟基与包裹在碳纳米管表面的聚合物PCz中的N原子形成氢键, 成功实现了超短碳管的高效去除, 使半导体型碳纳米管的长度分布实现了有效调控。基于长度分选后的碳纳米管制备的晶体管器件, 其开态电流和最大跨导达到8.9μA/μm和0.5mS/μm, 比长度未分选的器件分别提高了约300%和250%。
半导体型单壁碳纳米管 管长分选 高效吸附 semiconducting single-walled carbon nanotubes length sorting efficient absorption 
半导体光电
2022, 43(4): 786
作者单位
摘要
1 上海交通大学 电子信息与电气工程学院 微纳电子学系薄膜与微细技术教育部重点实验室,上海 200240
2 上海航天技术研究院,上海 201109
3 上海空间电源研究所空间电源技术国家重点实验室,上海 200245
基于碳纳米材料/体半导体范德华(vdW)异质结的光电器件可以同时实现碳纳米材料的超高载流子迁移率以及体半导体的优异光电性能,且具有结构简单、工艺简便、易于调控界面等优点。尤其是通过调控单壁碳纳米管(SWCNT)的直径/手性、费米能级等可以与体半导体形成能带匹配、具有原子级界面的新型混合维度vdW异质结。本文报道了一种基于(6,5)手性为主的SWCNT薄膜与n型GaAs所形成的pn结的宽光谱自驱动光电探测器,并利用石墨烯降低SWCNT薄膜内载流子的复合几率和促进载流子传输。实验结果表明,器件对405~1064 nm波段光子表现出高灵敏的光电响应,零偏压条件下最大光电响应度和比探测率分别可达1.214 A/W和2×1012 Jones。
范德华异质结 单壁碳纳米管 砷化镓 自驱动光电探测器 van der Waals heterojunctions single-walled carbon nanotubes GaAs self-powered photodetectors 
中国光学
2022, 15(2): 373
Author Affiliations
Abstract
1 Max Born Institute for Nonlinear Optics and Short Pulse Spectroscopy, 12489Berlin, Germany
2 Jiangsu Key Laboratory of Advanced Laser Materials and Devices, School of Physics and Electronic Engineering, Jiangsu Normal University, Xuzhou221116, China
3 Institute of Chemical Materials, China Academy of Engineering Physics, Mianyang621900, China
4 Key Laboratory of Advanced Ceramics and Mechanical Technology of Ministry of Education, School of Materials Science and Engineering, Tianjin University, Tianjin300072, China
5 Department of Physics, Korea Advanced Institute of Science and Technology (KAIST), 34141Daejeon, Republic of Korea
6 Centre de Recherche sur les Ions, les Matériaux et la Photonique (CIMAP), UMR 6252 CEA-CNRS-ENSICAEN, Université de Caen, 14050 Caen Cedex 4, France
7 Física i Cristal·lografia de Materials i Nanomaterials (FiCMA-FiCNA), Universitat Rovira i Virgili (URV), 43007Tarragona, Spain
8 State Key Laboratory of Crystal Materials and Institute of Crystal Materials, Shandong University, Jinan250100, China
We report on a power-scalable sub-100-fs laser in the 2-μm spectral range using a Tm3+-doped ‘mixed’ (Lu,Sc)2O3 sesquioxide ceramic as an active medium. Pulses as short as 58 fs at 2076 nm with an average output power of 114 mW at a pulse repetition rate of approximately 82.9 MHz are generated by employing single-walled carbon nanotubes as a saturable absorber. A higher average power of 350 mW at 2075 nm is obtained at the expense of the pulse duration (65 fs). A maximum average power of 486 mW is achieved for a pulse duration of 98 fs and an optical conversion efficiency of 22.3%, representing the highest value ever reported from sub-100-fs mode-locked Tm lasers.
