Littérature scientifique sur le sujet « DISPERSION FLATTENED »
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Articles de revues sur le sujet "DISPERSION FLATTENED"
NAKAJIMA, Kazuhide, et Takashi MATSUI. « Dispersion-Flattened Photonic Crystal Fiber ». Review of Laser Engineering 34, no 1 (2006) : 17–21. http://dx.doi.org/10.2184/lsj.34.17.
Texte intégralAl-Qdah, M. T. « Employing dispersion-flattened fiber for chromatic dispersion measurement ». Optical Engineering 45, no 5 (1 mai 2006) : 055005. http://dx.doi.org/10.1117/1.2205828.
Texte intégralHeusinger, Martin, Thomas Flügel-Paul, Kevin Grabowski, Dirk Michaelis, Stefan Risse et Uwe D. Zeitner. « High-dispersion TIR-GRISMs with flattened angular dispersion profile ». Optica 9, no 4 (11 avril 2022) : 412. http://dx.doi.org/10.1364/optica.427652.
Texte intégralGuo, Yuhao, Zeinab Jafari, Anu M. Agarwal, Lionel C. Kimerling, Guifang Li, Jurgen Michel et Lin Zhang. « Bilayer dispersion-flattened waveguides with four zero-dispersion wavelengths ». Optics Letters 41, no 21 (24 octobre 2016) : 4939. http://dx.doi.org/10.1364/ol.41.004939.
Texte intégralAbdur Razzak, S. M., Y. Namihira et F. Begum. « Ultra-flattened dispersion photonic crystal fibre ». Electronics Letters 43, no 11 (2007) : 615. http://dx.doi.org/10.1049/el:20070558.
Texte intégralSurvaiya, S. P., et R. K. Shevgaonkar. « Design of subpicosecond dispersion-flattened fibers ». IEEE Photonics Technology Letters 8, no 6 (juin 1996) : 803–5. http://dx.doi.org/10.1109/68.502100.
Texte intégralZhang, Lin, Yang Yue, Raymond G. Beausoleil et Alan E. Willner. « Flattened dispersion in silicon slot waveguides ». Optics Express 18, no 19 (10 septembre 2010) : 20529. http://dx.doi.org/10.1364/oe.18.020529.
Texte intégralYu, M., C. J. McKinstrie et Govind P. Agrawal. « Modulational instabilities in dispersion-flattened fibers ». Physical Review E 52, no 1 (1 juillet 1995) : 1072–80. http://dx.doi.org/10.1103/physreve.52.1072.
Texte intégralSafaai-Jazi, A., et H. T. Hattori. « Large-effective-area dispersion-flattened fiber ». Microwave and Optical Technology Letters 16, no 6 (20 décembre 1997) : 327–28. http://dx.doi.org/10.1002/(sici)1098-2760(19971220)16:6<327 ::aid-mop1>3.0.co;2-m.
Texte intégralIslam, Raonaqul, Shubi Felix Kaijage et Sohel Rana. « Low-loss and dispersion flattened terahertz fiber ». Optik 229 (mars 2021) : 166293. http://dx.doi.org/10.1016/j.ijleo.2021.166293.
Texte intégralThèses sur le sujet "DISPERSION FLATTENED"
Reeves, William Henry. « Photonic crystal fibre : the ultra-flattened dispersion regime ». Thesis, University of Bath, 2003. https://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.275816.
Texte intégralCHU, SHU-HAN, et 朱書漢. « Dispersion Flattened / Polarization Maintaining Photonic Crystal Fibers ». Thesis, 2018. http://ndltd.ncl.edu.tw/handle/8etq76.
