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The circle array was optimized by adopting a genetic algorithm with an improved real coding method coding the location of sub-apertures. The measure function was designed based on maximizing the distances between u-v coverage dots and minimizing the redundant array. The point spread function, optical transfer function and diffractive imaging were analyzed with the circle array synthetic aperture imaging system. The optimized result of 8 to 16 sub-apertures on a circle array was obtained, and they were compared to the results achieved through simulated annealing algorithm. Using the emulator program, the point spread function was analyzed and contrasted to that of a uniform circle array. Results show that the real coding genetic algorithm can resolve the array optimization well, cost less time and get a better optimization compared with the simulated annealing algorithm.",{"EN":77},"Optical synthetic aperture circle-array optimization based on genetic algorithm",{"VOID":79},"[\"5738018577076255354\"]",{"VOID":81},"Meinel A B. Aperture synthesis using independent telescope. Applied Optics, 1970, 9(11): 2501–2504\nThompson A R, Moran J M, Swenson G W. Interferometry and Synthesis in Radio Astronomy. New York: Wiley-Interscience, 2001, 426–466\nJiang Y S. Size effects of sub-aperture on imaging of linear array of optical synthetic aperture. Acta Optica Sinica, 2005, 25(8): 1042–1047 (in Chinese)\nGuyon O, Roddier F. Aperture rotation synthesis: optimization of the (u, v)-plane coverage for a rotating phased array of telescopes. Publications of the Astronomical Society of the Pacific, 2001, 113: 98–104\nChen H T, Jiang Y S, Zhong Y. Study of optimization and imaging characteristics of two-dimensional circle array for optical synthetic aperture system. Acta Optica Sinica, 2005, 25(12): 1616–1622 (in Chinese)\nCornwell T J. A novel principle for optimization of the instantaneous Fourier plane coverage of correlation arrays. IEEE Transactions on Antennas and Propagation, 1988, 36(8): 1165–1167\nXing WX, Xie J X. Modern Optimization Algorithms. Beijing: Tsinghua University Press, 1999, 140–192 (in Chinese)\nWang F L, Wang J Q, Wu C Y, et al. The improved research on actual number genetic algorithms. Journal of Biomathematics, 2006, 21(1): 153–158 (in Chinese)\nFan W J, Xia L Z, Zhou B F. Mathematical model of optical aperture synthesis image-plane interference and computer simulation. Journal of Infrared and Millimeter Waves, 2004, 23(2): 143–147 (in Chinese)\nGreenaway A H. Optical aperture synthesis. Measurement Science and Technology, 1991, (2): 1–12\nLong W J, Wang Z L, Zhou Y P. Imaging analysis computer simulation of optical synthetic aperture telescope. Acta Optica Sinica, 2004, 24(8): 1009–1014 (in Chinese)\nWang H T, Zhou B F. Beam combiner in optical aperture synthesis telescope array. Acta Optica Sinica, 2002, 22(9): 1109–1115 (in Chinese)",{"VOID":83},"10.1007\u002Fs12200-008-0070-9","PUBLICATION","VERIFIED","2024-06-26T22:47:09.763+00:00","Auto Verify","https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1007\u002Fs12200-008-0070-9",[90,108,121],{"id":91,"sortIndex":21,"researcher":20,"roles":92,"affiliations":94,"properties":103,"displayName":105,"givenName":20,"familyName":20},"bb9ef61b-9977-41fb-a89c-d5faca07c8b0",[93],"AUTHOR",[95],{"id":96,"sortIndex":21,"affiliation":97,"properties":20},"30f65f7a-2c7f-4092-a4ed-552caf3ffa73",{"id":96,"createTime":20,"updateTime":20,"relativeEntities":98,"slug":20,"properties":99,"entityType":20,"verifyStatus":20,"verifyTime":20,"verifyNote":20,"languages":20,"translateLanguages":20,"viewCount":20,"url":20,"parentIds":102,"statistic":20},[],{"title":100},{"VI":101},"School of Electronic Information Engineering, Beihang University, Beijing, China",[],{"title":104,"gsAuthor":106},{"VI":105},"Yuntao He",{"VOID":107},"[\"2oxx-rAAAAAJ\"]",{"id":109,"sortIndex":58,"researcher":20,"roles":110,"affiliations":111,"properties":118,"displayName":120,"givenName":20,"familyName":20},"6871d7de-2e84-4169-9d57-3bb71f2060ea",[93],[112],{"id":96,"sortIndex":21,"affiliation":113,"properties":20},{"id":96,"createTime":20,"updateTime":20,"relativeEntities":114,"slug":20,"properties":115,"entityType":20,"verifyStatus":20,"verifyTime":20,"verifyNote":20,"languages":20,"translateLanguages":20,"viewCount":20,"url":20,"parentIds":117,"statistic":20},[],{"title":116},{"VI":101},[],{"title":119},{"VI":120},"Yuesong Jiang",{"id":122,"sortIndex":123,"researcher":20,"roles":124,"affiliations":125,"properties":132,"displayName":134,"givenName":20,"familyName":20},"1740332b-9850-4322-92ec-6a0e3723f738",2,[93],[126],{"id":96,"sortIndex":21,"affiliation":127,"properties":20},{"id":96,"createTime":20,"updateTime":20,"relativeEntities":128,"slug":20,"properties":129,"entityType":20,"verifyStatus":20,"verifyTime":20,"verifyNote":20,"languages":20,"translateLanguages":20,"viewCount":20,"url":20,"parentIds":131,"statistic":20},[],{"title":130},{"VI":101},[],{"title":133},{"VI":134},"Guangda Liu","ARTICLE",{"url":88,"publisher":137,"properties":163},{"id":6,"createTime":7,"updateTime":8,"relativeEntities":138,"slug":10,"properties":139,"entityType":18,"verifyStatus":19,"verifyTime":20,"verifyNote":20,"languages":20,"translateLanguages":20,"viewCount":21,"subjectFields":143,"manageAffiliations":144,"indexDatabases":145,"url":55,"thumbnailPath":20,"statistic":158,"gsStatistic":20,"type":62,"analyzePriority":20},[],{"issn":140,"title":141,"eissn":142},{"VOID":13},{"EN":15},{"VOID":17},[],[],[146,152],{"id":26,"indexDatabase":147,"url":37,"indexYears":38,"academicFieldIds":20,"indexDatabaseRanking":39},{"id":28,"createTime":20,"updateTime":20,"relativeEntities":148,"label":149,"description":150,"key":34,"publicationTags":151,"standard":20},[],{"EN":31,"VI":31},{"EN":31,"VI":33},[36],{"id":41,"indexDatabase":153,"url":54,"indexYears":20,"academicFieldIds":20,"indexDatabaseRanking":20},{"id":43,"createTime":20,"updateTime":20,"relativeEntities":154,"label":155,"description":156,"key":50,"publicationTags":157,"standard":20},[],{"EN":46,"VI":46},{"EN":48,"VI":49},[52,53],{"impactFactor":21,"impactFactorByYear":159,"i10Index":21,"i10IndexLast5Year":21,"totalPublication":58,"totalPublicationByYear":160,"totalCitation":21,"totalCitationByYear":161,"totalCitationPerPublication":21,"totalCitationPerPublicationByYear":162,"hindexLast5Year":21,"hindex":21},{},{"2012":58},{},{},{"pages":164,"volume":166},{"VOID":165},"268-273",{"VOID":167},"1",{"total":58,"publishYear":169,"statisticByYear":170},2009,{"2016":58},"2009-02-05","DONE_ANALYZE_CITATION",[52,36],false,{"id":176,"createTime":177,"updateTime":178,"relativeEntities":179,"slug":180,"properties":181,"entityType":84,"verifyStatus":85,"verifyTime":192,"verifyNote":87,"languages":20,"translateLanguages":20,"viewCount":21,"primaryUrl":193,"fullTextUrl":20,"authors":194,"publicationType":135,"publisherRelationship":284,"citationCount":20,"citationInfo":20,"publishDate":315,"publishYear":316,"citationAnalyzeStatus":19,"lastCitationAnalyze":178,"indexDatabases":317,"openAccess":20,"references":20,"isForceReanalyzing":174},"aa305914-8df7-4009-8154-a472d4825bb4","2023-12-11T17:23:04.344+00:00","2026-07-16T20:53:43.783+00:00",[],"An-in-vitro-study-of-femtosecond-laser-photodisruption-in-rabbit-sclera",{"abstract":182,"title":184,"gsPaper":186,"references":188,"doi":190},{"EN":183},"To explore the possibility of photodisruption in rabbit sclera by femtosecond (fs) laser and seek appropriate incision techniques and relevant parameters, a fs laser (800 nm\u002F50 fs) with different pulse energies was applied to irradiate rabbit sclera in vitro. By moving a computer-controlled three-axis translation stage to which the sample was attached, the laser achieved three types of incisions: transscleral channel, snake pattern and linear cut. The irradiated samples were observed by light microscopy and scanning electron microscopy (SEM). In comparison with fs laser, Nd:YAG was used as control. The experimental results show that through an objective lens with numerical aperture (NA) of 0.2, the fs laser with power intensity larger than 955 TW\u002Fcm2 and pulse energy ranging from 37.5–125 μJ, cutting depths from 30–70 μm may be achieved after linearly scanning in sclera at a translation speed of 0.1 