Fiber-optic sensing technology has the advantages of passivity, anti-electromagnetic interference, long-distance measurement, high sensitivity and high accuracy, small size, and adaptability to harsh environments such as high-vacuum, high-pressure, and strong magnetic fields compared with the traditional electrical sensing technology. However, with the increasing application requirements, how to further improve the sensitivity of fiber-optic sensors, extend the detection limit and improve the maintenance-free capability has become one of the core issues of the current research. This paper reviews the principle, preparation, and application of fiber-optic microstructured sensing based on abrupt field type. It specifically outlines the development and applications of micro-nano optical fibers, photonic crystal optical fibers, optical fiber gratings and structured optical fibers, and lists the main preparation methods of two types of micro-nano optical fibers from the basic theory of optical fiber microstructured sensor devices.
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中国科学院光电技术研究所主办
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The advent of artificial intelligence (AI) has propelled augmented reality (AR) display technology to a pivotal juncture, positioning it as a contender for the next generation of mobile intelligent terminals. However, the pursuit of advanced AR displays, particularly those capable of delivering immersive 3D experiences, is significantly hindered by the performance limitations of current hardware and the complexity of system integration. In this study, we present an innovative multi-focal plane AR display system that integrates a non-orthogonal polarization-multiplexing metasurface, freeform optical elements, and an OLED display screen. All optical elements are integrated into a single solid-state architecture, based on a joint optimization design approach of ray tracing and diffraction theory. The multi-focal plane AR visual effect is realized by the compact and multiplexing metasurface, which performs distinct phase functions across diverse polarization channels. Meanwhile, freeform surfaces offer ample design flexibility for the collaborative optimization of multi-focal plane imaging and the see-through systems. Followed by a mechanical design and prototype assembly, we demonstrate the system's capabilities in real-time and multi-focal plane display. The digital images at all virtual image distances seamlessly integrate with the real environment, fully exhibiting the system's high parallelism and real-time interactivity. With the innovative design concept and joint design method, we believe that our work will spur more innovative and compact intelligent solutions for AR displays and inject new vitality into hybrid optical systems.
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中国科学院光电技术研究所主办
中国科协“中国科技期刊卓越行动计划高起点期刊”项目支持
CiteScore 19.2
聚焦重大科学问题背后的基础科学
打造光电基础科学的专业学术交流平台
主要方向包括但不限于：
• 发光原理 • 光场调控
• 新型光电材料 • 光与物质相互作用
• 非线性光学 • 量子光学
• 信息光学 • 生物光子学
• 激光光学 • 光伏原理
• 平面光学 • 机器学习
Launch in 2022, monthly
A high-quality, open access, peer reviewed research journal
CiteScore 19.2
Publishes reviews, research articles and letters
Reports the physical mechanisms and fundamental science of optics, photonics and optoelectronics
The scope includes，but is not limited to:
• Light-emitting principles • Light field manipulation
• New optoelectronic materials • Light-matter interactions
• Nonlinear optics • Quantum optics
• Information optics • Biophotonics
• Laser optics • Photovoltaic principles
• Flat optics • Machine learning
A catadioptric lens structure, also known as pancake lens, has been widely used in virtual reality (VR) displays to reduce the formfactor. However, the utilization of a half mirror (HM) to fold the optical path thrice leads to a significant optical loss. The theoretical maximum optical efficiency is merely 25%. To transcend this optical efficiency constraint while retaining the foldable characteristic inherent to traditional pancake optics, in this paper, we propose a theoretically lossless folded optical system to replace the HM with a nonreciprocal polarization rotator. In our feasibility demonstration experiment, we used a commercial Faraday rotator (FR) and reflective polarizers to replace the lossy HM. The theoretically predicted 100% efficiency can be achieved approximately by using two high-extinction-ratio reflective polarizers. In addition, we evaluated the ghost images using a micro-OLED panel in our imaging system. Indeed, the ghost images can be suppressed to undetectable level if the optics are with antireflection coating. Our novel pancake optical system holds great potential for revolutionizing next-generation VR displays with lightweight, compact formfactor, and low power consumption.
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","sort":0,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure1","type":"article","typesetSecTagId":"s01","viewNum":0},{"columnNums":2,"dataId":"65b35f2a99d881090c5a90e9","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2024/3/OEA-2023-0178WuShinTson-2.jpg","fileType":"fulltextFig","fileXMLPath":"OEA-2023-0178WuShinTson-2.jpg","id":"6cdc3f4e-ef57-4178-8533-8808fb9980ea","imgWidth":"17.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"2","nameEn":"Schematic of reciprocal and nonreciprocal polarization rotators. Polarization rotation in (a) a reciprocal polarization rotator during forward propagation and (b) backward propagation. Polarization rotation in (c) a nonreciprocal polarization rotator through forward propagation and (d) backward propagation.
","sort":1,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure2","type":"article","typesetSecTagId":"s02","viewNum":0},{"columnNums":2,"dataId":"65b35f2a99d881090c5a90e9","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2024/3/OEA-2023-0178WuShinTson-3.jpg","fileType":"fulltextFig","fileXMLPath":"OEA-2023-0178WuShinTson-3.jpg","id":"cdbb3e1a-bfdd-4904-9c38-7f5681287c09","imgWidth":"17.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"3","nameEn":"Working principle of the proposed novel pancake optics system. (a) Polarization conversion process in the proposed novel pancake optic system with a FR. (b) A possible configuration of the proposed novel pancake optics. (c) Polarization conversion process in the proposed novel pancake optic system without a FR.
","sort":2,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure3","type":"article","typesetSecTagId":"s02","viewNum":0},{"columnNums":1,"dataId":"65b35f2a99d881090c5a90e9","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2024/3/OEA-2023-0178WuShinTson-4.jpg","fileType":"fulltextFig","fileXMLPath":"OEA-2023-0178WuShinTson-4.jpg","id":"a888b77d-2859-42f2-8140-e43a1868a5b7","imgWidth":"8.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"4","nameEn":"Experiments using a laser source. The folded beams in pancake optics system (a) without FR, (b) with FR.
","sort":3,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure4","type":"article","typesetSecTagId":"s03","viewNum":0},{"columnNums":2,"dataId":"65b35f2a99d881090c5a90e9","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2024/3/OEA-2023-0178WuShinTson-5.jpg","fileType":"fulltextFig","fileXMLPath":"OEA-2023-0178WuShinTson-5.jpg","id":"ee31377b-bfec-4b7a-a512-0ef397412491","imgWidth":"17.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"5","nameEn":"Characterization of the FR in the novel pancake optics system. (a) Transmission spectrum of the FR. (b) Measurement setup for characterizing polarization rotation. LP stands for linear polarizer. (c) Measured and calculated normalized transmission spectra (zero means perfect polarization rotation) of the FR.
","sort":4,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure5","type":"article","typesetSecTagId":"s03","viewNum":0},{"columnNums":2,"dataId":"65b35f2a99d881090c5a90e9","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2024/3/OEA-2023-0178WuShinTson-6.jpg","fileType":"fulltextFig","fileXMLPath":"OEA-2023-0178WuShinTson-6.jpg","id":"7fbb345a-a497-451d-b2ab-22d9ae142987","imgWidth":"17.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"6","nameEn":"Experiments using a micro-OLED panel. (a) Original image. (b) 0th order folded image and (c) 1st order image in the pancake system without a FR. (d) 1st order image in the pancake system with a FR operating in 510-550 nm. (e) Original image. (f) 0th order folded image and (g) 1st order image in the pancake system without a FR. (h) 1st order image in the pancake system with a FR operating in 603–663 nm.