Texte intégral國立聯合大學
光電工程學系碩士班
106
Chromatic dispersion in single mode fibers (SMFs) may induce temporal optical pulse broadening; result in serious restrictions in transmission data rates in high-speed optical fiber communication systems. In order to use wavelength band effectively in communication systems, a characteristic of nearly zero flattened dispersion in broadband is desirable to avoid pulse broadening and increase transmission rate. Therefore, there had many studies of dispersion flattened fiber (DFF) published in the past time. In addition, in the fabrication process of conventional optical fiber, an asymmetry of the fiber shape, impurities contained in fiber; and in fiber installment construction, the banding and wiring stress ; these all may result in polarization modal dispersion (PMD). To reduce the transmission rate limited by PMD, many scholars had contributed to articles of polarization maintaining fibers (PMF). In order to reduce excessive loss and poor matching between two kind of fiber, this study merged the functions of DFF and PMF in one fiber, and designed a dual function of dispersion flattened and polarization maintaining fiber based on a photonic crystal fiber (DF/PM PCF). This study used the dispersion slope matching method to design a photonic crystal fiber with broadband nearly zero flattened dispersion and polarization maintain characteristics.
Chen, Yong-yu, et 陳詠裕. « A Study of Liquid-filled Dispersion-flattened Photonic Crystal Fiber ». Thesis, 2009. http://ndltd.ncl.edu.tw/handle/66721740160767554677.
Texte intégral國立聯合大學
光電工程學系碩士班
98
Photonic Crystal Fiber ( PCF ) is a novel fiber’s structure, which has more outstanding performance than traditional fiber has on the optic characteristics. In general, photonic crystal fiber can be classified into two types. The first one guides light by a principle of “ modified total internal reflection ( MTIR ) ”, which is named as “ Index-guiding Photonic Crystal Fiber ”. The other type of PCF guides light in the photonic band gap which is caused by its periodic structure. This kind of fiber is known as “ photonic band gap fiber ” because its light-guidance complies with photonic band gap effect. In this thesis, we will design an ultra-flatten dispersion fiber based on “ Index-guiding Photonic Crystal Fiber ” by using plane wave expansion ( PWE ) method ( BandSOLVE by RSoft Incorporated ). The material dispersion of a photonic crystal fiber is computed firstly, and then we simulate several PCF structures which fill some liquid of different index in specific cladding holes. To achieve nearly-zero dispersion of the fiber in ultra-wide band, we design the liquid-filled PCF structure deliberately and nullify the waveguide dispersion and material dispersion in the band as wide as possible. Finally, a liquid-filled PCF with ultra-flatten dispersion is designed, which with dispersion of ±1( ps/km-nm) from 1.28μm to 1.74μm is numerically demonstrated.
KHAMARU, AKASH, et KAJAL SHARMA. « MID-IR SUPERCONTINUUM GENERATION IN DISPERSION FLATTENED AS38SE62 CHALCOGENIDE PHOTONIC CRYSTAL FIBER ». Thesis, 2022. http://dspace.dtu.ac.in:8080/jspui/handle/repository/19530.
Texte intégralHuang, Kuo-Ming, et 黃國民. « The dispersion compensation and gain flattened in 4×10 GHz RZ transmission system by using Raman amplifier with DCF and FBGs ». Thesis, 2008. http://ndltd.ncl.edu.tw/handle/71004347591704217894.