mm\u002Fs. However, it failed to make any photodisruption when the power intensity was below 796 TW\u002Fcm2 or the pulse energy was less than 31.25 μJ under the same condition. Compared with the Nd:YAG laser, the inner wall of the channel was smoother and the damage to the surrounding tissues was slight with the fs laser. The high precision of intrascleral photodisruption and minimal damage to surrounding tissues by a fs laser display its potential application in the treatment of glaucoma.",{"EN":185},"An in vitro study of femtosecond laser photodisruption in rabbit sclera",{"VOID":187},"[\"14684841696035312275\"]",{"VOID":189},"Toyran S, Liu Y M, Singha S, et al. Femtosecond laser photodisruption of human trabecular meshwork: an in vitro study. Experimental Eye Research, 2005, 81(3): 298–305\nNgoi B K, Hou D X, Koh L H, et al. Femtosecond laser for glaucoma treatment: a study on ablation energy in pig iris. Lasers in Medical Science, 2005, 19(4): 218–222\nJuhasz T, Kastis G A, Suarez C, et al. Time-resolved observations of shock waves and cavitation bubbles generated by femtosecond laser pulses in corneal tissue and water. Lasers in Surgery and Medicine, 1996, 19(1): 23–31\nSchwab B, Hagner D, Müller W, et al. Bone ablation using ultrashort laser pulses. A new technique for middle ear surgery. Laryngorhinootologie, 2004, 83(4): 219–225\nBinder P S. Flap dimensions created with the IntraLase FS laser. Journal of Cataract and Refractive Surgery, 2004, 30(1): 26–32\nLubatschowski H, Maatz G, Heisterkamp A, et al. Application of ultra-short laser pulses for intrastromal refractive surgery. Graefe’s Archive for Clinical and Experimental Ophthalmology, 2000, 238(1): 33–39\nSacks Z S, Kurtz R M, Juhasz T, et al. High precision subsurface photodisruption in human sclera. Journal of Biomedical Optics, 2002, 7(3): 442–450\nWang X F, Jia T Q, Li X X, et al. Ablation and ultrafast dynamics of zinc selenide under femtosecond laser irradiation. Chinese Optics Letters, 2005, 3(10): 615–617\nSacks Z S, Kurtz R M, Juhasz T, et al. Subsurface photodisruption in human sclera: wavelength dependence. Ophthalmic Surgery, Lasers & Imaging, 2003, 34(2): 104–113\nChen H X, Jia T Q, Huang M, et al. Visible-infrared femtosecond laser-induced optical breakdown of 6H SiC. Acta Optica Sinica, 2006, 26(3): 468–470 (in Chinese)\nNiemz M H. Laser-Tissue Interactions Fundamentals and Applications (in Chinese, trans. Zhang Zhenxi). 3rd ed. Beijing: Science Press, 2005, 92–132\nXing Q R, Mao F L, Lang L Y, et al. Experiment research on femtosecond laser cell micromanipulation system. Chinese Journal of Lasers, 2004, 31(6): 728\nFrederickson K S, White W E, Wheeland R G, et al. Precise ablation of skin with reduced collateral damage using the femtosecond-pulsed, terawatt titanium-sapphire laser. Archives of Dermatology, 1993, 129(8): 989–993\nSuhm N, Götz M H, Fischer J P, et al. Ablation of neural tissue by short-pulsed lasers-a technical report. Acta Neurochirurgica, 1996, 138(3): 346–349\nKrueger R R, Kuszak J, Lubatschowski H, et al. First safety study of femtosecond laser photodisruption in animal lenses: tissue morphology and cataractogenesis. Journal of Cataract and Refractive Surgery, 2005, 31(12): 2386–2394\nGerten G, Ripken T, Breitenfeld P, et al. In vitro and in vivo investigations on the treatment of presbyopia using femtosecond lasers. Ophthalmologe, 2007, 104(1): 40–46\nSerbin J, Bauer T, Fallnich C, et al. Femtosecond lasers as novel tool in dental surgery. Applied Surface Science, 2002, 197–198: 737–740\nNiemz M H, Kasenbacher A, Strassl M, et al. Tooth ablation using a CPA-free thin disk femtosecond laser system. Applied Physics B, 2004, 79(3): 269–271\nVogel A, Venugopalan V. Mechanisms of pulsed laser ablation of biological tissues. Chemical Reviews, 2003, 103(2): 577–644\nStern D, Schoenlein R W, Puliafito C A, et al. Corneal ablation by nanosecond, picosecond and femtosecond lasers at 532 and 625 nm. Archives of Ophthalmology, 1989, 107(4): 587–592",{"VOID":191},"10.1007\u002Fs12200-008-0022-4","2024-06-25T05:45:27.327+00:00","http:\u002F\u002Flink.springer.com\u002F10.1007\u002Fs12200-008-0022-4",[195,210,223,240,256,270],{"id":196,"sortIndex":21,"researcher":20,"roles":197,"affiliations":198,"properties":207,"displayName":209,"givenName":20,"familyName":20},"50177a36-eb4d-409a-a9f3-e678c3318822",[93],[199],{"id":200,"sortIndex":21,"affiliation":201,"properties":20},"17668e16-9f63-4381-b08c-46431d1bed8e",{"id":200,"createTime":20,"updateTime":20,"relativeEntities":202,"slug":20,"properties":203,"entityType":20,"verifyStatus":20,"verifyTime":20,"verifyNote":20,"languages":20,"translateLanguages":20,"viewCount":20,"url":20,"parentIds":206,"statistic":20},[],{"title":204},{"EN":205},"Department of Ophthalmology, Union Hospital, Tongji Medical College, Huazhong University of Science and Technology, Wuhan, China",[],{"title":208},{"VI":209},"Fagang 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× 128, 128 × 160 and 256 × 256 AlGaAs\u002FGaAs quantum well infrared photodetector (QWIP) focal plane arrays (FPA) as well as a large area test device are designed and fabricated. The device with n-doped back-illuminated AlGaAs\u002FGaAs quantum structure is achieved by metal organic chemical vapor deposition (MOCVD) epitaxial growth and GaAs integrated circuit processing technology. The test device is valued by its dark current performance and Fourier transform infrared spectroscopy (FTIR) spectra at 77 K. Cut off wavelengths of 9 and 10.9 μm are realized by using different epitaxial structures. The blackbody detectivity D\n                        B* is as high as 2.6 × 109 cm⋅Hz1\u002F2⋅W−1. The 128 6128 FPA is flip-chip bonded on a CMOS readout integrated circuit with indium (In) bumps. The infrared thermal images of some targets under room temperature background have been successfully demonstrated at 80 K operating temperature. In addition, the methods to further improve the image quality are discussed.",{"EN":328},"AlGaAs\u002FGaAs quantum well infrared photodetector focal plane array based on MOCVD technology",{"VOID":330},"16847129206908425533",{"EN":332},"",{"VOID":334},"Levine B F. Quantum-well infrared photodetectors. Journal of Applied Physics, 1993, 74(8): R1–R81\nLevine B F, Zussman A, Kuo J M, et al. 19 μm cutoff long wavelength GaAs\u002FAlx Ga1-x As quantum well infrared photo-detectors. Journal of Applied Physics, 1992, 71(10), 5130–5135\nLiu H C, Wasilewski Z R, Buchanan M, et al. Segregation of Si δ doping in GaAs-AlGaAs quantum wells and the cause of the asymmetry in the current-voltage characteristics of intersubband infrared detectors. Applied Physics Letters, 1993, 63(6): 761–763\nGunapala S D, Bandara S V, Singh A, et al. 640 × 486 long-wavelength two-color GaAs\u002FAlGaAs quantum well infrared photodetector (QWIP) focal plane array camera. IEEE Transactions on Electron Devices, 2000, 47(5): 963–971\nGunapala S D, Bandara S V, Liu J K, et al. 1024 × 1024 mid-wavelength and long-wavelength QWIP focal plane arrays for imaging applications. Semiconductor Science and Technology, 2005, 20(5): 473–480\nYu X Z, Guo X D. A 128 × 1 multiquantum well infrared linear array and its signal readout. Infrared Technology, 1999, 21(2): 35–38 (in Chinese)\nLi N, Li N, Lu W, et al. Development of 64 × 64 GaAs\u002FAlGaAs MQW long-wave infrared FPAs. Journal of infrared and Millimeter Waves, 1999, 18(6): 427–430 (in Chinese)\nSu Y M, Zhong M, Zhang Y B, et al. A 128 × 160 pixel GaAs\u002F AlGaAs multi-quantum well long-wavelength infrared photo-detector focal plane array. Chinese Journal of Semiconductors, 2005, 26(10): 2044–2047 (in Chinese)\nLi X J, Liu Y B, Feng Z, et al. 9 μm cutoff 128 × 128 AlGaAs\u002F GaAs quantum well infrared photodetector focal plane arrays. Chinese Journal of Semiconductors, 2006, 27(8): 1355–1359\nZussman A, Levine B F, Kuo J M, et al. Extended long-wavelength λ = 11−15 μm GaAs\u002FAlx Ga1™x As quantum-well infrared photodetectors. Journal of Applied Physics, 1991, 70(9): 5101–5107\nGunapala S D, Bandara S V. Quantum well infrared photo-detector (QWIP) focal plane arrays. Semiconductors and Semimetals, 1999, 62: 