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","sort":-2,"supplementRemarkCn":"","supplementRemarkEn":"创刊于2018年
中国科学院光电技术研究所主办
中国科协“中国科技期刊国际影响力提升计划”D类项目支持
JCR影响因子22.4；CiteScore 26.8
探索全球光电科研热点的前沿创新
创造一个高端、专业的国际学术交流平台
主要方向包括但不限于：
• 光源和传感器 • 光电子学
• 纳米光子学 • 等离子体和超材料
• 光学成像 • 机器学习
• 先进光学材料
• 生物光子学和生物医学光学
• 非线性光学和超快光子学
• 光通信 • 光伏技术
微信公众号：光电期刊
推特：@OptoElectronAdv
Launch in March 2018, monthly
A high-quality, open access, peer reviewed research journal
JCR IF 22.4; CiteScore 26.8
Publishes top-quality original articles, letters and reviews
Focuses on the advances of the cutting edge innovations of optics, photonics and optoelectronics
The scope includes，but is not limited to:
• Light sources and sensors • Optoelectronics
• Nanophotonics • Plasmonics and metamaterials
• Optical imaging • Intelligent and digital optics
• Advanced optical materials
• Biophotonics and biomedical optics
• Nonlinear optics and ultrafast photonics
• Optical communications • Photovoltaics
Wechat: OE_Journal
Twitter: @OptoElectronAdv
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(a) Crystal structures of undoped and Sb3+-doped C10H22N6InCl7·H2O. (b) Photographs of C10H22N6In1-xSbxCl7·H2O under day light and UV light. (c) PLQY, (d) Normalized PLE and PL spectra, (e) PL decay curve, (f) Powder XRD patterns of C10H22N6In1-xSbxCl7·H2O. (g) XPS spectra of Sb 3d in C10H22N6In0.95Sb0.05Cl7·H2O. (h) XPS spectra of In 3d in pristine C10H22N6InCl7·H2O and C10H22N6In0.95Sb0.05Cl7·H2O.
","sort":0,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure1","type":"article","typesetSecTagId":"s03","viewNum":0},{"columnNums":2,"dataId":"65f0feaf99d881433ef827db","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2024/3/OEA-2023-0197Zangzhigang-2.jpg","fileType":"fulltextFig","fileXMLPath":"OEA-2023-0197Zangzhigang-2.jpg","id":"71614f41-4460-4841-b3fb-bf3344261e9d","imgWidth":"16.5cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"2","nameEn":"(a) PL of C10H22N6In0.95Sb0.05Cl7·H2O under different excitation wavelengths. (b) PL intensity of C10H22N6In0.95Sb0.05Cl7·H2O as a function of excitation powers. (c) PL spectra of C10H22N6In0.95Sb0.05Cl7·H2O under different temperatures. (d) Fitting curve between integrated PL intensity of C10H22N6In0.95Sb0.05Cl7·H2O and temperature. (e) The correlation between FWHM of the C10H22N6In0.95Sb0.05Cl7·H2O and temperature. (f) Schematic diagram of the photophysical processes.
","sort":1,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure2","type":"article","typesetSecTagId":"s03","viewNum":0},{"columnNums":2,"dataId":"65f0feaf99d881433ef827db","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2024/3/OEA-2023-0197Zangzhigang-3.jpg","fileType":"fulltextFig","fileXMLPath":"OEA-2023-0197Zangzhigang-3.jpg","id":"04f97c27-6e6d-438a-b97b-14d48092b3d1","imgWidth":"15.1cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"3","nameEn":"(a) Patterned images of C10H22N6In0.95Sb0.05Cl7·H2O and C10H22N6In0.95Sb0.05Cl7 under day light and UV light. Normalized PLE spectra and PL spectra of (b) C10H22N6In0.95Sb0.05Cl7·H2O and (c) C10H22N6In0.95Sb0.05Cl7. (d) PL decay curve of C10H22N6In0.95Sb0.05Cl7·H2O and C10H22N6In0.95Sb0.05Cl7. (e) The crystal structure of Sb3+-doped C10H22N6InCl7·H2O before and after heating. DFT electronic structures of (f) C10H22N6InCl7·H2O, (g) Sb3+-doped C10H22N6InCl7·H2O and (h) Sb3+-doped C10H22N6InCl7. Density of states of (i) C10H22N6InCl7·H2O, (j) Sb3+-doped C10H22N6InCl7·H2O and (k) Sb3+-doped C10H22N6InCl7.
","sort":2,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure3","type":"article","typesetSecTagId":"s03","viewNum":0},{"columnNums":2,"dataId":"65f0feaf99d881433ef827db","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2024/3/OEA-2023-0197Zangzhigang-4.jpg","fileType":"fulltextFig","fileXMLPath":"OEA-2023-0197Zangzhigang-4.jpg","id":"2a41f4bb-93bd-4e0c-852b-ebba65ed356e","imgWidth":"13.1cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"4","nameEn":"(a) Photographs of patterns composed of C10H22N6In0.95Sb0.05Cl7and C10H22N6In0.95Sb0.05Cl7@PMMA. (b) Information encryption process produced by C10H22N6In0.95Sb0.05Cl7·H2O and C10H22N6In0.95Sb0.05Cl7·H2O @PMMA. (c) Design of optical AND logical gate produced by C10H22N6In0.95Sb0.05Cl7·H2O and C10H22N6In0.95Sb0.05Cl7·H2O @PMMA. (d) The experimental demonstration of optical AND logical gate.
","sort":3,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure4","type":"article","typesetSecTagId":"s03","viewNum":0}],"filePath":"/fileOEJ/journal/article/gdjz/2024/3/","firstFig":{"dataId":"65f0feaf99d881433ef827db","fileFrom":"xml","fileLastName":"png","filePath":"/fileOEJ/journal/article/gdjz/2024/3/20230197.png","fileType":"firstFig","fileXMLPath":"20230197.png","id":"135a3ebd-8080-4d82-99da-940e88b42435","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"FIG. 3029.","nameCn":"FIG. 3029.","nameEn":"TOC
","sort":-2,"supplementRemarkCn":"","supplementRemarkEn":"创刊于2018年
中国科学院光电技术研究所主办
中国科协“中国科技期刊国际影响力提升计划”D类项目支持
JCR影响因子22.4；CiteScore 26.8
探索全球光电科研热点的前沿创新
创造一个高端、专业的国际学术交流平台
主要方向包括但不限于：
• 光源和传感器 • 光电子学
• 纳米光子学 • 等离子体和超材料
• 光学成像 • 机器学习
• 先进光学材料
• 生物光子学和生物医学光学
• 非线性光学和超快光子学
• 光通信 • 光伏技术
微信公众号：光电期刊
推特：@OptoElectronAdv
Launch in March 2018, monthly
A high-quality, open access, peer reviewed research journal
JCR IF 22.4; CiteScore 26.8
Publishes top-quality original articles, letters and reviews
Focuses on the advances of the cutting edge innovations of optics, photonics and optoelectronics
The scope includes，but is not limited to:
• Light sources and sensors • Optoelectronics
• Nanophotonics • Plasmonics and metamaterials
• Optical imaging • Intelligent and digital optics
• Advanced optical materials
• Biophotonics and biomedical optics
• Nonlinear optics and ultrafast photonics
• Optical communications • Photovoltaics
Wechat: OE_Journal
Twitter: @OptoElectronAdv
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","sort":-2,"supplementRemarkCn":"","supplementRemarkEn":"A highly sensitive light-induced thermoelectric spectroscopy (LITES) sensor based on a multi-pass cell (MPC) with dense spot pattern and a novel quartz tuning fork (QTF) with low resonance frequency is reported in this manuscript. An erbium-doped fiber amplifier (EDFA) was employed to amplify the output optical power so that the signal level was further enhanced. The optical path length (OPL) and the ratio of optical path length to volume (RLV) of the MPC is 37.7 m and 13.8 cm-2, respectively. A commercial QTF and a self-designed trapezoidal-tip QTF with low frequency of 9461.83 Hz were used as the detectors of the sensor, respectively. The target gas selected to test the performance of the system was acetylene (C2H2). When the optical power was constant at 1000 mW, the minimum detection limit (MDL) of the C2H2-LITES sensor can be achieved 48.3 ppb when using the commercial QTF and 24.6 ppb when using the trapezoidal-tip QTF. An improvement of the detection performance by a factor of 1.96 was achieved after replacing the commercial QTF with the trapezoidal-tip QTF.