Texte intégral國立東華大學
光電工程研究所
96
Since the wavelength dependence of the dispersion in the fiber, the signals of different channels suffer different dispersion, a single bare dispersion-compensated fiber (DCF) cannot compensate for the dispersion of all channels in an optical wavelength division multiplex (WDM) transmission system. However, the chromatic dispersion by which the different wavelength produces must compensate individually, and after long distance transmission the signal energy would decay significantly and must be individually amplified. Although progress in the optical fiber technology had led to the high density wavelength division multiplex (DWDM) transmission, it was still unable regarding the original WDM shortcoming to overcome completely. However the traditional compensation technology still had to penetrate parts, such as optical filter, optical coupler, which constitute a complicated compensation system. Therefore, we proposed in this thesis a new dispersion slope compensator that can simultaneously carry on the chromatic dispersion compensation and the gain-flattening to the DWDM system. This research is also the first experimental demonstration to realize this aspect. An optical gain flattening and double-pass chromatic dispersion compensation system is proposed, the main discussion is under the linear system. We select four wavelengths in C-band to take the DWDM channel and carry on the chromatic dispersion compensation and the gain-flattening in view of the 50km single mode fiber (SMF) optic transmission. We used 4×10GHz electroabsorption modulators integrated distributed feedback laser diode (EA-DFB LD) as the light source, the transmission 50km SMF has the total chromatic dispersion value of 800ps/nm. We used fiber Bragg gratings (FBG’s) to reflect the different channel pulses at different positions for the accumulated dispersion and flatten the signal gain by Raman amplifier (RA) in WDM system. The used pump wavelengths for RA were 1420nm, 1435nm, 1450nm and 1480nm. In the penetration way back and forth compensates two mechanisms, the profile may reply the close primitive optical signals in the time domain full width at half maximum (FWHM), the extinction ratio still held about 10dB, the signals still possess the same central frequencies with their energies restore to the original ones because of the flattened gain. This experimental characteristic lies in the penetration light circulator and the FBG’s having two chromatic dispersion compensations and two Raman gains in the DCF that reduces the DCF length effectively and simultaneously reduces complexity of compensation construction and compensation cost. Besides it is suitable in the RZ transmission system, it will also suitable in the NRZ transmission system as a convenient and effective compensation technology for the high speed and the high bandwidth DWDM system transmission.
Jian, You-Ren, et 簡佑任. « Design of Broad Band and Gain Flattened Dispersion Compensating Raman/Erbium Doped Fiber Hybrid Amplifiers with All-Optical Gain-Clamped for WDM Systems ». Thesis, 2008. http://ndltd.ncl.edu.tw/handle/76832515025912033936.
Texte intégral國立東華大學
光電工程研究所
96
In this thesis, we design dispersion-compensated Raman/erbium-doped fiber hybrid amplifiers recycling residual Raman pump for wavelength-division multiplexing (WDM) systems. The hybrid amplifiers system only require single Raman pump source. The experimental results showed that the hybrid amplifiers scheme have net gain of more than 17 dB which provide gain bandwidth over 70 nm from 1525 to 1595 nm for input signal power of -20 dBm. Compared with the conventional dispersion-compensated Raman amplifiers (DCRA), the net gain increases 4.36 dB and the gain bandwidth broadens 50 nm. Besides, there is no significant increase of noise figure (NF) in our experimental setup. The NF is about 6.79 dB. In order to increase gain bandwidth and to flatten gain of the hybrid amplifiers. We used multiple wavelengths Raman pump units to pump the Raman fiber amplifiers. The gain ripple of less than ±1.47 dB can be achieved over 65 nm from 1525 to 1590 nm by the optimal combination of pump wavelength at 1435 and 1480 nm. The gain bandwidth is over 80 nm at a wavelength range of 1520 to 1600 nm. The net gain and NF are 20.01 dB and 5.74 dB for input signal power of -20 dBm, respectively. The all-optical gain clamped technique is a simple and effective way to achieve constant gain characteristics regardless of input signal power variations. To our knowledge, this is the first experimentally demonstration gain-clamped broad band and gain flattened dispersion-compensated Raman/erbium-doped fiber hybrid amplifiers by recycling residual Raman pump with only using a single FBG for WDM systems. The optimum gain clamped wavelength is 1564 nm. The gain variation of less than 0.21 dB can be achieved over 100 nm from 1525 to 1625 nm and the dynamic signal input exceed 18 dBm ranging from -20 to -2 dBm. Besides, the gain ripple of less than ±1.75 dB is achievable over 65 nm from 1530 to 1595 nm. The gain bandwidth is over 80 nm from 1520 to 1600 nm. This hybrid amplifiers system has the advantages of the high transmission capacity, high gain, low noise, broad gain bandwidth, high flattened gain and large dynamic range of input power.
Wen, Yu-Hsiang, et 溫裕翔. « The Study of Broadband and Gain Flatten double-pass Raman Amplifier in Dispersion Compensating Fiber using Multi-Wavelength Pumping and Residual Pump Power for Increased Efficiency ». Thesis, 2009. http://ndltd.ncl.edu.tw/handle/19147554517217888996.
