Bibliografías temáticas / CW supercontinuum

Literatura académica sobre el tema "CW supercontinuum"

Autor: Grafiati
Publicado: 6 de septiembre de 2023

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Artículos de revistas sobre el tema "CW supercontinuum"

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Kudlinski, Alexandre y Arnaud Mussot. "Visible cw-pumped supercontinuum". Optics Letters 33, n.º 20 (15 de octubre de 2008): 2407. http://dx.doi.org/10.1364/ol.33.002407.

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Guo, C. Y., S. C. Ruan, P. G. Yan, H. F. Wei, Z. C. Chen, D. Q. Ouyang, H. Q. Lin y X. J. Hu. "A low-cost CW-pumped supercontinuum source". Laser Physics 23, n.º 5 (10 de abril de 2013): 055403. http://dx.doi.org/10.1088/1054-660x/23/5/055403.

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Cumberland, B. A., J. C. Travers, S. V. Popov y J. R. Taylor. "29 W High power CW supercontinuum source". Optics Express 16, n.º 8 (11 de abril de 2008): 5954. http://dx.doi.org/10.1364/oe.16.005954.

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Yang, Jinhui, Huaiqin Lin, Shuangchen Ruan, Yiming Wu, Deqin Ouyang, Jinhui Yang, Huifeng Wei y Xuejuan Hu. "High-power all-fiber CW-pumped supercontinuum source". JOURNAL OF SHENZHEN UNIVERSITY SCIENCE AND ENGINEERING 30, n.º 4 (29 de noviembre de 2013): 423–27. http://dx.doi.org/10.3724/sp.j.1249.2013.04423.

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5

Kobtsev, S. M. y S. V. Smirnov. "Supercontinuum fiber sources under pulsed and CW pumping". Laser Physics 17, n.º 11 (noviembre de 2007): 1303–5. http://dx.doi.org/10.1134/s1054660x07110059.

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Larsen, C., S. T. Sørensen, D. Noordegraaf, K. P. Hansen, K. E. Mattsson y O. Bang. "Zero-dispersion wavelength independent quasi-CW pumped supercontinuum generation". Optics Communications 290 (marzo de 2013): 170–74. http://dx.doi.org/10.1016/j.optcom.2012.10.030.

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Mussot, A., A. Kudlinski, M. Kolobov, E. Louvergneaux, M. Douay y M. Taki. "Observation of extreme temporal events in CW-pumped supercontinuum". Optics Express 17, n.º 19 (9 de septiembre de 2009): 17010. http://dx.doi.org/10.1364/oe.17.017010.

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8

Xu, Xing, Chi Zhang, T. I. Yuk, Kevin K. Tsia y Kenneth K. Y. Wong. "Stabilized Wide-Band Wavelength Conversion Enabled by CW-Triggered Supercontinuum". IEEE Photonics Technology Letters 24, n.º 20 (octubre de 2012): 1886–89. http://dx.doi.org/10.1109/lpt.2012.2218099.

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Kudlinski, Alexandre, GÉraud Bouwmans, Marc Douay, Majid Taki y Arnaud Mussot. "Dispersion-Engineered Photonic Crystal Fibers for CW-Pumped Supercontinuum Sources". Journal of Lightwave Technology 27, n.º 11 (junio de 2009): 1556–64. http://dx.doi.org/10.1109/jlt.2009.2015966.

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Kobtsev, S. M. y S. V. Smirnov. "Temporal structure of a supercontinuum generated under pulsed and CW pumping". Laser Physics 18, n.º 11 (noviembre de 2008): 1260–63. http://dx.doi.org/10.1134/s1054660x08110091.

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Tesis sobre el tema "CW supercontinuum"

1

Song, Yue. "Ultra wideband CW pumped optical supercontinuum source". Thesis, 2007. http://spectrum.library.concordia.ca/975596/1/MR40898.pdf.