197–282",{"VOID":336},"10.1007\u002Fs12200-008-0051-z","2024-04-25T20:27:13.086+00:00","https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1007\u002Fs12200-008-0051-z",[340,355,368,381,394,407,420,434,448],{"id":341,"sortIndex":21,"researcher":20,"roles":342,"affiliations":343,"properties":352,"displayName":354,"givenName":20,"familyName":20},"6d077d20-e728-4d6f-a27b-20457c36f9c0",[93],[344],{"id":345,"sortIndex":21,"affiliation":346,"properties":20},"9185408b-02f2-4f42-a8bf-9a8bcecf6259",{"id":345,"createTime":20,"updateTime":20,"relativeEntities":347,"slug":20,"properties":348,"entityType":20,"verifyStatus":20,"verifyTime":20,"verifyNote":20,"languages":20,"translateLanguages":20,"viewCount":20,"url":20,"parentIds":351,"statistic":20},[],{"title":349},{"VI":350},"13th Institute of China Electronic Technology Group Corporation, Shijiazhuang, China",[],{"title":353},{"VI":354},"Xianjie 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all-optical filter structure to simultaneously implement microwave bandpass and notch filter is proposed and experimentally demonstrated. The structure is based on a recirculating delay line (RDL) loop consisting of a semiconductor optical amplifier (SOA) followed by a tunable narrowband optical filter and a 10:90 coupler. The converted signal is generated in a wavelength conversion process based on cross-gain modulation of amplified spontaneous emission in the SOA. The converted signal circulating in RDL loop realizes a negative bandpass response. The negative bandpass filter and a broadband allpass filter are synthesized to achieve a notch filter with flat passband which can excise interference with minimal impact on the wanted signal.",{"EN":500},"All-optical filter for simultaneous implementation of microwave bandpass and notch responses based on semiconductor optical amplifier",{"VOID":502},"[\"894482526551990325\"]",{"VOID":504},"Hunter D B, Minasian R A. Photonic signal processing of microwave signals using an active-fiber Bragg-grating-pair structure. IEEE Transactions on Microwave Theory and Techniques, 1997, 45(8): 1463–1466\nChan E H W, Minasian R A. Reflective amplified recirculating delay line bandpass filter. Journal of Lightwave Technology, 2007, 25(6): 1441–1446\nNing G, Aditya S, Shum P, Zhou J Q. Switchable coherence-free microwave photonic notch filter using a pair of intensity modulators. IEEE Photonics Technology Letters, 2008, 20(4): 261–263\nWang J, Yao J P. A tunable photonic microwave notch filter based on all-optical mixing. IEEE Photonics Technology Letters, 2006, 18(1–4): 382–384\nChan E H W, Minasian R A. Remodulation based coherence-free photonic notch filter with wide passband. Electronics Letters, 2007, 43(11): 641–642\nChan E H W, Minasian R A. High-resolution photonics-based interference suppression filter with wide passband. Journal of Lightwave Technology, 2003, 21(12): 3144–3149\nMinasian R A, Alameh K E, Chan E H W. Photonics-based interference mitigation filters. IEEE Transactions on Microwave Theory and Techniques, 2001, 49(10): 1894–1899\nYi X K, Fang W, Ng J H, Lu C. Tunable microwave filter design using wavelength conversion technique and high dispersion time delays. IEEE Photonics Technology Letters, 2001, 13(8): 857–859\nLiu DM, Ng J H, Lu C. Wavelength conversion based on cross-gain modulation of ASE spectrum of SOA. IEEE Photonics Technology Letters, 2000, 12(9): 1222–1224\nXu E M, Zhang X L, Zhou L N, Zhang Y, Huang D X. All-optical microwave notch filter with flat passband based on semiconductor optical amplifier. Optics Communications, 2009, 282(12): 2297–2300\nXu E M, Zhang X L, Zhou L N, Zhang Y, Huang D X. A simple microwave photonic notch filter based on a semiconductor optical amplifier. Journal of Optics A: Pure and Applied Optics, 2009, 11(8): 085405\nNing G, Cheng L H, Aditya S, Shum P, Zhou J Q. Microwave photonic filter with triangle shaped infinite impulse response. Electronics Letters, 2008, 44(3): 208–210",{"VOID":506},"10.1007\u002Fs12200-009-0060-6","2024-05-14T22:01:47.430+00:00","https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1007\u002Fs12200-009-0060-6",[510,525,540,553,568,583,596],{"id":511,"sortIndex":21,"researcher":20,"roles":512,"affiliations":513,"properties":522,"displayName":524,"givenName":20,"familyName":20},"b5c0d938-51d5-4876-b3a2-3417cae73beb",[93],[514],{"id":515,"sortIndex":21,"affiliation":516,"properties":20},"5c6fdd75-85e2-4ea2-90f5-f45256439950",{"id":515,"createTime":20,"updateTime":20,"relativeEntities":517,"slug":20,"properties":518,"entityType":20,"verifyStatus":20,"verifyTime":20,"verifyNote":20,"languages":20,"translateLanguages":20,"viewCount":20,"url":20,"parentIds":521,"statistic":20},[],{"title":519},{"VI":520},"Wuhan National Laboratory for Optoelectronics, College of Optoelectronic Science and Engineering, Huazhong University of Science and Technology, Wuhan, China",[],{"title":523},{"VI":524},"Enming Xu",{"id":526,"sortIndex":58,"researcher":20,"roles":527,"affiliations":528,"properties":535,"displayName":537,"givenName":20,"familyName":20},"25fec234-3022-49d3-abdc-9b4a19f75ac9",[93],[529],{"id":515,"sortIndex":21,"affiliation":530,"properties":20},{"id":515,"createTime":20,"updateTime":20,"relativeEntities":531,"slug":20,"properties":532,"entityType":20,"verifyStatus":20,"verifyTime":20,"verifyNote":20,"languages":20,"translateLanguages":20,"viewCount":20,"url":20,"parentIds":534,"statistic":20},[],{"title":533},{"VI":520},[],{"title":536,"gsAuthor":538},{"VI":537},"Xinliang 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Huang",{"url":508,"publisher":610,"properties":636},{"id":6,"createTime":7,"updateTime":8,"relativeEntities":611,"slug":10,"properties":612,"entityType":18,"verifyStatus":19,"verifyTime":20,"verifyNote":20,"languages":20,"translateLanguages":20,"viewCount":21,"subjectFields":616,"manageAffiliations":617,"indexDatabases":618,"url":55,"thumbnailPath":20,"statistic":631,"gsStatistic":20,"type":62,"analyzePriority":20},[],{"issn":613,"title":614,"eissn":615},{"VOID":13},{"EN":15},{"VOID":17},[],[],[619,625],{"id":26,"indexDatabase":620,"url":37,"indexYears":38,"academicFieldIds":20,"indexDatabaseRanking":39},{"id":28,"createTime":20,"updateTime":20,"relativeEntities":621,"label":622,"description":623,"key":34,"publicationTags":624,"standard":20},[],{"EN":31,"VI":31},{"EN":31,"VI":33},[36],{"id":41,"indexDatabase":626,"url":54,"indexYears":20,"academicFieldIds":20,"indexDatabaseRanking":20},{"id":43,"createTime":20,"updateTime":20,"relativeEntities":627,"label":628,"description":629,"key":50,"publicationTags":630,"standard":20},[],{"EN":46,"VI":46},{"EN":48,"VI":49},[52,53],{"impactFactor":21,"impactFactorByYear":632,"i10Index":21,"i10IndexLast5Year":21,"totalPublication":58,"totalPublicationByYear":633,"totalCitation":21,"totalCitationByYear":634,"totalCitationPerPublication":21,"totalCitationPerPublicationByYear":635,"hindexLast5Year":21,"hindex":21},{},{"2012":58},{},{},{"pages":637,"volume":639},{"VOID":638},"403-406",{"VOID":640},"2",{"total":21,"publishYear":169,"statisticByYear":642},{},"2009-10-16",[52,36],{"id":646,"createTime":647,"updateTime":648,"relativeEntities":649,"slug":650,"properties":651,"entityType":84,"verifyStatus":85,"verifyTime":662,"verifyNote":87,"languages":20,"translateLanguages":20,"viewCount":21,"primaryUrl":663,"fullTextUrl":20,"authors":664,"publicationType":135,"publisherRelationship":680,"citationCount":21,"citationInfo":711,"publishDate":315,"publishYear":316,"citationAnalyzeStatus":19,"lastCitationAnalyze":648,"indexDatabases":713,"openAccess":20,"references":20,"isForceReanalyzing":174},"3072fd8a-bef1-4022-80c3-945511ffbeb1","2024-01-11T01:06:36.834+00:00","2026-05-16T13:47:49.897+00:00",[],"On-the-theory-of-temporal-aberrations-for-dynamic-electron-optics",{"abstract":652,"title":654,"gsPaper":656,"references":658,"doi":660},{"EN":653},"A new theory for temporal aberrations of dynamic optics by applying the direct integral method is put forward in the present paper. A new definition of temporal aberration is given, in which a certain initial energy of electron emission emitted from a photocathode along the axial direction √ɛ\n                           z1(0⩽√ɛ\n                           z1⩽√ɛ0max) was taken as a criterion. New expressions of the temporary aberration coefficients in integral forms for the electron optical imaging systems have been deduced. An electrostatic concentric spherical system model is used to test and