","appendixList":[],"articleBusiness":{"articleId":"65d1b17a99d881090c5c7863","baiduIncludeResult":0,"baiduIncludeResultSearchNum":0,"baiduXueShuIncludeResult":0,"baiduXueShuIncludeResultSearchNum":0,"citeCount":0,"googleIncludeResult":0,"googleIncludeResultSearchNum":0,"htmlSource":1,"htmlViewCount":0,"id":"4477c2c6-481c-11f0-9a6d-c4c6e6f11e4a","isRegCstr":0,"isRegDOI":1,"isUpdate":"1","pdfDownCount":0,"pdfEnFileSizeInt":0,"pdfFileName":"OEA-2023-0230Mayufei.pdf","pdfFileSize":3335.06,"pdfFileSizeInt":3335,"viewCount":0},"articleNo":"OEA-2023-0230Mayufei","articleReleaseProgresses":[],"authors":[{"addressTagIds":"aff1,aff2","articleId":"65d1b17a99d881090c5c7863","authorNameCn":"","authorNameEn":"Yahui Liu","authorRoleType":"author","authorTagVal":"1,2","authorType":"org","corresper":false,"deceased":0,"givenNamesEn":"Yahui","id":"5f9d37f8-fd4f-4078-b0e7-fe11275f8ef6","sortNumber":1,"surNameEn":"Liu"},{"addressTagIds":"aff1,aff2","articleId":"65d1b17a99d881090c5c7863","authorNameCn":"","authorNameEn":"Shunda Qiao","authorRoleType":"author","authorTagVal":"1,2","authorType":"org","corresper":false,"deceased":0,"givenNamesEn":"Shunda","id":"05398e92-12bd-45e3-9b1a-cee91f851048","sortNumber":2,"surNameEn":"Qiao"},{"addressTagIds":"aff1,aff2","articleId":"65d1b17a99d881090c5c7863","authorNameCn":"","authorNameEn":"Chao Fang","authorRoleType":"author","authorTagVal":"1,2","authorType":"org","corresper":false,"deceased":0,"givenNamesEn":"Chao","id":"cf9b416f-ff97-47a6-800b-15d7531d0540","sortNumber":3,"surNameEn":"Fang"},{"addressTagIds":"aff1,aff2","articleId":"65d1b17a99d881090c5c7863","authorNameCn":"","authorNameEn":"Ying He","authorRoleType":"author","authorTagVal":"1,2","authorType":"org","corresper":false,"deceased":0,"givenNamesEn":"Ying","id":"aeda55af-c62a-403f-9949-981acef2fc1d","sortNumber":4,"surNameEn":"He"},{"addressTagIds":"aff1,aff2","articleId":"65d1b17a99d881090c5c7863","authorNameCn":"","authorNameEn":"Haiyue Sun","authorRoleType":"author","authorTagVal":"1,2","authorType":"org","corresper":false,"deceased":0,"givenNamesEn":"Haiyue","id":"458564bd-e88a-4f23-a8d5-14c6f3b87d12","sortNumber":5,"surNameEn":"Sun"},{"addressTagIds":"aff3","articleId":"65d1b17a99d881090c5c7863","authorNameCn":"","authorNameEn":"Jian Liu","authorRoleType":"author","authorTagVal":"3","authorType":"org","corresper":false,"deceased":0,"givenNamesEn":"Jian","id":"fe54ccf7-ed66-4e27-9ced-2d5a4ba627e1","sortNumber":6,"surNameEn":"Liu"},{"addressTagIds":"aff1,aff2","articleId":"65d1b17a99d881090c5c7863","authorNameCn":"","authorNameEn":"Yufei Ma","authorRoleType":"author","authorTagVal":"1,2","authorType":"org","corresper":true,"correspinfoEn":"YF Ma, E-mail: mayufei@hit.edu.cn","deceased":0,"email":"mayufei@hit.edu.cn","givenNamesEn":"Yufei","id":"9148bbf9-8406-48ec-a907-29f095f1b129","sortNumber":7,"surNameEn":"Ma"}],"categoryNameCn":"","categoryNameEn":"Article","citationCn":"","citationEn":"Liu YH, Qiao SD, Fang C et al. A highly sensitive LITES sensor based on a multi-pass cell with dense spot pattern and a novel quartz tuning fork with low frequency. Opto-Electron Adv 7, 230230 (2024). DOI: 10.29026/oea.2024.230230","doi":"10.29026/oea.2024.230230","figList":[{"columnNums":2,"dataId":"65d1b17a99d881090c5c7863","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2024/3/OEA-2023-0230Mayufei-1.jpg","fileType":"fulltextFig","fileXMLPath":"OEA-2023-0230Mayufei-1.jpg","id":"39674392-3421-4be9-b7f6-fe834ba5342d","imgWidth":"17.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"1","nameEn":"Structure parameter diagram of MPC and spot distribution on the surface of the incident mirror, where the green circle represents the location of the incident perforation. (a) Structure parameter diagram of MPC. (b) Simulation based on the established computational model. (c) Spot distribution obtained with a He-Ne laser.
","sort":0,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure1","type":"article","typesetSecTagId":"s02","viewNum":0},{"columnNums":2,"dataId":"65d1b17a99d881090c5c7863","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2024/3/OEA-2023-0230Mayufei-2.jpg","fileType":"fulltextFig","fileXMLPath":"OEA-2023-0230Mayufei-2.jpg","id":"ddefa878-0954-4fa7-a5dc-691ca9274802","imgWidth":"16.1cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"2","nameEn":"The features of two QTFs. (a) A photograph of the QTFs. (b) Frequency response of the commercial QTF (line in green) and the trapezoidal-tip QTF (line in red).
","sort":1,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure2","type":"article","typesetSecTagId":"s02","viewNum":0},{"columnNums":2,"dataId":"65d1b17a99d881090c5c7863","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2024/3/OEA-2023-0230Mayufei-3.jpg","fileType":"fulltextFig","fileXMLPath":"OEA-2023-0230Mayufei-3.jpg","id":"245ac21d-2f67-4863-95c3-b77a6d9a37c3","imgWidth":"15.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"3","nameEn":"Schematic configuration of LITES sensor based on a multi-pass cell with dense spot pattern.
","sort":2,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure3","type":"article","typesetSecTagId":"s02","viewNum":0},{"columnNums":2,"dataId":"65d1b17a99d881090c5c7863","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2024/3/OEA-2023-0230Mayufei-4.jpg","fileType":"fulltextFig","fileXMLPath":"OEA-2023-0230Mayufei-4.jpg","id":"db6a64b1-2d1f-4379-b3ff-aa54ee0590fa","imgWidth":"16.1cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"4","nameEn":"System characteristics at different optical powers. (a) Peak value of 2f signal of the commercial QTF based system. Inset: 2f signal waveform. (b) Peak value of 2f signal of the trapezoidal-tip QTF based system. Inset: 2f signal waveform. (c) Noise and SNR of the system when commercial QTF and trapezoidal-tip QTF were adopted, respectively.
","sort":3,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure4","type":"article","typesetSecTagId":"s03","viewNum":0},{"columnNums":2,"dataId":"65d1b17a99d881090c5c7863","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2024/3/OEA-2023-0230Mayufei-5.jpg","fileType":"fulltextFig","fileXMLPath":"OEA-2023-0230Mayufei-5.jpg","id":"9188b2c8-0f33-45e7-8eef-b12c9da048f0","imgWidth":"17.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"5","nameEn":"(a) 2f signal at different concentrations when commercial QTF was used. (b) 2f signal at different concentrations when trapezoidal-tip QTF was used. (c)The function relationship between different concentrations and the peak value of the 2f signals when commercial QTF was used. (d) The function relationship between different concentrations and the peak value of the 2f signals when trapezoidal-tip QTF was used.
","sort":4,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure5","type":"article","typesetSecTagId":"s03","viewNum":0},{"columnNums":1,"dataId":"65d1b17a99d881090c5c7863","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2024/3/OEA-2023-0230Mayufei-6.jpg","fileType":"fulltextFig","fileXMLPath":"OEA-2023-0230Mayufei-6.jpg","id":"7cb2ee7f-b422-48fd-b737-4f377c72af1d","imgWidth":"8.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"6","nameEn":"Background noise of the LITES sensor system when different QTFs were used as the detector.