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Optical supercontinuum (OSC) laser source is a new generation wideband laser which has various commercial applications such as telecommunication, biomedicine, and optical sensing systems. However the high costs of current OSC laser sources generally have impeded them to be used more widely. In this thesis, we demonstrated a low-cost OSC laser source based on a continuum wave (CW) pumped Erbium/Ytterbium co-doped fiber (EYCDF) ring cavity with a 1.2 km highly nonlinear fiber (HNLF). This OSC laser source has 350nm spectral coverage, from 1550nm to 1900nm in wavelength. This is the first CW pumped OSC that generates continuum spectrum above 1750nm. The wide spectral coverage in the long wavelength range allows more advanced utilization of OSC sources. In this thesis, the evolution mechanism of the CW pumped OSC is discussed. The analysis of the results shows that self-phase modulation (SPM), and stimulated Raman scattering (SRS) dominate the evolution of OSC. Therefore, the evolution pattern is different to those of previous CW pumped OSCs where the modulation instability (MI) and SRS effects, or purely SRS effect dominate OSC generation. In addition, the experimental results suggest that the OSC generated by this evolution pattern has high flatness, which is caused by two reasons. Firstly, the intense SRS effect suppresses the MI effect, which could induce spectral vibration. Secondly, SPM induced spectrum broadening produce a smooth spectrum. The intense SPM and SRS effect are benefited from the ring-cavity structure which effectively increases the effective length of nonlinear fiber. Keyword. Supercontinuum, ultra wide optical source, nonlinear optical effects, continuous wave pump, ring cavity laser
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2

Arun, S. "Continuous-Wave Supercontinuum Generation using Cascaded Raman Fiber Lasers". Thesis, 2018. https://etd.iisc.ac.in/handle/2005/4888.

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This thesis explains architecture and techniques to generate high power, CW supercontinuum laser sources using standard Silica fibers as the nonlinear medium, pumped using high power CW Yb doped fiber lasers. Unlike the pulsed supercontinuum sources, the CW supercontinuum sources offer high average powers leading to spectacular power spectral densities at the output and can be realized at lower costs, in an all fiber architecture, which makes the system more compact and favorable towards power scaling. We have demonstrated a high power, all-fiber, wavelength tunable, fiber laser source that can operate in the L-band region (1.5-1.6 um), based on 6th order cascaded Raman amplification scheme, which can generate ~24 W of output power and is widely tunable from 1560-1590 nm. Using this laser we could pump the HNLF to generate a supercontinuum of ~700 nm bandwidth to powers as high as 35 W which is nearly double the output power than what has been previously demonstrated. To enhance the bandwidth and scale the output power, we have demonstrated a simple but highly impactful solution which uses the standard telecom fiber as the nonlinear medium. The supercontinuum generation module we demonstrated, is essentially a high efficiency cascaded Raman converter, which can take any CW, high power Ytterbium-doped fiber laser as the input and generate an octave spanning supercontinuum with an average power of ~34W, spanning over 1000nm (>1 octave) from 880nm to 1900nm at an efficiency of ~44%. The supercontinuum source exhibited excellent spectral and temporal stability for an extended duration of operation (>1 hour). The most highlighting result reported in this thesis is the record high output power that has been demonstrated from a CW supercontinuum so far. Using the recently proposed nonlinear power combining architecture we could leverage the output power (limited by available pump power) from the telecom fiber based octave spanning, CW supercontinuum. This involves nonlinear spectral power combining of outputs from multiple, independent, Yb lasers operating at different wavelengths as the pump sources, to generate supercontinuum at an efficiency of ~44% with a spectacular PSD of >3mW/nm from 850nm-1350 nm and an impressive PSD of >100mW/nm from 1350nm-1900nm at an output power of ~72 W.
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Actas de conferencias sobre el tema "CW supercontinuum"

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Wen, Cai, Peng Lu, H. Y. Fu y Qian Li. "CW Triggering in CW Pumped Supercontinuum Generation". En Frontiers in Optics. Washington, D.C.: OSA, 2017. http://dx.doi.org/10.1364/fio.2017.jw4a.71.

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2

Cumberland, B. A., A. B. Rulkov, J. C. Travers, S. V. Popov y J. R. Taylor. "High Power CW Pumped Supercontinuum Sources". En Asia Optical Fiber Communication and Optoelectronic Exposition and Conference. Washington, D.C.: OSA, 2008. http://dx.doi.org/10.1364/aoe.2008.sab1.