verify expressions of the coefficients given by the “direct integral method” and “τ variation method”. The analytical solutions prove that both methods are correct and equivalent. Compared to the “τ variation method”, the direct integral method only needs to carry out the integral calculation for the three geometrical temporal aberration coefficients of the second order, which is more convenient and suitable for computation in the practical design. Finally, results of the study for the theory of temporal aberrations of electron optical imaging systems, from the point of view of methodology, have been elaborated.",{"EN":655},"On the theory of temporal aberrations for dynamic electron optics",{"VOID":657},"[\"2341803582134418141\"]",{"VOID":659},"Monastyrski M A, Schelev M Y. Theory of Temporal Aberrations of Cathode Lenses. Moscow: Lebedeev Institute of Physics, 1980 (in Russian)\nRecknagel A. Theorie des elektrisohen elecktronen miktroskops fur selbstrakler. Z Angew Physik, 1941, 117: 689–708 (in German)\nArtimovich L A. Electrostatic properties of emission systems. Bulletin of Academy of Sciences, USSR Physics Series, 1944, 8(6): 313–328 (in Russian)\nSavoisky Y K. Fanchenko S D. Physical foundation of electron-optical chronograph. Report of Academy of Sciences, USSR, 1956, 108(2): 218–221 (in Russian)\nCsorba I P. Chromatic aberration limited image transfer characteristics of image tube lenses of simple geometry. RCA Review, 1970, 31(3): 534–550\nZhou L W, Li Y, Zhang Z Q, et al. Test and verification of temporal aberration theory for electron optical imaging systems by an electrostatic concentric spherical system. Acta Physica Sinica, 2005, 54(8): 3597–3603 (in Chinese)\nZhou L W. Electron Optics with Wide Beam Focusing (Monograph). Beijing: Beijing Institute of Technology Press, 1993 (in Chinese)\nZhou L W, Ai K C, Pan S C. On aberration theory of cathode lenses with combined electromagnetic focusing. Acta Physica Sinica, 1983, 32(3), 376–392 (in Chinese)\nZhou L W. Electron optics of concentric spherical system composed of two electrodes. Focusing and Imaging of Wide Electron Beams—Selected Papers on Electron Optics. Beijing: Beijing Institute of Technology Press, 1994, 11–29 (in Chinese)\nXimen J. Electron-optical properties and aberration theory of combined immersion objectives. Acta Physica Sinica, 1957, 13(4): 339–356 (in Chinese)\nKulikov Y V, Monastyrski M A, Feiding H E. Aberration theory of third order of cathode lenses: aberrations of cathode lenses with combined electric and magnetic fields. Radiotechnics and Electronics, 1978, 23(1): 167–174\nXimen J, Zhou L W, Ai K C. Variation theory of aberrations in cathode lenses. Optik, 1983, 66: 19–34\nZhou L W, Li Y, Zhang Z Q, et al. On the theory of temporal aberrations for cathode lenses. Optik, 2005, 116(4): 175–184\nZhou L W, Li Y, Zhang Z Q, et al. Theory of temporal aberrations for electron optical imaging systems by “Direct Integral Method”. Acta Physica Sinica, 2005, 54(8): 3591–3596 (in Chinese)\nZhou L W, Li Y, Zhang Z Q, et al. On the theory of temporal aberrations for electron optical imaging systems by using “Direct Integral Method”. In: Proceedings of SPIE, 2005, 5580: 710–724\nRuska E. Zur fokussierbarkeit von kathoden-strahlbundeln grosser ausgangsquerchnitte. Z Angew Physik, 1993, 83(9): 684–687 (in German)\nSchagen P, Bruining H, Francken J C. A simple electrostatic electron-optical system with only one voltage. Philips Research Reports, 1952, 7(2): 119–130\nZhou L W. Electron optics of concentric spherical electromagnetic focusing systems. Advances in Electronics and Electron Physics, 1979, 52: 119–132\nZhou L W, Monastyrski M A, Schelev M Ya, et al. On the temporal aberration theory of electron optical imaging systems by “τ Variation Method”. Acta Electronica Sinica, 2006, 34(2): 193–197 (in Chinese)\nLai H L, Jin T J. Biography of K. Popper. Shijiazhuang: Hebei People Press, 1998 (in Chinese)",{"VOID":661},"10.1007\u002Fs12200-008-0001-9","2024-05-12T11:59:04.148+00:00","https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1007\u002Fs12200-008-0001-9",[665],{"id":666,"sortIndex":21,"researcher":20,"roles":667,"affiliations":668,"properties":677,"displayName":679,"givenName":20,"familyName":20},"2fd9d6d0-2dc2-42af-aac1-12c0d169d73b",[93],[669],{"id":670,"sortIndex":21,"affiliation":671,"properties":20},"d2349d79-5317-4d72-9aeb-0359ceda2cf5",{"id":670,"createTime":20,"updateTime":20,"relativeEntities":672,"slug":20,"properties":673,"entityType":20,"verifyStatus":20,"verifyTime":20,"verifyNote":20,"languages":20,"translateLanguages":20,"viewCount":20,"url":20,"parentIds":676,"statistic":20},[],{"title":674},{"VI":675},"Department of Optical Engineering, School of Information Science and Technology, Beijing Institute of Technology, Beijing, China",[],{"title":678},{"VI":679},"Liwei Zhou",{"url":663,"publisher":681,"properties":707},{"id":6,"createTime":7,"updateTime":8,"relativeEntities":682,"slug":10,"properties":683,"entityType":18,"verifyStatus":19,"verifyTime":20,"verifyNote":20,"languages":20,"translateLanguages":20,"viewCount":21,"subjectFields":687,"manageAffiliations":688,"indexDatabases":689,"url":55,"thumbnailPath":20,"statistic":702,"gsStatistic":20,"type":62,"analyzePriority":20},[],{"issn":684,"title":685,"eissn":686},{"VOID":13},{"EN":15},{"VOID":17},[],[],[690,696],{"id":26,"indexDatabase":691,"url":37,"indexYears":38,"academicFieldIds":20,"indexDatabaseRanking":39},{"id":28,"createTime":20,"updateTime":20,"relativeEntities":692,"label":693,"description":694,"key":34,"publicationTags":695,"standard":20},[],{"EN":31,"VI":31},{"EN":31,"VI":33},[36],{"id":41,"indexDatabase":697,"url":54,"indexYears":20,"academicFieldIds":20,"indexDatabaseRanking":20},{"id":43,"createTime":20,"updateTime":20,"relativeEntities":698,"label":699,"description":700,"key":50,"publicationTags":701,"standard":20},[],{"EN":46,"VI":46},{"EN":48,"VI":49},[52,53],{"impactFactor":21,"impactFactorByYear":703,"i10Index":21,"i10IndexLast5Year":21,"totalPublication":58,"totalPublicationByYear":704,"totalCitation":21,"totalCitationByYear":705,"totalCitationPerPublication":21,"totalCitationPerPublicationByYear":706,"hindexLast5Year":21,"hindex":21},{},{"2012":58},{},{},{"pages":708,"volume":710},{"VOID":709},"50-57",{"VOID":167},{"total":21,"publishYear":316,"statisticByYear":712},{},[52,36],{"id":715,"createTime":716,"updateTime":717,"relativeEntities":718,"slug":719,"properties":720,"entityType":84,"verifyStatus":85,"verifyTime":729,"verifyNote":87,"languages":20,"translateLanguages":20,"viewCount":21,"primaryUrl":730,"fullTextUrl":20,"authors":731,"publicationType":135,"publisherRelationship":760,"citationCount":21,"citationInfo":791,"publishDate":315,"publishYear":316,"citationAnalyzeStatus":19,"lastCitationAnalyze":717,"indexDatabases":793,"openAccess":20,"references":794,"isForceReanalyzing":174},"eb7f4f00-cc58-4915-8047-a9bfd345b14b","2024-01-05T11:26:34.346+00:00","2026-04-21T15:28:23.428+00:00",[],"Incident-angle-of-parallel-light-measurements-based-on-optical-vernier-principle",{"abstract":721,"title":723,"gsPaper":725,"doi":727},{"EN":722},"The incident angle of a parallel light beam is hard to measure accurately under the requirement of both high precision and large measurement range. A solution based on the optical vernier principle is presented, and a corresponding measuring device is given. Compared with the former method, the suggested apparatus realizes high accuracy in a larger measurement range. The experiments on the designed apparatus show a high precision of better than 0.02° in a measurement range of ±64° and the experimental results are in accordance with analytical results in theory. The invented apparatus can be widely used in many technical areas such as aerospace, precision measurement and automatic control.",{"EN":724},"Incident angle of parallel light measurements based on optical vernier principle",{"VOID":726},"[\"9969886146359693484\"]",{"VOID":728},"10.1007\u002Fs12200-008-0021-5","2024-04-30T18:37:56.232+00:00","https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1007\u002Fs12200-008-0021-5",[732,747],{"id":733,"sortIndex":21,"researcher":20,"roles":734,"affiliations":735,"properties":744,"displayName":746,"givenName":20,"familyName":20},"5c6c7aa3-cc99-40ef-9e06-ceab2fb23c01",[93],[736],{"id":737,"sortIndex":21,"affiliation":738,"properties":20},"2260c5d3-14ba-460b-8103-c917cd9ecdea",{"id":737,"createTime":20,"updateTime":20,"relativeEntities":739,"slug":20,"properties":740,"entityType":20,"verifyStatus":20,"verifyTime":20,"verifyNote":20,"languages":20,"translateLanguages":20,"viewCount":20,"url":20,"parentIds":743,"statistic":20},[],{"title":741},{"VI":742},"Department