","sort":5,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure6","type":"article","typesetSecTagId":"s03","viewNum":0},{"columnNums":2,"dataId":"65d1b17a99d881090c5c7863","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2024/3/OEA-2023-0230Mayufei-7.jpg","fileType":"fulltextFig","fileXMLPath":"OEA-2023-0230Mayufei-7.jpg","id":"57a8840e-6d8d-470a-aa23-59c4fa424f39","imgWidth":"16.2cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"7","nameEn":"Allan deviation analysis. (a) Allan deviation analysis for commercial QTF based C2H2-LITES sensor. (b) Allan deviation analysis for trapezoidal-tip QTF based C2H2-LITES sensor.
","sort":6,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure7","type":"article","typesetSecTagId":"s03","viewNum":0}],"filePath":"/fileOEJ/journal/article/gdjz/2024/3/","firstFig":{"dataId":"65d1b17a99d881090c5c7863","fileFrom":"xml","fileLastName":"png","filePath":"/fileOEJ/journal/article/gdjz/2024/3/230230.png","fileType":"firstFig","fileXMLPath":"230230.png","id":"9d05964d-9300-4bf4-934c-4692ab3e5bee","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"FIG. 2939.","nameCn":"FIG. 2939.","nameEn":"TOC
","sort":-2,"supplementRemarkCn":"","supplementRemarkEn":"创刊于2018年
中国科学院光电技术研究所主办
中国科协“中国科技期刊国际影响力提升计划”D类项目支持
JCR影响因子22.4；CiteScore 26.8
探索全球光电科研热点的前沿创新
创造一个高端、专业的国际学术交流平台
主要方向包括但不限于：
• 光源和传感器 • 光电子学
• 纳米光子学 • 等离子体和超材料
• 光学成像 • 机器学习
• 先进光学材料
• 生物光子学和生物医学光学
• 非线性光学和超快光子学
• 光通信 • 光伏技术
微信公众号：光电期刊
推特：@OptoElectronAdv
Launch in March 2018, monthly
A high-quality, open access, peer reviewed research journal
JCR IF 22.4; CiteScore 26.8
Publishes top-quality original articles, letters and reviews
Focuses on the advances of the cutting edge innovations of optics, photonics and optoelectronics
The scope includes，but is not limited to:
• Light sources and sensors • Optoelectronics
• Nanophotonics • Plasmonics and metamaterials
• Optical imaging • Intelligent and digital optics
• Advanced optical materials
• Biophotonics and biomedical optics
• Nonlinear optics and ultrafast photonics
• Optical communications • Photovoltaics
Wechat: OE_Journal
Twitter: @OptoElectronAdv
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","sort":-2,"supplementRemarkCn":"","supplementRemarkEn":"创刊于2018年
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Author Correction: ITO-free silicon-integrated perovskite electrochemical cell for light-emission and light-detection. Opto-Electron Adv 7, 220154C (2024). DOI: 10.29026/oea.2024.220154C","doi":"10.29026/oea.2024.220154C","figList":[],"filePath":"/fileOEJ/journal/article/gdjz/2024/3/","firstFig":{"dataId":"65f950ff99d881433ef8be9a","fileFrom":"xml","fileLastName":"png","filePath":"/fileOEJ/journal/article/gdjz/2024/3/Correction.png","fileType":"firstFig","fileXMLPath":"Correction.png","id":"e2c8d3c1-4d1d-42dc-9eb0-81d183817b98","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"FIG. 3036.","nameCn":"FIG. 3036.","nameEn":"TOC
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中国科学院光电技术研究所主办
中国科协“中国科技期刊国际影响力提升计划”D类项目支持
JCR影响因子22.4；CiteScore 26.8
探索全球光电科研热点的前沿创新
创造一个高端、专业的国际学术交流平台
主要方向包括但不限于：
• 光源和传感器 • 光电子学
• 纳米光子学 • 等离子体和超材料
• 光学成像 • 机器学习
• 先进光学材料
• 生物光子学和生物医学光学
• 非线性光学和超快光子学
• 光通信 • 光伏技术
微信公众号：光电期刊
推特：@OptoElectronAdv
Launch in March 2018, monthly
A high-quality, open access, peer reviewed research journal
JCR IF 22.4; CiteScore 26.8
Publishes top-quality original articles, letters and reviews
Focuses on the advances of the cutting edge innovations of optics, photonics and optoelectronics
The scope includes，but is not limited to:
• Light sources and sensors • Optoelectronics
• Nanophotonics • Plasmonics and metamaterials
• Optical imaging • Intelligent and digital optics
• Advanced optical materials
• Biophotonics and biomedical optics
• Nonlinear optics and ultrafast photonics
• Optical communications • Photovoltaics
Wechat: OE_Journal
Twitter: @OptoElectronAdv
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","sort":-2,"supplementRemarkCn":"","supplementRemarkEn":"The degree of coherence (DOC) function that characterizes the second-order correlations at any two points in a light field is shown to provide a new degree of freedom for carrying information. As a rule, the DOC varies along the beam propagation path, preventing from the efficient information recovery. In this paper, we report that when a partially coherent beam carrying a cross phase propagates in free space, in a paraxial optical system or in a turbulent medium, the modulus of the far-field (focal plane) DOC acquires the same value as it has in the source plane. This unique propagation feature is employed in a novel protocol for far-field imaging via the DOC, applicable to transmission in both free-space and turbulence. The advantages of the proposed approach are the confidentiality and resistance to turbulence, as well as the weaker requirement for the beam alignment accuracy. We demonstrate the feasibility and the robustness of the far-field imaging via the DOC in the turbulent media through both the experiment and the numerical simulations. Our findings have potential applications in optical imaging and remote sensing in natural environments, in the presence of optical turbulence.