Texte intégral國立東華大學
電機工程學系
97
In this thesis, because the short dispersion compensation fiber (DCF) length reduces the amount of available gain for a given amount of pump power in the double-pass dispersion compensation Raman amplifier (double-pass DCRA), we proposed double-pass DCRA with pump-reflector. The circulator loop composed of an optical circulator used as pump-reflector so as to recycle residual Raman pump for increase efficiency of the system. When input signal is -25dBm at 1550nm, Raman pump is 260mW at 1450nm, the net gain of the backward pumping double-pass DCRA increased 3.09 dB form 10.49 dB to 13.58 dB and NF decrease 0.35 dB form 7.18 dB to 6.83 dB by adding circulator loop. In addition, the forward pumping double-pass DCRA also increased 3.09 dB form 11.24 dB to 14.33 dB and NF decrease 0.3 dB form 6.55 dB to 6.25 dB by adding circulator loop. We successfully showed that the net gain can be increase and NF decrease of the double-pass DCRA by recycling residual Raman pump. Next, we compared the measured results of the backward pumping scheme with the forward pumping scheme, the net gain of the forward pumping scheme is higher than that backward pumping scheme about 0.75dB with the same components. In addition, the NF of the forward pumping scheme is lower than that backward pumping scheme about 0.58dB. We experimentally demonstrated that the proposed forward pumping scheme is better than the backward pumping scheme form the aspect of Raman gain and NF. And then, we applied the forward pumping double-pass DCRA with pump-reflector into the WDM system further. We compare the measured results of forward multi-pumping scheme with and without circulator loop. When the input signal power level of -25dBm, the results showed overall net gain increase 2.31dB, noise figure decrease 0.36dB and the gain ripple maintain less than ±0.81dB in the gain bandwidth of 52nm form 1533nm to 1585nm just by using 3 wavelength channels Raman pump including 1435nm, 1450nm and 1480nm. In addition, in the same gain bandwidth of 52nm, the proposed forward pumping scheme applied here is also better than the backward pumping scheme because the net gain is 0.59dB higher and the NF is 0.8dB lower with gain ripple ±0.81dB. Finally, we discussed the effects of double Rayleigh scattering/double Rayleigh back scattering (DRS/DRBS) on the above proposed structure by means of modified time-domain extinction method (MTEM). For the forward pumping double-pass DCRA, the multi-path interference (MPI) noise of with circulator loop scheme is lower than that of without circulator loop scheme.
Chapitres de livres sur le sujet "DISPERSION FLATTENED"
Weik, Martin H. « dispersion-flattened optical fiber ». Dans Computer Science and Communications Dictionary, 433. Boston, MA : Springer US, 2000. http://dx.doi.org/10.1007/1-4020-0613-6_5292.
Texte intégralKarak, Anup, et Sanchita Pramanik. « Analysis and Dispersion Engineering for Generation of Ultra-flattened Dispersion in Photonic Crystal Fibers ». Dans Advances in Computer, Communication and Control, 185–95. Singapore : Springer Singapore, 2019. http://dx.doi.org/10.1007/978-981-13-3122-0_18.
Texte intégralKaur, Amritveer, Julie Devi, Ritu Sharma, Varshali Sharma et Santosh Chaudhary. « Design of Octagonal and Decagonal Lattice Photonic Crystal Fiber for Achieving Ultra Low Flattened Dispersion ». Dans Lecture Notes in Electrical Engineering, 39–49. Singapore : Springer Singapore, 2018. http://dx.doi.org/10.1007/978-981-10-7395-3_5.
Texte intégralDevi, Julie, Amritveer Kaur, Ritu Sharma, Varshali Sharma et Santosh Chaudhary. « Design and Analysis of Spiral Photonic Crystal Fiber for Ultra-Flattened Dispersion for C+L+U ». Dans Lecture Notes in Electrical Engineering, 21–28. Singapore : Springer Singapore, 2018. http://dx.doi.org/10.1007/978-981-10-7395-3_3.