of Precision Instruments and Mechanology, Tsinghua University, Beijing, China",[],{"title":745},{"VI":746},"Feifan Chen",{"id":748,"sortIndex":58,"researcher":20,"roles":749,"affiliations":750,"properties":757,"displayName":759,"givenName":20,"familyName":20},"debba477-0781-47f5-9220-bc21a0ce62e8",[93],[751],{"id":737,"sortIndex":21,"affiliation":752,"properties":20},{"id":737,"createTime":20,"updateTime":20,"relativeEntities":753,"slug":20,"properties":754,"entityType":20,"verifyStatus":20,"verifyTime":20,"verifyNote":20,"languages":20,"translateLanguages":20,"viewCount":20,"url":20,"parentIds":756,"statistic":20},[],{"title":755},{"VI":742},[],{"title":758},{"VI":759},"Zhiwei Hong",{"url":730,"publisher":761,"properties":787},{"id":6,"createTime":7,"updateTime":8,"relativeEntities":762,"slug":10,"properties":763,"entityType":18,"verifyStatus":19,"verifyTime":20,"verifyNote":20,"languages":20,"translateLanguages":20,"viewCount":21,"subjectFields":767,"manageAffiliations":768,"indexDatabases":769,"url":55,"thumbnailPath":20,"statistic":782,"gsStatistic":20,"type":62,"analyzePriority":20},[],{"issn":764,"title":765,"eissn":766},{"VOID":13},{"EN":15},{"VOID":17},[],[],[770,776],{"id":26,"indexDatabase":771,"url":37,"indexYears":38,"academicFieldIds":20,"indexDatabaseRanking":39},{"id":28,"createTime":20,"updateTime":20,"relativeEntities":772,"label":773,"description":774,"key":34,"publicationTags":775,"standard":20},[],{"EN":31,"VI":31},{"EN":31,"VI":33},[36],{"id":41,"indexDatabase":777,"url":54,"indexYears":20,"academicFieldIds":20,"indexDatabaseRanking":20},{"id":43,"createTime":20,"updateTime":20,"relativeEntities":778,"label":779,"description":780,"key":50,"publicationTags":781,"standard":20},[],{"EN":46,"VI":46},{"EN":48,"VI":49},[52,53],{"impactFactor":21,"impactFactorByYear":783,"i10Index":21,"i10IndexLast5Year":21,"totalPublication":58,"totalPublicationByYear":784,"totalCitation":21,"totalCitationByYear":785,"totalCitationPerPublication":21,"totalCitationPerPublicationByYear":786,"hindexLast5Year":21,"hindex":21},{},{"2012":58},{},{},{"pages":788,"volume":790},{"VOID":789},"192-196",{"VOID":167},{"total":21,"publishYear":316,"statisticByYear":792},{},[52,36],[795,801,805,808,814,817,820,823,826],{"id":796,"text":797,"url":798,"identifiers":799},"4c68646b-0035-4279-8000-0006b275d4fa","Chen Feifan, Chen Yifeng. Two-axis micro sun sensor using optical nonlinear compensation. Journal of Tsinghua University (Science and Technology), 2004, 44(2): 197–200 (in Chinese)","https:\u002F\u002Flink.springer.com\u002F10.1007\u002Fs10440-022-00541-7",{"doi":800},"10.1007\u002Fs10440-022-00541-7",{"id":20,"text":802,"url":803,"identifiers":804},"Chum J, Vojta J, Base J, et al. A simple low cost digital sun sensor for micro-satellites. http:\u002F\u002Fwww.dlr.de\u002Fiaa.symp\u002FPortaldata\u002F49\u002FResources\u002Fdokumente\u002Farchiv4\u002FIAA-B4-1205P.pdf, 2004","http:\u002F\u002Fwww.dlr.de\u002Fiaa.symp\u002FPortaldata\u002F49\u002FResources\u002Fdokumente\u002Farchiv4\u002FIAA-B4-1205P.pdf",{},{"id":20,"text":806,"url":20,"identifiers":807},"de Boom C W. Sun sensors from TNO TPD. Delft: TNO TPD, 2003",{},{"id":809,"text":810,"url":811,"identifiers":812},"56b66cdf-14a5-4747-a7f5-fbe579c227bf","Buonocore M, Grassi M, Rufino G. APS-based miniature sun sensor for earth observation nanosatellites. Acta Astronautica, 4th IAA International Symposium on Small Satellites for Earth Observation, 2005, 56(1–2): 139–145","https:\u002F\u002Fwww.sciencedirect.com\u002Fscience\u002Farticle\u002Fpii\u002FS0094576504002929",{"doi":813},"10.1016\u002Fj.actaastro.2004.09.006",{"id":20,"text":815,"url":20,"identifiers":816},"Kouzmin V S, Cheremoukhin G S, Fedoseev V I. Miniature sun sensor. Proceedings of SPIE, 1996, 2739: 407–410",{},{"id":20,"text":818,"url":20,"identifiers":819},"Cai Shuzhang, Jing Fangsheng. Optical-Electrical Autocollimation and the Application. Beijing: China Metrology Publishing House, 1986 (in Chinese)",{},{"id":20,"text":821,"url":20,"identifiers":822},"Qin Shiqiao, Chen Yujiao, Su Yong, et al. High precision automatic angle measuring system. Instrument Technique and Sensor, 1999, (11): 13–15 (in Chinese)",{},{"id":20,"text":824,"url":20,"identifiers":825},"Cao Xuedong, Geng Lihong, Fan Tianquan. A new calibration apparatus for elevation angle of theodolite. Opto-Electronic Engineering, 1999, (S1): 135–138 (in Chinese)",{},{"id":20,"text":827,"url":20,"identifiers":828},"Pan Mengchun, Ren Yongyi, Mao Shengyong. The real-time detection of pose and control of laser guiding vehicle (LGV). Journal of National University of Defense Technology, 1994, 16(2): 34–37 (in Chinese)",{},{"id":830,"createTime":831,"updateTime":832,"relativeEntities":833,"slug":834,"properties":835,"entityType":84,"verifyStatus":85,"verifyTime":846,"verifyNote":87,"languages":20,"translateLanguages":20,"viewCount":21,"primaryUrl":847,"fullTextUrl":20,"authors":848,"publicationType":135,"publisherRelationship":864,"citationCount":20,"citationInfo":20,"publishDate":895,"publishYear":169,"citationAnalyzeStatus":896,"lastCitationAnalyze":897,"indexDatabases":898,"openAccess":20,"references":20,"isForceReanalyzing":174},"0a2dacda-3af5-494c-80e6-18c18ab13c88","2023-12-12T00:00:26.302+00:00","2026-03-16T01:32:30.150+00:00",[],"Propagation-properties-of-beams-generated-by-Gaussian-mirror-resonator-in-fractional-Fourier-transform-plane",{"abstract":836,"title":838,"gsPaper":840,"references":842,"doi":844},{"EN":837},"Based on the definition of the fractional Fourier transform (FRFT) and irradiance moments in the cylindrical coordinate system, the propagation expressions and kurtosis parameter of beams generated by Gaussian mirror resonator passing through the ideal fractional Fourier transformation systems are obtained. The propagation properties and kurtosis parametric characteristic of the beams in the FRFT plane are analyzed in detail. Some numerical examples are given to illustrate the analytical results. The influences of the fractional order on the intensity distribution and the kurtosis parameter of the beams are also investigated. The results show that the intensity distribution and the kurtosis parameter of the beams in the FRFT plane are closely related to the fractional order and beam parameters.",{"EN":839},"Propagation properties of beams generated by Gaussian mirror resonator in fractional Fourier transform plane",{"VOID":841},"[]",{"VOID":843},"Mendlovic D, Ozaktas H M. Fractional Fourier transforms and their optical implementation: I. Journal of the Optical Society of America A, 1993, 10(9): 1875–1881\nOzaktas H M, Mendlovic D. Fractional Fourier transforms and their optical implementation: II. Journal of the Optical Society of America A, 1993, 10(12): 2522–2531\nLohmann A W. Image rotation, Wigner rotation, and the fractional Fourier transform. Journal of the Optical Society of America A, 1993, 10(10): 2181–2186\nZhang Y, Dong B, Gu B, Yang G. Beam shaping in the fractional Fourier transform domain. Journal of the Optical Society of America A, 1998, 15(5): 1114–1120\nXue X, Wei H Q, Kirk A G. Beam analysis by fractional Fourier transform. Optics Letters, 2001, 26(22): 1746–1748\nLin Q, Cai Y. Fractional Fourier transform for partially coherent Gaussian-Schell model beams. Optics Letters, 2002, 27(19): 1672–1674\nCai Y, Lin Q. Fractional Fourier transform for elliptical Gaussian beams. Optics Communications, 2003, 217(1–6): 7–13\nCai Y, Lin Q. Properties of a flattened Gaussian beam in the fractional Fourier transform plane. Journal of Optics A: Pure and Applied Optics, 2003, 5(3): 272–275\nCai Y, Lin Q. Transformation and spectrum properties of partially coherent beams in the fractional Fourier transform plane. Journal of the Optical Society of America A, 2003, 20(8): 1528–1536\nCai Y, Ge D, Lin Q. Fractional Fourier transform for partially coherent and partially polarized Gaussian-Schell model beams. Journal of