","appendixList":[],"articleBusiness":{"articleId":"61adb11299d8812a099e4431","baiduIncludeResult":0,"baiduIncludeResultSearchNum":0,"baiduXueShuIncludeResult":0,"baiduXueShuIncludeResultSearchNum":0,"citeCount":0,"googleIncludeResult":0,"googleIncludeResultSearchNum":0,"htmlSource":1,"htmlViewCount":0,"id":"447e3617-481c-11f0-9a6d-c4c6e6f11e4a","isRegCstr":0,"isRegDOI":1,"isUpdate":"1","pdfDownCount":0,"pdfEnFileSizeInt":0,"pdfFileName":"oea-2021-0027-Caiyangjian.pdf","pdfFileSize":3345.0,"pdfFileSizeInt":3345,"viewCount":0},"articleNo":"oea-2021-0027-Caiyangjian","articleReleaseProgresses":[],"authors":[{"addressTagIds":"aff1,aff2","articleId":"61adb11299d8812a099e4431","authorNameCn":"","authorNameEn":"Yonglei Liu","authorRoleType":"author","authorTagVal":"1,2","authorType":"org","corresper":false,"deceased":0,"givenNamesEn":"Yonglei","id":"24eaf2cc-ca80-4939-ad1e-1d900d039088","sortNumber":1,"surNameEn":"Liu"},{"addressTagIds":"aff3","articleId":"61adb11299d8812a099e4431","authorNameCn":"","authorNameEn":"Yahong Chen","authorRoleType":"author","authorTagVal":"3","authorType":"org","corresper":false,"deceased":0,"email":"yahongchen@suda.edu.cn","givenNamesEn":"Yahong","id":"4c299aac-d52e-4cf6-bc0a-7957dc599e66","sortNumber":2,"surNameEn":"Chen"},{"addressTagIds":"aff3","articleId":"61adb11299d8812a099e4431","authorNameCn":"","authorNameEn":"Fei Wang","authorRoleType":"author","authorTagVal":"3","authorType":"org","corresper":true,"correspinfoEn":"F Wang, E-mail: fwang@suda.edu.cn","deceased":0,"email":"fwang@suda.edu.cn","givenNamesEn":"Fei","id":"2fb51b82-0f71-4337-a227-671bcf89130a","sortNumber":3,"surNameEn":"Wang"},{"addressTagIds":"aff1,aff2,aff3","articleId":"61adb11299d8812a099e4431","authorNameCn":"","authorNameEn":"Yangjian Cai","authorRoleType":"author","authorTagVal":"1,2,3","authorType":"org","corresper":true,"correspinfoEn":"YJ Cai, E-mail: yangjiancai@suda.edu.cn","deceased":0,"email":"yangjiancai@suda.edu.cn","givenNamesEn":"Yangjian","id":"6c0809d3-efd2-4c92-af1f-def6c9c35209","sortNumber":4,"surNameEn":"Cai"},{"addressTagIds":"aff1,aff2","articleId":"61adb11299d8812a099e4431","authorNameCn":"","authorNameEn":"Chunhao Liang","authorRoleType":"author","authorTagVal":"1,2","authorType":"org","corresper":true,"correspinfoEn":"CH Liang, E-mail: Cliang@dal.ca","deceased":0,"email":"Cliang@dal.ca","givenNamesEn":"Chunhao","id":"2414c84b-25be-4159-a54e-2f92b7fe1c3b","sortNumber":5,"surNameEn":"Liang"},{"addressTagIds":"aff4","articleId":"61adb11299d8812a099e4431","authorNameCn":"","authorNameEn":"Olga Korotkova","authorRoleType":"author","authorTagVal":"4","authorType":"org","corresper":false,"deceased":0,"givenNamesEn":"Olga","id":"9a1bfdab-6150-4e2a-b0f8-9dbbe3571969","sortNumber":6,"surNameEn":"Korotkova"}],"categoryNameEn":"Original Article","citationCn":"","citationEn":"Liu YL, Chen YH, Wang F, Cai YJ, Liang CH et al. Robust far-field imaging by spatial coherence engineering. Opto-Electron Adv 4, 210027 (2021). DOI: 10.29026/oea.2021.210027","doi":"10.29026/oea.2021.210027","figList":[{"columnNums":2,"dataId":"61adb11299d8812a099e4431","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2021/12/oea-2021-0027-Caiyangjian-1.jpg","fileType":"fulltextFig","fileXMLPath":"oea-2021-0027-Caiyangjian-1.jpg","id":"98d8e48e-955e-45c4-9739-e7cebaa267dd","imgWidth":"16.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"1","nameEn":"Variation of the modulus of DOC |μ| of a CGCSM beam with the propagation distance z after the focusing lens, with the CP strength factor (a1−a4) u = 0 mm−2, (b1−b4) u = 2 mm−2, (c1−c4) u = 10 mm−2, and (d1−d4) u = 70 mm−2. The parameters are set as λ = 532 nm, δ0 =0.5 mm and n=1.
","sort":0,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure1","type":"article","typesetSecTagId":"s02","viewNum":0},{"columnNums":2,"dataId":"61adb11299d8812a099e4431","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2021/12/oea-2021-0027-Caiyangjian-2.jpg","fileType":"fulltextFig","fileXMLPath":"oea-2021-0027-Caiyangjian-2.jpg","id":"34a5b477-f586-4253-99c6-79f51627dba0","imgWidth":"16.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"2","nameEn":"Theoretical results of the modulus of the DOC |μ| at different propagation distances z after the lens with the CP strength factor u=−60 mm−2. The inserted letter “S” in (a) is adopted as the power spectral density P(v) function.
","sort":1,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure2","type":"article","typesetSecTagId":"s02","viewNum":0},{"columnNums":2,"dataId":"61adb11299d8812a099e4431","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2021/12/oea-2021-0027-Caiyangjian-3.jpg","fileType":"fulltextFig","fileXMLPath":"oea-2021-0027-Caiyangjian-3.jpg","id":"cdefddc6-0712-4387-9797-ff21f0a81b71","imgWidth":"16.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"3","nameEn":"Schematic diagram of the experiment setup for generation of Schell-model beams with a controllable CP structure, measurement of the modulus of the DOC in the far field propagation in free space as well as in turbulent atmosphere. Laser, a Nd:YAG laser with wavelength 532nm; M, mirror; BE, beam expander; SLM1, SLM2, spatial light modulator; RGGD, rotating ground glass disk; L1, L2, L3, L4, L5, L6, thin lenses with the identical focal length f=250mm; GAF, Gaussian amplitude filter; BS, beam splitter; CA, circular aperture; SP, source plane; CCD, charge-coupled device; HP, hot plate; PC1, PC2, PC3, personal computers.
","sort":2,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure3","type":"article","typesetSecTagId":"s03","viewNum":0},{"columnNums":2,"dataId":"61adb11299d8812a099e4431","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2021/12/oea-2021-0027-Caiyangjian-4.jpg","fileType":"fulltextFig","fileXMLPath":"oea-2021-0027-Caiyangjian-4.jpg","id":"5afde5f5-463f-4718-a029-f45219dd0df8","imgWidth":"16.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"4","nameEn":"(a−d) Experimental results of the modulus of the DOC |μ| in the focal plane with different strength factors u. (e−h) The modulus of the DOC |μ| at different propagation distances z after the lens with the CP strength factor u=−60 mm−2.
","sort":3,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure4","type":"article","typesetSecTagId":"s03","viewNum":0},{"columnNums":2,"dataId":"61adb11299d8812a099e4431","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2021/12/oea-2021-0027-Caiyangjian-5.jpg","fileType":"fulltextFig","fileXMLPath":"oea-2021-0027-Caiyangjian-5.jpg","id":"381c21ca-0a3d-4245-b1c2-79db1e2e5b9a","imgWidth":"16.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"5","nameEn":"Experimental results of the modulus of the DOC |μ| in the focal plane at different temperatures of the HP. The strength factor of the CP is u=−60 mm−2. T=0 °C stands for the free space case.
","sort":4,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure5","type":"article","typesetSecTagId":"s03","viewNum":0},{"columnNums":2,"dataId":"61adb11299d8812a099e4431","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2021/12/oea-2021-0027-Caiyangjian-6.jpg","fileType":"fulltextFig","fileXMLPath":"oea-2021-0027-Caiyangjian-6.jpg","id":"8ced9f88-70b9-40d2-bad8-5a86a05cef85","imgWidth":"16.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"6","nameEn":"Experimental results of the dependence of the quality of the recovered image on the strength factor u in the focal plane in free space.
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","sort":7,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure8","type":"article","typesetSecTagId":"s04","viewNum":0}],"filePath":"/fileOEJ/journal/article/gdjz/2021/12/","firstFig":{"dataId":"61adb11299d8812a099e4431","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2021/12/OEA202112002_mini.jpg","fileType":"firstFig","fileXMLPath":"OEA202112002.jpg","id":"dbd491fe-0ae3-45fb-8b38-85ece0aad405","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"FIG. 1127.","nameCn":"FIG. 1127.","nameEn":"cover
","sort":-2,"supplementRemarkCn":"","supplementRemarkEn":"创刊于2018年
中国科学院光电技术研究所主办
中国科协“中国科技期刊国际影响力提升计划”D类项目支持
JCR影响因子22.4；CiteScore 26.8
探索全球光电科研热点的前沿创新
创造一个高端、专业的国际学术交流平台
主要方向包括但不限于：
• 光源和传感器 • 光电子学
• 纳米光子学 • 等离子体和超材料
• 光学成像 • 机器学习
• 先进光学材料
• 生物光子学和生物医学光学
• 非线性光学和超快光子学
• 光通信 • 光伏技术
微信公众号：光电期刊
推特：@OptoElectronAdv
Launch in March 2018, monthly
A high-quality, open access, peer reviewed research journal
JCR IF 22.4; CiteScore 26.8
Publishes top-quality original articles, letters and reviews
Focuses on the advances of the cutting edge innovations of optics, photonics and optoelectronics
The scope includes，but is not limited to:
• Light sources and sensors • Optoelectronics
• Nanophotonics • Plasmonics and metamaterials
• Optical imaging • Intelligent and digital optics
• Advanced optical materials
• Biophotonics and biomedical optics
• Nonlinear optics and ultrafast photonics
• Optical communications • Photovoltaics
Wechat: OE_Journal
Twitter: @OptoElectronAdv
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","sort":-2,"supplementRemarkCn":"","supplementRemarkEn":"The silver nanowires (Ag NWs) electrodes, which consist of incompact Ag nanoparticles (NPs) formed by multi-photon photoreduction, usually have poor conductivities. An effective strategy for enhancing conductivity of the Ag NWs electrodes is plasmon-enhanced nanosoldering (PLNS) by laser irradiation. Here, plasmon-enhanced photothermal effect is used to locally solder Ag NPs and then aggregates of these NPs grow into large irregular particles in PLNS process. Finite element method (FEM) simulations indicate that the soldering process is triggered by localized surface plasmon-induced electric field enhancement at “hot-spots”. The effectiveness of PLNS for enhancing conductivity depends on laser power density and irradiation time. By optimizing the conditions of PLNS, the electrical conductivity of Ag NWs is significantly enhanced and the conductivity σs is increased to 2.45×107 S/m, which is about 39% of the bulk Ag. This PLNS of Ag NWs provides an efficient and cost-effective technique to rapidly produce large-area metal nanowire electrodes and capacitors with high conductivity, excellent uniformity, and good flexibility.