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3

Huang, Chao, H. Y. Fu y Qian Li. "Stimulated Supercontinuum Generation in CW-pumped Regime". En Frontiers in Optics. Washington, D.C.: OSA, 2018. http://dx.doi.org/10.1364/fio.2018.jtu2a.42.

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Cumberland, B. A., J. C. Travers, S. V. Popov y J. R. Taylor. "High power 29 W CW supercontinuum source". En Lasers and Applications in Science and Engineering, editado por Jes Broeng y Clifford Headley III. SPIE, 2008. http://dx.doi.org/10.1117/12.762075.

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Cumberland, B. A., J. C. Travers, S. V. Popov y J. R. Taylor. "High power 29 W CW supercontinuum source". En 2008 Conference on Lasers and Electro-Optics (CLEO). IEEE, 2008. http://dx.doi.org/10.1109/cleo.2008.4551143.

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6

Travers, J. C., S. V. Popov y J. R. Taylor. "A new model for CW supercontinuum generation". En 2008 Conference on Lasers and Electro-Optics (CLEO). IEEE, 2008. http://dx.doi.org/10.1109/cleo.2008.4551286.

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7

Cumberland, B. A., A. B. Rulkov, J. C. Travers, S. V. Popov y J. R. Taylor. "High Power Fibre-Integrated Supercontinuum Sources". En Workshop on Specialty Optical Fibers and their Applications. Washington, D.C.: Optica Publishing Group, 2008. http://dx.doi.org/10.1364/wsof.2008.ps19.

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High average power supercontinua are described both picosecond and cw laser pumped. Techniques are described for enhancing the short wavelength extent of the supercontinua and spectral power densities up to 100mW/nm have been achieved.
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8

Huang, Rongle, Renlai Zhou y Qian Li. "Mid-Infrared Supercontinuum Generation with a Weak CW Trigger". En Frontiers in Optics. Washington, D.C.: OSA, 2018. http://dx.doi.org/10.1364/fio.2018.jtu2a.93.

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9

Kudlinski, A., B. A. Cumberland, J. C. Travers, G. Bouwmans, Y. Quiquempois y A. Mussot. "CW Supercontinuum Generation in Photonic Crystal Fibres with Two Zero-Dispersion Wavelengths". En Workshop on Specialty Optical Fibers and their Applications. Washington, D.C.: Optica Publishing Group, 2008. http://dx.doi.org/10.1364/wsof.2008.osnf15.

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This study is devoted to supercontinuum generation in photonic crystal fibres using a continuous-wave pumping scheme. We demonstrate that the spectral broadening of a continuous-wave laser can be more efficiently achieved in a short piece of photonic crystal fibre with two zero-dispersion wavelengths rather than in a fibre with a single one. This is due to efficient self-frequency shift of the solitons initially created by modulation instability, because their peak power is kept high in fibres with two zero-dispersion wavelengths. We then focus on the dynamics of the supercontinuum evolution under continuous-wave pumping in a series of different photonic crystal fibres exhibiting two zero-dispersion wavelengths. Control of the supercontinuum spectral extension is demonstrated as well as the changing dynamics as the zero-dispersion wavelengths are brought closer together. For closest zero-dispersion wavelengths, the spectral broadening is mainly due to parametric processes. For increasing spectral separation between the two zero-dispersion wavelengths, the soliton self-frequency shift due to intrapulse Raman scattering becomes more important. The soliton self-frequency shift is canceled just before the second zero-dispersion wavelength and some energy is transferred to a phase-matched dispersive wave. We also pay particular attention to the effect of the water absorption band located around 1380 nm.
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10

Lu, Peng y Qian Li. "A weak femtosecond pulse seed on CW pumped supercontinuum generation". En 2017 Conference on Lasers and Electro-Optics Pacific Rim (CLEO-PR). IEEE, 2017. http://dx.doi.org/10.1109/cleopr.2017.8118810.

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