Optics A: Pure and Applied Optics, 2003, 5(5): 453–459\nCai Y, Lin Q. The fractional Fourier transform for a partially coherent pulse. Journal of Optics A: Pure and Applied Optics, 2004, 6(4): 307–311\nZhao D, Mao H, Liu H, Wang S, Jing F, Wei X. Propagation of Hermite-cosh-Gaussian beams in apertured fractional Fourier transforming systems. Optics Communications, 2004, 236(4–6): 225–235\nZhao D, Mao H, Zheng C, Wang S, Jing F, Wei X, Zhu Q, Liu H. The propagation properties and kurtosis parametric characteristics of Hermite-cosh-Gaussian beams passing through fractional Fourier transformation systems. Optik - International Journal for Light and Electron Optics, 2005, 116(10): 461–468\nZheng C. Fractional Fourier transform for a hollow Gaussian beam. Physics Letters A, 2006, 355(2): 156–161\nZheng C. Fractional Fourier transform for off-axis elliptical Gaussian beams. Optics Communications, 2006, 259(2): 445–448\nDu X, Zhao D. Fractional Fourier transform of truncated elliptical Gaussian beams. Applied Optics, 2006, 45(36): 9049–9052\nDu X, Zhao D. Fractional Fourier transforms of elliptical Hermite-cosh- Gaussian beams. Physics Letters A, 2007, 366(3): 271–275\nDu X, Zhao D. Fractional Fourier transform of off-axial elliptical cosh-Gaussian beams. Optik - International Journal for Light and Electron Optics, 2008, 119(8): 379–382\nZheng C. Fractional Fourier transform of an elliptical dark-hollow beam. Optics and Laser Technology, 2008, 40(4): 632–640\nZhou G. Fractional Fourier transform of a higher-order cosh-Gaussian beam. Journal of Modern Optics, 2009, 56(7): 886–892\nZhou G. Fractional Fourier transform of Lorentz-Gaussian beams. Journal of the Optical Society of America A, 2009, 26(2): 350–355\nChen S, Zhang T, Feng X. Propagation properties of cosh-squared-Gaussian beam through fractional Fourier transform systems. Optics Communications, 2009, 282(6): 1083–1087\nGaniel U, Hardy A. Eigenmodes of optical resonators with mirrors having Gaussian reflectivity profiles. Applied Optics, 1976, 15(9): 2145–2149\nMcCarthy N, Lavigne P. Optical resonators with Gaussian reflectivity mirrors: misalignment sensitivity. Applied Optics, 1983, 22(17): 2704–2708\nMcCarthy N, Lavigne P. Large-size Gaussian mode in unstable resonators using Gaussian mirrors. Optics Letters, 1985, 10(11): 553–555\nDeng D, Wei C, Yi K, Shao J, Fan Z, Tian Y. Propagation properties of beam generated by Gaussian mirror resonator. Optics Communications, 2006, 258(1): 43–50\nDeng D, Xia Z, Wei C, Shao J, Fan Z. Far-field intensity distribution, M 2 factor of beams generated by Gaussian mirror resonator. Optik — International Journal for Light and Electron Optics, 2007, 118(11): 533–536\nDeng D, Shen J, Tian Y, Shao J, Fan Z. Propagation properties of beams generated by Gaussian mirror resonator in uniaxial crystals. Optik — International Journal for Light and Electron Optics, 2007, 118(11): 547–551\nMartinez-Herrero R, Piquero G, Mejias P M. On the propagation of the kurtosis parameter of general beams. Optics Communications, 1995, 115(3–4): 225–232\nAmarande S A. Beam propagation factor and the kurtosis parameter of flattened Gaussian beams. Optics Communications, 1996, 129(5–6): 311–317",{"VOID":845},"10.1007\u002Fs12200-009-0074-0","2024-05-16T13:28:58.909+00:00","http:\u002F\u002Flink.springer.com\u002F10.1007\u002Fs12200-009-0074-0",[849],{"id":850,"sortIndex":21,"researcher":20,"roles":851,"affiliations":852,"properties":861,"displayName":863,"givenName":20,"familyName":20},"55d19889-0bcc-46f9-ab80-8547e290527f",[93],[853],{"id":854,"sortIndex":21,"affiliation":855,"properties":20},"e04cae04-c3cf-4011-832a-737cec23d212",{"id":854,"createTime":20,"updateTime":20,"relativeEntities":856,"slug":20,"properties":857,"entityType":20,"verifyStatus":20,"verifyTime":20,"verifyNote":20,"languages":20,"translateLanguages":20,"viewCount":20,"url":20,"parentIds":860,"statistic":20},[],{"title":858},{"VI":859},"School of Mathematics and Physics, Jiangsu Polytechnic University, Changzhou, China",[],{"title":862},{"VI":863},"Bin 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Zhang",{"VOID":956},"A5088141052",{"url":20,"publisher":958,"properties":20},{"id":6,"createTime":7,"updateTime":8,"relativeEntities":959,"slug":10,"properties":960,"entityType":18,"verifyStatus":19,"verifyTime":20,"verifyNote":20,"languages":20,"translateLanguages":20,"viewCount":21,"subjectFields":964,"manageAffiliations":965,"indexDatabases":966,"url":55,"thumbnailPath":20,"statistic":979,"gsStatistic":20,"type":62,"analyzePriority":20},[],{"issn":961,"title":962,"eissn":963},{"VOID":13},{"EN":15},{"VOID":17},[],[],[967,973],{"id":26,"indexDatabase":968,"url":37,"indexYears":38,"academicFieldIds":20,"indexDatabaseRanking":39},{"id":28,"createTime":20,"updateTime":20,"relativeEntities":969,"label":970,"description":971,"key":34,"publicationTags":972,"standard":20},[],{"EN":31,"VI":31},{"EN":31,"VI":33},[36],{"id":41,"indexDatabase":974,"url":54,"indexYears":20,"academicFieldIds":20,"indexDatabaseRanking":20},{"id":43,"createTime":20,"updateTime":20,"relativeEntities":975,"label":976,"description":977,"key":50,"publicationTags":978,"standard":20},[],{"EN":46,"VI":46},{"EN":48,"VI":49},[52,53],{"impactFactor":21,"impactFactorByYear":980,"i10Index":21,"i10IndexLast5Year":21,"totalPublication":58,"totalPublicationByYear":981,"totalCitation":21,"totalCitationByYear":982,"totalCitationPerPublication":21,"totalCitationPerPublicationByYear":983,"hindexLast5Year":21,"hindex":21},{},{"2012":58},{},{},{"total":123,"publishYear":985,"statisticByYear":986},2010,{"2015":58,"2018":58},"2010-06-01","2025-11-15T10:41:42.694+00:00",[52,36],[991,995,999,1003,1007,1011,1015,1019,1023,1027,1031,1035,1039,1043,1047],{"id":20,"text":992,"url":20,"identifiers":993},"Yao J P, Zeng F, Wang Q. Photonic generation of ultrawideband signals. Journal of Lightwave Technology, 2007, 25(11): 3219–3235",{"doi":994},"10.1109\u002FJLT.2007.906820",{"id":20,"text":996,"url":20,"identifiers":997},"Lin W P, Chen Y C. Design of a new optical impulse radio system for ultra-wideband wireless communications. IEEE Journal of Selected Topics in Quantum Electronics, 2006, 12(4): 882–887",{"doi":998},"10.1109\u002FJSTQE.2006.876613",{"id":20,"text":1000,"url":20,"identifiers":1001},"Wang Q, Zeng F, Blais S, Yao J P. Optical ultrawideband monocycle pulse generation based on cross-gain modulation in a semiconductor optical amplifier. Optics Letters, 2006, 31(21): 3083–3085",{"doi":1002},"10.1364\u002FOL.31.003083",{"id":20,"text":1004,"url":20,"identifiers":1005},"Zeng F, Yao J P. An approach to ultrawideband pulse generation and distribution over optical fiber. IEEE Photonics Technology Letters, 2006, 18(7): 823–825",{"doi":1006},"10.1109\u002FLPT.2006.871844",{"id":20,"text":1008,"url":20,"identifiers":1009},"Zeng F, Yao J P. Ultrawideband impulse radio signal generation using a high-speed electrooptic phase modulator and a fiber-Bragggrating-based frequency discriminator. IEEE Photonics Technology Letters, 2006, 18(19): 2062–2064",{"doi":1010},"10.1109\u002FLPT.2006.883310",{"id":20,"text":1012,"url":20,"identifiers":1013},"Chou J, Han Y, Jalali B. Adaptive RF-photonic arbitrary waveform generator. IEEE Photonics Technology Letters, 2003, 15(4): 581–583",{"doi":1014},"10.1109\u002FLPT.2003.809309",{"id":20,"text":1016,"url":20,"identifiers":1017},"Wang C, Zeng F, Yao J P. All-fiber ultrawideband pulse generation based on spectral-shaping and dispersion-induced frequency-to-time conversion. IEEE Photonics Technology Letters, 2007, 19(3): 137–139",{"doi":1018},"10.1109\u002FLPT.2006.888966",{"id":20,"text":1020,"url":20,"identifiers":1021},"Chen H, Chen M, Qiu C, Zhang J, Xie S. UWB monocycle pulse generation by optical polarisation time delay method. Electronics Letters, 2007, 43(9): 542–543",{"doi":1022},"10.1049\u002Fel:20070042",{"id":20,"text":1024,"url":20,"identifiers":1025},"Chen H, Chen M, Wang T, Li M, Xie S. Methods for ultra-wideband pulse generation based on optical cross-polarization modulation. Journal of Lightwave Technology, 2008, 26(15): 2492–2499",{"doi":1026},"10.1109\u002FJLT.2008.927616",{"id":20,"text":1028,"url":20,"identifiers":1029},"Dong J J, Zhang X L, Xu J, Huang D X, Fu S N, Shum P. Ultrawideband monocycle generation using cross-phase modulation in a semiconductor optical amplifier. Optics Letters, 2007, 32(10): 1223–1225",{"doi":1030},"10.1364\u002FOL.32.001223",{"id":20,"text":1032,"url":20,"identifiers":1033},"Dong J J, Zhang X L, Xu J, Huang D X. All-optical ultrawideband monocycle generation utilizing gain saturation of a dark return-to-zero signal in a semiconductor optical amplifier. Optics Letters, 2007, 32(15): 2158–2160",{"doi":1034},"10.1364\u002FOL.32.002158",{"id":20,"text":1036,"url":20,"identifiers":1037},"Dong J J, Zhang X L, Xu J, Huang D X, Fu S N, Shum P. High order ultrawideband pulse generation from NRZ-DPSK signals. In: Proceedings of National Fiber Optic Engineers Conference. 