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","sort":0,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure1","type":"article","typesetSecTagId":"s02","viewNum":0},{"columnNums":2,"dataId":"6065740399d8817cffa1aa59","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2021/12/OEA-2020-0101-Duanxuanming-2.jpg","fileType":"fulltextFig","fileXMLPath":"OEA-2020-0101-Duanxuanming-2.jpg","id":"44869c8c-3d78-4f06-ab58-16470de490e7","imgWidth":"16.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"2","nameEn":"TEM images of Ag NWs for overall (a), local (b) and magnified (c) topographies before the laser illumination. (d) Typical HRTEM images and (e) SAED patterns of Ag NPs before the laser illumination. TEM images of Ag NWs for overall (f), local (g) and magnified (h) topographies after the illumination. (i) Typical HRTEM images and (j) SAED pattern of Ag NPs after laser illumination for 15 min.
","sort":1,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure2","type":"article","typesetSecTagId":"s02","viewNum":0},{"columnNums":2,"dataId":"6065740399d8817cffa1aa59","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2021/12/OEA-2020-0101-Duanxuanming-3.jpg","fileType":"fulltextFig","fileXMLPath":"OEA-2020-0101-Duanxuanming-3.jpg","id":"b4283262-2825-454a-a752-ed4d22637873","imgWidth":"16.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"3","nameEn":"(a) Schematic of two-probe measurement method. (b) I-V curve of the fabricated Ag NWs before and after the laser nanosoldering. (c, f) Morphology of Ag NWs cut by focus ion beam. (d, g) AFM images and the height profile of the Ag NWs before and after the laser nanosoldering.
","sort":2,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure3","type":"article","typesetSecTagId":"s02","viewNum":0},{"columnNums":2,"dataId":"6065740399d8817cffa1aa59","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2021/12/OEA-2020-0101-Duanxuanming-4.jpg","fileType":"fulltextFig","fileXMLPath":"OEA-2020-0101-Duanxuanming-4.jpg","id":"b5c68695-a7f5-4aa2-ac6f-41d9b2b2451f","imgWidth":"16.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"4","nameEn":"(a) Measured resistance of the Ag NWs electrodes as a function of the laser nanosoldering power density with the laser nanosoldering time of 11 min. (b) Measured resistance of the Ag NWs electrodes as a function of the laser nanosoldering time with laser nanosoldering power density of 7.01 MW/cm2.
","sort":3,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure4","type":"article","typesetSecTagId":"s02","viewNum":0},{"columnNums":2,"dataId":"6065740399d8817cffa1aa59","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2021/12/OEA-2020-0101-Duanxuanming-5.jpg","fileType":"fulltextFig","fileXMLPath":"OEA-2020-0101-Duanxuanming-5.jpg","id":"74abeeb1-5b77-4bf3-93f1-0dcd7a146d71","imgWidth":"16.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"5","nameEn":"(a) Size distribution of Ag NPs in the Ag NWs fabricated in the silver ion contained precursor solutions at different concentrations of surfactant. (b) Schematic of simulation setup, a planar configuration is taken as an example. (c) Calculated temperature increasing ΔT (°C) at the surface of Ag NPs as a function of Ag NPs size, considering the local light intensity increased 300 times. The black areas (hot-spots) present the simulation results of the temperature distributions when the enhanced light field intensity increases 10 (d) and 300 (e) times by using FEM method.
","sort":4,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure5","type":"article","typesetSecTagId":"s02","viewNum":0},{"dataId":"6065740399d8817cffa1aa59","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2021/12/OEA202112003.jpg","fileType":"fulltextFig","fileXMLPath":"OEA202112003.jpg","id":"b826e542-6d8d-4181-a857-5ab06821a742","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"FIG. 1183.","nameEn":"","sort":5,"supplementRemarkCn":"","supplementRemarkEn":"(a) Schematic of experimental system for PLNS. (b) Scanning electron microscope (SEM) image of Ag NWs with inset showing the size distribution of Ag NPs in Ag NWs. (c) Plasmon-enhanced electric field as a function of interparticle gap for light polarization direction parallel and vertical to the interparticle axis. (d) Schematic illustration of PLNS with increasing laser irradiation time. (e) SEM images of the morphological changes of Ag NWs in PLNS process.
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中国科学院光电技术研究所主办
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","appendixList":[],"articleBusiness":{"articleId":"61ce65ec99d88125d5e50285","baiduIncludeResult":0,"baiduIncludeResultSearchNum":0,"baiduXueShuIncludeResult":0,"baiduXueShuIncludeResultSearchNum":0,"citeCount":0,"googleIncludeResult":0,"googleIncludeResultSearchNum":0,"htmlSource":1,"htmlViewCount":0,"id":"446f99a7-481c-11f0-9a6d-c4c6e6f11e4a","isRegCstr":0,"isRegDOI":1,"isUpdate":"1","pdfDownCount":0,"pdfEnFileSizeInt":0,"pdfFileName":"oea-2020-0036-Jiatianqing.pdf","pdfFileSize":2630.0,"pdfFileSizeInt":2630,"viewCount":0},"articleNo":"oea-2020-0036-Jiatianqing","articleReleaseProgresses":[],"authors":[{"addressTagIds":"aff1,aff2","articleId":"61ce65ec99d88125d5e50285","authorNameCn":"","authorNameEn":"Long Chen","authorRoleType":"author","authorTagVal":"1,2","corresper":false,"deceased":0,"givenNamesEn":"Long","id":"069e7648-ba15-4de8-bd4f-7cdb1e19abed","sortNumber":1,"surNameEn":"Chen"},{"addressTagIds":"aff1","articleId":"61ce65ec99d88125d5e50285","authorNameCn":"","authorNameEn":"Kaiqiang Cao","authorRoleType":"author","authorTagVal":"1","corresper":false,"deceased":0,"givenNamesEn":"Kaiqiang","id":"a87f8cde-dec6-452f-90b5-45bbab5f77ba","sortNumber":2,"surNameEn":"Cao"},{"addressTagIds":"aff1","articleId":"61ce65ec99d88125d5e50285","authorNameCn":"","authorNameEn":"Yanli Li","authorRoleType":"author","authorTagVal":"1","corresper":false,"deceased":0,"givenNamesEn":"Yanli","id":"67257f82-1306-4e25-9dfd-77c09e8cac2e","sortNumber":3,"surNameEn":"Li"},{"addressTagIds":"aff1","articleId":"61ce65ec99d88125d5e50285","authorNameCn":"","authorNameEn":"Jukun Liu","authorRoleType":"author","authorTagVal":"1","corresper":false,"deceased":0,"givenNamesEn":"Jukun","id":"d23bd6ca-bff5-4df4-bef2-e37156287685","sortNumber":4,"surNameEn":"Liu"},{"addressTagIds":"aff1","articleId":"61ce65ec99d88125d5e50285","authorNameCn":"","authorNameEn":"Shian Zhang","authorRoleType":"author","authorTagVal":"1","corresper":false,"deceased":0,"givenNamesEn":"Shian","id":"e07362f8-c53a-4cc7-80d2-b8f1f739536d","sortNumber":5,"surNameEn":"Zhang"},{"addressTagIds":"aff1","articleId":"61ce65ec99d88125d5e50285","authorNameCn":"","authorNameEn":"Donghai Feng","authorRoleType":"author","authorTagVal":"1","corresper":false,"deceased":0,"givenNamesEn":"Donghai","id":"4624e9e2-2f93-4a3d-9b39-9ee984e4708e","sortNumber":6,"surNameEn":"Feng"},{"addressTagIds":"aff1","articleId":"61ce65ec99d88125d5e50285","authorNameCn":"","authorNameEn":"Zhenrong