Texte intégralCai, Yi-Jun, Shu-Han Chu et Jui-Ming Hsu. « Ultra-broadband dispersion-flattened/polarization-maintaining photonic-crystal fiber ». Dans Engineering Innovation and Design, 30–36. CRC Press, 2019. http://dx.doi.org/10.1201/9780429019777-6.
Texte intégralActes de conférences sur le sujet "DISPERSION FLATTENED"
BHAGAVATULA, V. A. « Dispersion-shifted and dispersion-flattened single-mode designs ». Dans Optical Fiber Communication Conference. Washington, D.C. : OSA, 1986. http://dx.doi.org/10.1364/ofc.1986.wf1.
Texte intégralHeusinger, M., T. Flügel-Paul, K. Grabowski, D. Michaelis et U. D. Zeitner. « High dispersive TIR-GRISMs with flattened angular dispersion profile ». Dans Optics and Photonics for Sensing the Environment. Washington, D.C. : OSA, 2020. http://dx.doi.org/10.1364/es.2020.em2c.7.
Texte intégralMalheiros-Silveira, G. N., J. A. Mores-Jr, E. F. Chillcce, H. E. Hernández-Figueroa et H. L. Fragnito. « Tellurite Based PCF with Flattened Dispersion ». Dans Latin America Optics and Photonics Conference. Washington, D.C. : OSA, 2010. http://dx.doi.org/10.1364/laop.2010.we30.
Texte intégralLucki, M. « Photonic crystal fiber with flattened dispersion ». Dans SPIE Optics + Optoelectronics, sous la direction de Francesco Baldini, Jiri Homola, Robert A. Lieberman et Kyriacos Kalli. SPIE, 2011. http://dx.doi.org/10.1117/12.886807.
Texte intégralLiao, Meisong, ZhongChao Duan, Weiqing Gao, Xin Yan, Takenobu Suzuki et Yasutake Ohishi. « A dispersion flattened tellurite composite holey fiber ». Dans SPIE OPTO, sous la direction de Shibin Jiang, Michel J. F. Digonnet et J. Christopher Dries. SPIE, 2012. http://dx.doi.org/10.1117/12.905737.
Texte intégralChavez Boggio, J. M., D. Bodenmueller, T. Fremberg, R. Haynes, M. M. Roth, R. Eisermann, L. Zimmermann et M. Bohm. « Silicon nitride waveguide with flattened chromatic dispersion ». Dans SPIE Optics + Optoelectronics. SPIE, 2013. http://dx.doi.org/10.1117/12.2017302.
Texte intégralHuang, Guan-Ru, et Jui-Ming Hsu. « Liquid-filled dispersion-flattened photonic crystal fiber ». Dans 2017 International Conference on Applied System Innovation (ICASI). IEEE, 2017. http://dx.doi.org/10.1109/icasi.2017.7988176.
Texte intégralChu, Shu-Han, et Jui-Ming Hsu. « Dispersion flattened / polarization maintaining photonic crystal fiber ». Dans 2018 IEEE International Conference on Applied System Innovation (ICASI). IEEE, 2018. http://dx.doi.org/10.1109/icasi.2018.8394440.
Texte intégralGao, Yangsheng. « Parametric study for low loss dispersion-flattened fibers ». Dans OSA Annual Meeting. Washington, D.C. : Optica Publishing Group, 1992. http://dx.doi.org/10.1364/oam.1992.thww4.
Texte intégralFerrando, Albert, J. J. Miret, Enrique Silvestre-Mora, Miguel V. Andres, Pedro Andres et Philip S. Russell. « Designing a photonic crystal fiber with flattened dispersion ». Dans ICO XVIII 18th Congress of the International Commission for Optics, sous la direction de Alexander J. Glass, Joseph W. Goodman, Milton Chang, Arthur H. Guenther et Toshimitsu Asakura. SPIE, 1999. http://dx.doi.org/10.1117/12.354920.
Texte intégral