2008, JThA67",{"doi":1038},"10.1109\u002FOFC.2008.4528099",{"id":20,"text":1040,"url":20,"identifiers":1041},"Torres-Company V, Prince K, Monroy I T. Fiber transmission and generation of ultrawideband pulses by direct current modulation of semiconductor lasers and chirp-to-intensity conversion. Optics Letters, 2008, 33(3): 222–224",{"doi":1042},"10.1364\u002FOL.33.000222",{"id":20,"text":1044,"url":20,"identifiers":1045},"Li J Q, Fu S N, Xu K, Wu J, Lin J T, Tang M, Shum P. Photonic ultrawideband monocycle pulse generation using a single electrooptic modulator. Optics Letters, 2008, 33(3): 288–290",{"doi":1046},"10.1364\u002FOL.33.000288",{"id":20,"text":1048,"url":20,"identifiers":1049},"García Larrodé M, Koonen A M J, Vegas Olmos J J, Verdurmen E J M. Microwave signal generation and transmission based on optical frequency multiplication with a polarization interferometer. Journal of Lightwave Technology, 2007, 25(6): 1372–1378",{"doi":1050},"10.1109\u002FJLT.2007.895338",{"id":1052,"createTime":1053,"updateTime":1054,"relativeEntities":1055,"slug":1056,"properties":1057,"entityType":84,"verifyStatus":85,"verifyTime":1066,"verifyNote":87,"languages":20,"translateLanguages":20,"viewCount":21,"primaryUrl":1067,"fullTextUrl":20,"authors":1068,"publicationType":135,"publisherRelationship":1084,"citationCount":21,"citationInfo":1116,"publishDate":1119,"publishYear":1117,"citationAnalyzeStatus":19,"lastCitationAnalyze":1120,"indexDatabases":1121,"openAccess":20,"references":1122,"isForceReanalyzing":174},"04076162-74e5-4134-8081-23b825f9f2ca","2024-02-09T18:41:07.389+00:00","2025-09-11T17:13:39.647+00:00",[],"Temperature-effects-on-output-characteristics-of-quantum-dot-white-light-emitting-diode",{"abstract":1058,"title":1060,"gsPaper":1062,"doi":1064},{"EN":1059},"In this paper, we proposed quantum dot (QD) based structure for implementation of white light emitting diode (WLED) based on InGaN\u002FGaN. The proposed structure included three layers of InGaN QD with box shapes and GaN barriers. By using of single band effective mass method and considering strain effect, piezoelectric and spontaneous polarizations internal fields, then solving Schrödinger and Poisson equations self consistently, we obtained electron and hole eigen energies and wave functions. By evaluating dipole moment matrix elements for interband transitions, the output intensity was calculated due to the interband transition between two energy levels with highest emission probability. We adjusted QDs dimensions and material compositions so that the output light can be close to the ideal white light in chromaticity diagrams. Finally, effects of temperature variations on output spectrum and chromaticity coordinates were studied. We demonstrated that temperature variations in the range of 100 to 400 K decrease output intensity, broaden output spectral profile and cause a red shift in three main colors spectrums. This temperature variation deviates (x, y) are coordinated in the chromaticity diagram, but the output color still remains close to white.",{"EN":1061},"Temperature effects on output characteristics of quantum dot white light emitting diode",{"VOID":1063},"[\"16021070962115647712\"]",{"VOID":1065},"10.1007\u002Fs12200-012-0275-9","2024-05-04T07:04:52.634+00:00","https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1007\u002Fs12200-012-0275-9",[1069],{"id":1070,"sortIndex":21,"researcher":20,"roles":1071,"affiliations":1072,"properties":1081,"displayName":1083,"givenName":20,"familyName":20},"21349a74-7b91-4db4-9bdf-001b1e51e8eb",[93],[1073],{"id":1074,"sortIndex":21,"affiliation":1075,"properties":20},"861eb67a-412e-44da-84c8-e737290bf8e3",{"id":1074,"createTime":20,"updateTime":20,"relativeEntities":1076,"slug":20,"properties":1077,"entityType":20,"verifyStatus":20,"verifyTime":20,"verifyNote":20,"languages":20,"translateLanguages":20,"viewCount":20,"url":20,"parentIds":1080,"statistic":20},[],{"title":1078},{"VI":1079},"Faculty of Engineering, Islamic Azad University, Hamedan Branch, Hamedan, Iran",[],{"title":1082},{"VI":1083},"Amin Ranjbaran",{"url":1067,"publisher":1085,"properties":1111},{"id":6,"createTime":7,"updateTime":8,"relativeEntities":1086,"slug":10,"properties":1087,"entityType":18,"verifyStatus":19,"verifyTime":20,"verifyNote":20,"languages":20,"translateLanguages":20,"viewCount":21,"subjectFields":1091,"manageAffiliations":1092,"indexDatabases":1093,"url":55,"thumbnailPath":20,"statistic":1106,"gsStatistic":20,"type":62,"analyzePriority":20},[],{"issn":1088,"title":1089,"eissn":1090},{"VOID":13},{"EN":15},{"VOID":17},[],[],[1094,1100],{"id":26,"indexDatabase":1095,"url":37,"indexYears":38,"academicFieldIds":20,"indexDatabaseRanking":39},{"id":28,"createTime":20,"updateTime":20,"relativeEntities":1096,"label":1097,"description":1098,"key":34,"publicationTags":1099,"standard":20},[],{"EN":31,"VI":31},{"EN":31,"VI":33},[36],{"id":41,"indexDatabase":1101,"url":54,"indexYears":20,"academicFieldIds":20,"indexDatabaseRanking":20},{"id":43,"createTime":20,"updateTime":20,"relativeEntities":1102,"label":1103,"description":1104,"key":50,"publicationTags":1105,"standard":20},[],{"EN":46,"VI":46},{"EN":48,"VI":49},[52,53],{"impactFactor":21,"impactFactorByYear":1107,"i10Index":21,"i10IndexLast5Year":21,"totalPublication":58,"totalPublicationByYear":1108,"totalCitation":21,"totalCitationByYear":1109,"totalCitationPerPublication":21,"totalCitationPerPublicationByYear":1110,"hindexLast5Year":21,"hindex":21},{},{"2012":58},{},{},{"pages":1112,"volume":1114},{"VOID":1113},"284-291",{"VOID":1115},"5",{"total":21,"publishYear":1117,"statisticByYear":1118},2012,{},"2012-07-28","2025-09-11T17:13:39.646+00:00",[52],[1123,1126,1129,1135,1138,1141,1144,1147,1150,1153,1156,1159,1162,1165,1168,1174,1177,1180,1183,1186,1189,1192,1195,1198,1201],{"id":796,"text":1124,"url":798,"identifiers":1125},"Nakamura S, Mukai T, Senoh M. Candela-class high-brightness InGaN\u002FAIGaN double-heterostructure blue-light-emitting diodes. Applied Physics Letters, 1994, 64(13): 1687–1689",{"doi":800},{"id":796,"text":1127,"url":798,"identifiers":1128},"Nakamura S. Zn-doped InGaN growth and InGaN\u002FA1GaN doubleheterostructure blue-light-emitting diodes. Journal of Crystal Growth, 1994, 145(1–4): 911–917",{"doi":800},{"id":1130,"text":1131,"url":1132,"identifiers":1133},"20ae4601-fdb1-4456-bddf-3d9b2c907ad2","Vurgaftmana I, Meyer J R, Ram-Mohan L R. Band parameters for III–V compound semiconductors and their alloys. Journal of Applied Physics, 2001, 89(11): 5815–5875","https:\u002F\u002Fpubs.aip.org\u002Fjap\u002Farticle\u002F89\u002F11\u002F5815\u002F488612\u002FBand-parameters-for-III-V-compound-semiconductors",{"doi":1134},"10.1063\u002F1.1368156",{"id":796,"text":1136,"url":798,"identifiers":1137},"Wu J, Walukiewicz W, Yu K M, Ager J W, Haller E E, Lu H, Schaff W J. Small band gap bowing in In1 − x GaxN alloys. Applied Physics Letters, 2002, 80(25): 4741–4743",{"doi":800},{"id":796,"text":1139,"url":798,"identifiers":1140},"Piprek J. Nitride Semiconductor Devices: Principles and Simulation. NewYork: WILEY-VCH, 2007",{"doi":800},{"id":796,"text":1142,"url":798,"identifiers":1143},"Allen S C, Steck A J. A nearly ideal phosphor-converted white lightemitting diode. Applied Physics Letters, 2008, 92(14): 143309–143311",{"doi":800},{"id":796,"text":1145,"url":798,"identifiers":1146},"Xie R J, Hirosaki N, Kimura N, Sakuma K, Mitomo M. 2-phosphorconverted white light-emitting diodes using oxynitride\u002F nitride phosphors. Applied Physics Letters, 2007, 90(19): 191101–191103",{"doi":800},{"id":796,"text":1148,"url":798,"identifiers":1149},"Khoshnegar M, Sodagar M, Eftekharian A, Khorasani S. Design of