Sun","authorRoleType":"author","authorTagVal":"1","corresper":false,"deceased":0,"givenNamesEn":"Zhenrong","id":"0c144b17-82a4-4217-8cd0-8901ed4dd60d","sortNumber":7,"surNameEn":"Sun"},{"addressTagIds":"aff1,aff2","articleId":"61ce65ec99d88125d5e50285","authorNameCn":"","authorNameEn":"Tianqing Jia","authorRoleType":"author","authorTagVal":"1,2","corresper":true,"correspinfoEn":"TQ Jia, E-mail: tqjia@phy.ecnu.edu.cn","deceased":0,"email":"tqjia@phy.ecnu.edu.cn","givenNamesEn":"Tianqing","id":"0ce3553f-a8df-4921-b359-c1d677028e15","sortNumber":8,"surNameEn":"Jia"}],"categoryNameCn":"","categoryNameEn":"Original Article","citationCn":"","citationEn":"Chen L, Cao KQ, Li YL, Liu JK, Zhang SA et al. Large-area straight, regular periodic surface structures produced on fused silica by the interference of two femtosecond laser beams through cylindrical lens. Opto-Electron Adv 4, 200036 (2021). DOI: 10.29026/oea.2021.200036","doi":"10.29026/oea.2021.200036","figList":[{"columnNums":2,"dataId":"61ce65ec99d88125d5e50285","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2021/12/oea-2020-0036-Jiatianqing-1.jpg","fileType":"fulltextFig","fileXMLPath":"oea-2020-0036-Jiatianqing-1.jpg","id":"eaaad8ec-e89a-4922-aa6f-9a85ae444ff9","imgWidth":"16.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"1","nameEn":"Experimental setup for femtosecond laser interference using two cylindrical lenses. HWP: half-wave plate, GP: Glan prism, BS: beam splitter. The double arrow and letter E represent the laser polarization.
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","sort":1,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure2","type":"article","typesetSecTagId":"s02","viewNum":0},{"columnNums":2,"dataId":"61ce65ec99d88125d5e50285","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2021/12/oea-2020-0036-Jiatianqing-3.jpg","fileType":"fulltextFig","fileXMLPath":"oea-2020-0036-Jiatianqing-3.jpg","id":"7ed9533a-b9ae-415e-ad82-595d823a7466","imgWidth":"16.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"3","nameEn":"(a) Schematic diagram of laser processing of fused silica surface. Green squares indicate the regions at which the images in (b) and (c) were measured. SEM images of LSFLs obtained using (b) cylindrical lens and (c) circular lens. The laser fluence is 2.8 J/cm2, and the scanning velocity is 3.1 mm/s. The scale bar in (b) and (c) is 5 μm. (d) SEM image of cross section of LSFL on fused silica obtained using a laser focused by a cylindrical lens. (e) and (f) are the 2D-FT images of the LSFLs in (b) and (c), respectively. (g) is the FT spectra for ky = 0 μm–1.
","sort":2,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure3","type":"article","typesetSecTagId":"s03","viewNum":0},{"columnNums":1,"dataId":"61ce65ec99d88125d5e50285","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2021/12/oea-2020-0036-Jiatianqing-4.jpg","fileType":"fulltextFig","fileXMLPath":"oea-2020-0036-Jiatianqing-4.jpg","id":"5119c39c-f8ee-4f6d-8fd5-18798c5d4112","imgWidth":"8.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"4","nameEn":"SEM images of micro-/nanostructures on fused silica produced by TBI, where each laser beam had a fluence of 2.8 J/cm2, and the scanning velocity was (a) 8.2 and (b) 4.8 mm/s. (c) and (d) are SEM images of the red areas in (a) and (b), respectively. The green arrow represents the scanning direction. The scale bar is 20 μm in (a) and (b), and is 2 μm in (c) and (d).
","sort":3,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure4","type":"article","typesetSecTagId":"s03","viewNum":0},{"columnNums":1,"dataId":"61ce65ec99d88125d5e50285","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2021/12/oea-2020-0036-Jiatianqing-5.jpg","fileType":"fulltextFig","fileXMLPath":"oea-2020-0036-Jiatianqing-5.jpg","id":"9d220e72-9504-438d-bfcf-15f8669d2bca","imgWidth":"8.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"5","nameEn":"SEM images of micro-/nanostructures on fused silica obtained at a scanning velocity of 6.2 mm/s and laser fluences of (a) 1.8, (b) 2.1, (c) 2.8, and (d) 3.2 J/cm2. The scale bar is 2 μm. Double arrow indicates the laser polarization direction.
","sort":4,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure5","type":"article","typesetSecTagId":"s03","viewNum":0},{"columnNums":1,"dataId":"61ce65ec99d88125d5e50285","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2021/12/oea-2020-0036-Jiatianqing-6.jpg","fileType":"fulltextFig","fileXMLPath":"oea-2020-0036-Jiatianqing-6.jpg","id":"51a99ff4-bf8a-456c-b2cb-8608a90e9069","imgWidth":"8.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"6","nameEn":"LIPSS period and duty cycle versus fluence at a constant scanning velocity of 6.2 mm/s.
","sort":5,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure6","type":"article","typesetSecTagId":"s03","viewNum":0},{"columnNums":1,"dataId":"61ce65ec99d88125d5e50285","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2021/12/oea-2020-0036-Jiatianqing-7.jpg","fileType":"fulltextFig","fileXMLPath":"oea-2020-0036-Jiatianqing-7.jpg","id":"7eca6a8a-e7ad-4af6-aa77-baf4717d42bb","imgWidth":"8.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"7","nameEn":"SEM images of micro-/nanostructures on fused silica obtained at a constant laser fluence of 2.8 J/cm2 and a scanning velocity of (a) 12, (b) 6.2, (c) 4.8, and (d) 2.4 mm/s. The scale bar is 5 μm. The double-headed arrow and E in (a) indicate the incident laser polarization direction.
","sort":6,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure7","type":"article","typesetSecTagId":"s03","viewNum":0},{"columnNums":1,"dataId":"61ce65ec99d88125d5e50285","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2021/12/oea-2020-0036-Jiatianqing-8.jpg","fileType":"fulltextFig","fileXMLPath":"oea-2020-0036-Jiatianqing-8.jpg","id":"bb95bd6c-54a7-4a7c-94e4-d1338a5135e2","imgWidth":"8.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"8","nameEn":"LIPSS period and the duty cycle versus scanning velocity at a constant laser fluence of 2.8 J/cm2.
","sort":7,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure8","type":"article","typesetSecTagId":"s03","viewNum":0},{"columnNums":2,"dataId":"61ce65ec99d88125d5e50285","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2021/12/oea-2020-0036-Jiatianqing-9.jpg","fileType":"fulltextFig","fileXMLPath":"oea-2020-0036-Jiatianqing-9.jpg","id":"009a47b1-c15e-4fcf-8759-529a2c2e6dcd","imgWidth":"16.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"9","nameEn":"Optical characterization of structured silica surface with grating-like LIPSSs and spaced LIPSSs. (a) Diffraction spectra and (b) color images of structured silica with grating-like LIPSSs. (c) Diffraction spectra and (d) color images of structured silica with spaced LIPSSs.