2-μm mode-locked laser single-walled carbon nanotubes Tm:2O3 
High Power Laser Science and Engineering
2021, 9(4): 04000e50
仲路铭 1,2寇天一 1,2袁帅 1,2彭滟 1冯吉军 1,2,*
作者单位
摘要
1 上海理工大学 上海市现代光学系统重点实验室,上海 200093
2 上海理工大学 光电信息与计算机工程学院,上海 200093
单壁碳纳米管是新一代透明导电材料,具有许多特殊的光学、电学和机械特性,在多种领域应用广泛。为此通过电弧法制备了单壁碳纳米管并进一步与有机玻璃(PMMA)管状波导集成,经实验和模拟研究了基于管状波导的单壁碳纳米管太赫兹透射光谱特性。研究结果表明,单壁碳纳米管可以使管状波导的太赫兹共振增强,可有效提高共振消光比,而石墨烯和炭黑对管状波导的太赫兹透射光谱几乎没有影响。
太赫兹光谱 单壁碳纳米管 管状波导 THz spectroscopy single-walled carbon nanotubes tube waveguide 
光学仪器
2020, 42(4): 56
郑苗苗 1,2,*李亚辉 2姚建 2邱松 2[ ... ]李清文 1,2
作者单位
摘要
1 上海科技大学 物质科学与技术学院, 上海 201210
2 中国科学院苏州纳米技术与纳米仿生研究所 先进材料研究部, 江苏 苏州 215123
高纯度的单手性单壁碳纳米管对于下一代碳基电子器件的发展具有重要意义。利用聚[(9, 9-二辛基芴-2, 7-二基)-共-联吡啶](PFO-BPy)、聚(9,9-二辛基芴-2,7-二基)(PFO)和聚(9,9-二辛基芴-共苯并噻二唑)(PFO-BT)三种聚合物在有机相中分别分选出(6,5), (7,5)和(10,5)三种手性单壁碳纳米管, 具有较高纯度以及浓度, 并去除了超过99%的残留分散剂。使用上述溶液沉积获得高均匀性和高密度的碳纳米管薄膜, 以此作为器件沟道材料, 制备了手性单壁碳纳米管场效应晶体管阵列。结果显示, 大直径的(10,5)手性碳纳米管晶体管器件具有较好的电学性能, 其迁移率最高达16cm2?V-1?s-1, 开关比达107。
单壁碳纳米管 手性分离 碳纳米管薄膜 场效应晶体管器件 single-walled carbon nanotubes chiral separation carbon nanotube films field effect transistor 
半导体光电
2020, 41(3): 344
崔丹丹 1,2石玉娇 1,2,*
作者单位
摘要
1 华南师范大学 a.生物光子学研究院
2 b.激光生命科学研究所教育部重点实验室, 广州 510631
传统光声成像外源对比剂的光吸收主要集中在可见光区和传统近红外区(NIR, 750~900 nm), 开发具有更高光学组织穿透能力的近红外二区(NIR-II, 1 000~1 700 nm)光吸收外源对比剂对活体深层组织光声成像具有重要意义。本文中, 作者选取了光吸收峰在1 000 nm左右的半导体型单壁碳纳米管为近红外二区光学吸收外源对比剂, 测试了其在近红外二区激光激发下能够产生较强的光声效应。进一步地, 作者通过将该纳米材料包埋在仿体组织的不同深度的位置, 获得了仿体组织的深层光声成像, 成像深度可达1.5 cm。试验结果表明, 具有近红外二区光吸收能力的半导体型单壁碳纳米管在活体深层组织光声成像中有很大的应用潜力。
半导体型单壁碳纳米管 近红外二区 光声成像 semiconductor single-walled carbon nanotubes near infrared region photoacousticimaging 
激光生物学报
2019, 28(5): 463
Author Affiliations
Abstract
1 Biophotonics Research Laboratory Center for Interdisciplinary Biomedical Education and Research University of Central Oklahoma, Edmond, Oklahoma 73034, USA
2 Department of Oncology The First Affiliated Hospital of Chinese PLA General Hospital, Fucheng Road 51 Beijing, P. R. China
3 University of Oklahoma Health Sciences Center 940 Stanton. L.Young Blvd., BMSB Rm.513 Oklahoma City Oklahoma 73104, USA
4 SouthWest Nano Technologies, Norman, Oklahoma 73071, USA
The ideal treatment modality for metastatic cancer would be a local treatment that can destroy primary tumors while inducing an effective systemic anti-tumor response. To this end, we developed laser immunotherapy, combining photothermal laser application with an immunoadjuvant for the treatment of metastatic cancer. Additionally, to enhance the selective photothermal effect, we integrated light-absorbing nanomaterials into this innovative treatment. Specifically, we developed an immunologically modified carbon nanotube combining single-walled carbon nanotubes (SWNTs) with the immunoadjuvant glycated chitosan (GC). To determine the effectiveness of laser irradiation, a series of experiments were performed using two different irradiation durations — 5 and 10 min. Rats were inoculated with DMBA-4 cancer cells, a metastatic cancer cell line. The treatment group of rats receiving laser irradiation for 10 min had a 50% longterm survival rate without residual primary or metastatic tumors. The treatment group of rats receiving laser irradiation for 5 min had no long-term survivors; all rats died with multiple metastases at several distant sites. Therefore, LasertSWNT–GC treatment with 10 min of laser irradiation proved to be effective at reducing tumor size and inducing long-term anti-tumor immunity.
Anti-tumor immune response laser immunotherapy single-walled carbon nanotubes glycated chitosan laser irradiation 
Journal of Innovative Optical Health Sciences
2015, 8(4): 1550036

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