a GaN white light-emitting diode through envelope function analysis. IEEE Journal of Quantum Electronics, 2010, 46(2): 228–237",{"doi":800},{"id":796,"text":1151,"url":798,"identifiers":1152},"Anikeeva P O, Halpert J E, Bawendi M G, Bulović V. Electroluminescence from a mixed red-green-blue colloidal quantum dot monolayer. Nano Letters, 2007, 7(8): 2196–2200",{"doi":800},{"id":796,"text":1154,"url":798,"identifiers":1155},"Schubert E F, Kim J K. Solid-state light sources getting smart. Science, 2005, 308(5726): 1274–1278",{"doi":800},{"id":796,"text":1157,"url":798,"identifiers":1158},"Chen C H, Su Y K, Sheu J K, Chen J F, Kuo C H, Lin Y C. Nitridebased cascade near white light-emitting diodes. IEEE Photonics Technology Letters, 2002, 14(7): 908–910",{"doi":800},{"id":796,"text":1160,"url":798,"identifiers":1161},"Ozden I, Makarona E, Nurmikko A V, Takeuchi T, Krames M. A dual-wavelength indium gallium nitride quantum well light emitting diode. Applied Physics Letters, 2001, 79(16): 2532–2534",{"doi":800},{"id":796,"text":1163,"url":798,"identifiers":1164},"Park K, Kwon M K, Cho C Y, Lim J H, Park S J. Phosphor-free white light-emitting diode with laterally distributed multiple quantum wells. Applied Physics Letters, 2008, 92(9): 091110–091112",{"doi":800},{"id":796,"text":1166,"url":798,"identifiers":1167},"Shei S C, Sheu J K, Tsai C M, Lai W C, Lee M L, Kuo C H. Emission mechanism of mixed-color InGaN\u002FGaN multi-quantumwell light-emitting diodes. Japanese Journal of Applied Physics, 2006, 45(4): 2463–2466",{"doi":800},{"id":1169,"text":1170,"url":1171,"identifiers":1172},"7b8ad286-26c6-40dd-8429-48be8696a42b","Rostami A, Rasooli Saghai H, Baghban Asghari Nejad H. A proposal for enhancement of optical nonlinearity in GaN\u002FAlGaN centered defect quantum box (CDQB) nanocrystal. Solid-State Electronics, 2008, 52(7): 1075–1108","https:\u002F\u002Fwww.sciencedirect.com\u002Fscience\u002Farticle\u002Fpii\u002FS0038110108000841",{"doi":1173},"10.1016\u002Fj.sse.2008.03.014",{"id":20,"text":1175,"url":20,"identifiers":1176},"Lai C Y, Hsu T M. Polarization field effect on group III-nitride semiconductors. Dissertation for the Doctoral Degree. Taiwan, China, 2003",{},{"id":20,"text":1178,"url":20,"identifiers":1179},"Winkelnkemper M, Schliwa A, Bimberg D. Interrelation of structural and electronic properties in InxGa1 − x N\u002FGaN quantum dots using an eight-band k·p model. Physical Review B: Condensed Matter and Materials Physics, 2006, 74(15): 155322–155333",{},{"id":796,"text":1181,"url":798,"identifiers":1182},"Wu Y R, Lin Y Y, Huang H H, Singh J. Electronic and optical properties of InGaN quantum dot based light emitters for solid state lighting. Applied Physics, 2009, 105: 13117–13123",{"doi":800},{"id":796,"text":1184,"url":798,"identifiers":1185},"Ranjan V, Allan G, Priester C, Delerue C. Self-consistent calculations of the optical properties of GaN quantum dots. Physical Review B: Condensed Matter and Materials Physics, 2003, 68(11): 115305–115311",{"doi":800},{"id":796,"text":1187,"url":798,"identifiers":1188},"Sakamoto A, Sugawara M. Theoretical calculation of lasing spectra of quantum-dot lasers: effect of homogeneous broadening of optical gain. IEEE Photonics Technology Letters, 2000, 12(2): 107–109",{"doi":800},{"id":796,"text":1190,"url":798,"identifiers":1191},"Sugawara M. Self-Assembled InGaAs\u002FGaAs Quantum Dots. London: Academic press, 1999",{"doi":800},{"id":796,"text":1193,"url":798,"identifiers":1194},"Asada M, Miyamoto Y, Suematsu Y. Gain and the threshold of three-dimensional quantum-box lasers. IEEE Journal of Quantum Electronics, 1986, QE-22(9): 1915–1921",{"doi":800},{"id":796,"text":1196,"url":798,"identifiers":1197},"Fairman H S, Brill M H, Hemmendinger H. How the CIE 1931 color-matching functions were derived from Wright-Guild data. Color Research and Application, 1998, 22(1): 11–23",{"doi":800},{"id":796,"text":1199,"url":798,"identifiers":1200},"Han D S, Asryan L V. Output power of a double tunneling-injection quantum dot laser. Nanotechnology, 2010, 21(1): 15201–15214",{"doi":800},{"id":20,"text":1202,"url":20,"identifiers":1203},"Schubert E F, Gessmann T, Kim J K. Light-Emitting Diodes. Cambridge: Cambridge University Press, 2003",{},{"id":1205,"createTime":1206,"updateTime":1207,"relativeEntities":1208,"slug":1209,"properties":1210,"entityType":84,"verifyStatus":85,"verifyTime":1223,"verifyNote":87,"languages":20,"translateLanguages":1224,"viewCount":21,"primaryUrl":1226,"fullTextUrl":20,"authors":1227,"publicationType":135,"publisherRelationship":1282,"citationCount":20,"citationInfo":20,"publishDate":1313,"publishYear":169,"citationAnalyzeStatus":19,"lastCitationAnalyze":20,"indexDatabases":1314,"openAccess":20,"references":20,"isForceReanalyzing":174},"46ce642c-ff14-4f5b-a8c4-2f9043faa1eb","2023-11-30T15:51:48.261+00:00","2025-02-26T20:52:23.069+00:00",[],"A-new-magnetic-sensor-with-Mach-Zehnder-Sagnac-optical-fiber-interferometer",{"abstract":1211,"title":1214,"keywords":1217,"references":1219,"doi":1221},{"EN":1212,"VI":1213},"This paper presents a new structure for magnetic sensor with Mach-Zehnder\u002FSagnac optical fiber interferometer. The magnetostrictive optical fiber sensor is placed in one of the two arms of the Mach-Zehnder interferometer, which can detect the optic phase shift by testing the length difference of the arm caused by environmental magnetic field. Because of forward and backward transmission in the arms, the Mach-Zehnder\u002FSagnac optical fiber interferometer can deduce twice exactly of the phase shift proportional to the length difference as Mach-Zehnder interferometer. Theoretically, description of the Mach-Zehnder\u002FSagnac interferometer is given, and some main issues in the magnetic field sensor with optical fiber interferometer are demonstrated with experiments. The magnetic sensors are implemented using the proposed methods.","Bài báo này giới thiệu một cấu trúc mới cho cảm biến từ tính sử dụng giao thoa kế sợi quang Mach-Zehnder\u002FSagnac. Cảm biến sợi quang có tính từ trở được đặt trong một trong hai nhánh của giao thoa kế Mach-Zehnder, có khả năng phát hiện độ dịch pha quang bằng cách kiểm tra sự khác biệt chiều dài của nhánh do trường từ trường môi trường gây ra. Nhờ vào việc truyền đi và truyền về trong các nhánh, giao thoa kế sợi quang Mach-Zehnder\u002FSagnac có thể luận suy chính xác gấp đôi độ dịch pha tỷ lệ với sự khác biệt chiều dài như giao thoa kế Mach-Zehnder. Về lý thuyết, mô tả về giao thoa kế Mach-Zehnder\u002FSagnac được đưa ra, và một số vấn đề chính trong cảm biến trường từ với giao thoa kế sợi quang được chứng minh thông qua thí nghiệm. Các cảm biến từ tính được thực hiện sử dụng các phương pháp đã đề xuất.",{"EN":1215,"VI":1216},"A new magnetic sensor with Mach-Zehnder\u002FSagnac optical fiber interferometer","Cảm biến từ mới với giao thoa kế sợi quang Mach-Zehnder\u002FSagnac",{"VI":1218},"Cảm biến từ tính, giao thoa kế sợi quang Mach-Zehnder\u002FSagnac, độ dịch pha quang, cảm biến sợi quang",{"VOID":1220},"Kirkendall C K, Dandridge A. Overview of high performance fibreoptic sensing. Journal of Physics D: Applied Physics, 2004, 37(18): 197–216\nDagenais DM, Bucholtz F, Koo K P, Dandridge A. Demonstration of 3 pT\u002FHz1\u002F2 at 10 Hz in a fibre-optic magnetometer. Electronics Letters, 1988, 24(23): 1422–1423\nBucholtz F, Dagenais D M, Koo K P. High-frequency fibre-optic magnetometer with 70 fT\u002FHz1\u002F2 resolution. Electronics Letters, 1989, 25(25): 1719–1721\nShi C H, Chen J P, Li X W, Ye A L, Zhou J H. Directivity of the magnetostrictive fiber-optic interferometric transducers. IEEE Sensors Journal, 2006, 6(5): 1191–1194\nWang X, Chen S, Du Z, Wang X, Shi C, Chen J. Experimental study of some key issues on fiber-optic interferometric sensors detecting weak magnetic field. IEEE Sensors Journal, 2008, 8(7): 1173–1179\nHuang Y L, Dong X F. Research on dual-pass Mach-Zehnder interferometer filters. Laser Journal, 2006, 27(6): 47–48 (in chinese)\nChow J H, Littler I C M, McClelland D E, Gray M B. Backscatter immune Mach-Zehnder-Sagnac hybrid interferometric sensor. Proceedings of SPIE, 2008, 7004: 1–4\nChow J H, McClelland D E, Gray M B. Backscatter immune, polarization managed, all fiber Sagnac sensing interferometer. 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