","sort":8,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure9","type":"article","typesetSecTagId":"s03","viewNum":0},{"columnNums":1,"dataId":"61ce65ec99d88125d5e50285","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2021/12/oea-2020-0036-Jiatianqing-10.jpg","fileType":"fulltextFig","fileXMLPath":"oea-2020-0036-Jiatianqing-10.jpg","id":"f04e455c-0b34-4e4e-9173-05a5a3a3a3e7","imgWidth":"8.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"10","nameEn":"Optical image of falling petal pattern consisting of grating-like LIPSSs.
","sort":9,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure10","type":"article","typesetSecTagId":"s03","viewNum":0},{"columnNums":1,"dataId":"61ce65ec99d88125d5e50285","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2021/12/oea-2020-0036-Jiatianqing-11.jpg","fileType":"fulltextFig","fileXMLPath":"oea-2020-0036-Jiatianqing-11.jpg","id":"4476c472-67d4-4efe-acca-deed25710adb","imgWidth":"8.0cm","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"11","nameEn":"Colorful optical images of two flower patterns consisting of grating-like LIPSSs oriented in different directions. (a) Schematic of the processing method. The green arrow represents the scanning direction. (b) Schematic of the flower pattern. (c) The images of flowers with grating-like LIPSSs in radial direction, and (d) in azimuthal direction. Insets show SEM images of the grating-like LIPSSs in the open red squares.
","sort":10,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure11","type":"article","typesetSecTagId":"s03","viewNum":0},{"dataId":"61ce65ec99d88125d5e50285","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2021/12/OEA202112004.jpg","fileType":"fulltextFig","fileXMLPath":"OEA202112004.jpg","id":"b623a927-192a-4935-ba35-e85015721cc0","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"FIG. 1195.","nameEn":"","sort":11,"supplementRemarkCn":"","supplementRemarkEn":"Experimental setup for femtosecond laser interference using two cylindrical lenses. HWP: half-wave plate, GP: Glan prism, BS: beam splitter. The double arrow and letter E represent the laser polarization.
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中国科学院光电技术研究所主办
中国科协“中国科技期刊国际影响力提升计划”D类项目支持
JCR影响因子22.4；CiteScore 26.8
探索全球光电科研热点的前沿创新
创造一个高端、专业的国际学术交流平台
主要方向包括但不限于：
• 光源和传感器 • 光电子学
• 纳米光子学 • 等离子体和超材料
• 光学成像 • 机器学习
• 先进光学材料
• 生物光子学和生物医学光学
• 非线性光学和超快光子学
• 光通信 • 光伏技术
微信公众号：光电期刊
推特：@OptoElectronAdv
Launch in March 2018, monthly
A high-quality, open access, peer reviewed research journal
JCR IF 22.4; CiteScore 26.8
Publishes top-quality original articles, letters and reviews
Focuses on the advances of the cutting edge innovations of optics, photonics and optoelectronics
The scope includes，but is not limited to:
• Light sources and sensors • Optoelectronics
• Nanophotonics • Plasmonics and metamaterials
• Optical imaging • Intelligent and digital optics
• Advanced optical materials
• Biophotonics and biomedical optics
• Nonlinear optics and ultrafast photonics
• Optical communications • Photovoltaics
Wechat: OE_Journal
Twitter: @OptoElectronAdv
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","sort":1,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure2","type":"article","typesetSecTagId":"s2","viewNum":0},{"dataId":"5fa4dc9ff4d7917194c90a84","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2020/9/OEA-3-9-190043-1-3.jpg","fileType":"fulltextFig","fileXMLPath":"OEA-3-9-190043-1-3.jpg","id":"cfd7ab84-29d3-4eb6-9983-c369332e25ce","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"3","nameEn":"(a) Cross-sectional TEM structure characterization and optical absorption spectra stability test before and after ALD treatment74. (b) EELS color-coded elemental intensity maps of Al and Br, CsPbBr3 QD/AlOx nanocomposites PL properties over 45 days of storage in ambient conditions and after 1 h of soaking in water70. Figure reproduced from: (a) ref.74, American Chemical Society; (b) ref.70, John Wiley and Sons.
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","sort":3,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure4","type":"article","typesetSecTagId":"s2","viewNum":0},{"dataId":"5fa4dc9ff4d7917194c90a84","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2020/9/OEA-3-9-190043-1-5.jpg","fileType":"fulltextFig","fileXMLPath":"OEA-3-9-190043-1-5.jpg","id":"9ba8421d-0014-4858-89b2-fe637656effa","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"5","nameEn":"(a) FTIR spectra of ALD-coated and uncoated thin films comprised of ZnO nanocrystals76. (b) XPS scans for Pb 4f and Al 2p of the AlxOy-PbS film78. (c) Ligands exchange and ALD infilling schematic resulting in barrier width and height reduce55. Figure reproduced from: (a) ref.76, American Chemical Society; (b) ref.78, AIP Publishing; (c) ref.55, American Chemical Society.
","sort":4,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure5","type":"article","typesetSecTagId":"s2","viewNum":0},{"dataId":"5fa4dc9ff4d7917194c90a84","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2020/9/OEA-3-9-190043-1-6.jpg","fileType":"fulltextFig","fileXMLPath":"OEA-3-9-190043-1-6.jpg","id":"13d64ec5-058a-411f-8f77-56b8cc84fa3a","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"6","nameEn":"(a) Schematic of barrier layer configurations available in quantum dot-sensitized solar cells. Comparison of device efficiency and dark current onset for TiO2/Al2O3/QD and TiO2/QD/Al2O3 configurations under 1 sun of illumination with varying ALD cycles of Al2O382. (b) Band energy level diagram of each material in QLED. Current density of electron only device without and with Al2O3 interlayers, and hole only device. Device lifetime of QLEDs without and with Al2O3 interlayer63. Figure reproduced from: (a) ref.82, American Chemical Society; (b) ref.63, Creative Commons Attribution 3.0 International License.
","sort":5,"supplementRemarkCn":"","supplementRemarkEn":"","tagId":"Figure6","type":"article","typesetSecTagId":"s2","viewNum":0},{"dataId":"5fa4dc9ff4d7917194c90a84","fileFrom":"xml","fileLastName":"jpg","filePath":"/fileOEJ/journal/article/gdjz/2020/9/OEA-3-9-190043-1-7.jpg","fileType":"fulltextFig","fileXMLPath":"OEA-3-9-190043-1-7.jpg","id":"88df17ee-1f1d-4d77-904b-3a30609dfb4c","journalId":"4ee57c6d-45a7-470d-89c1-62fa1069de73","labelText":"7","nameEn":"(a) Schematic diagram of the ALD interface passivating mechanism61. (b) EDS mappings obtained after device operation for QLEDs without and with an Al2O3 barrier layer61. Figure reproduced from ref.61, American Chemical Society.
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中国科学院光电技术研究所主办
中国科协“中国科技期刊国际影响力提升计划”D类项目支持
JCR影响因子22.4；CiteScore 26.8
探索全球光电科研热点的前沿创新
创造一个高端、专业的国际学术交流平台
主要方向包括但不限于：
• 光源和传感器 • 光电子学
• 纳米光子学 • 等离子体和超材料
• 光学成像 • 机器学习
• 先进光学材料
• 生物光子学和生物医学光学
• 非线性光学和超快光子学
• 光通信 • 光伏技术
微信公众号：光电期刊
推特：@OptoElectronAdv
Launch in March 2018, monthly
A high-quality, open access, peer reviewed research journal
JCR IF 22.4; CiteScore 26.8
Publishes top-quality original articles, letters and reviews
Focuses on the advances of the cutting edge innovations of optics, photonics and optoelectronics
The scope includes，but is not limited to:
• Light sources and sensors • Optoelectronics
• Nanophotonics • Plasmonics and metamaterials
• Optical imaging • Intelligent and digital optics
• Advanced optical materials
• Biophotonics and biomedical optics
• Nonlinear optics and ultrafast photonics
• Optical communications • Photovoltaics
Wechat: OE_Journal
Twitter: @OptoElectronAdv
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