Relevant bibliographies by topics / Fiber laser amplifier

Contents

  1. Journal articles
  2. Dissertations / Theses
  3. Books
  4. Book chapters
  5. Conference papers
  6. Reports

Academic literature on the topic 'Fiber laser amplifier'

Author: Grafiati
Published: 4 June 2021
Last updated: 26 July 2025

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Journal articles on the topic "Fiber laser amplifier"

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Guan, Biao, Fengping Yan, Wenguo Han, et al. "High-Power, Narrow-Linewidth, Continuous-Wave, Thulium-Doped Fiber Laser Based on MOPA." Photonics 10, no. 4 (2023): 347. http://dx.doi.org/10.3390/photonics10040347.

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A high-power, narrow-linewidth, continuous-wave, thulium-doped fiber laser (TDFL) based on a master-oscillator power-amplifier (MOPA) was experimentally demonstrated. The main oscillator (seed source) yielded 0.64 W of narrow-linewidth laser output at a central wavelength of 1940.32 nm and a 3 dB spectral bandwidth of 0.05 nm. The output narrow-linewidth laser from the main oscillator was amplified by two-stage, cladding-pumped, thulium-doped, all-fiber amplifiers. The main amplifier yielded 26 W of narrow-linewidth laser at a central wavelength of 1940.33 nm. The slope efficiency of the main
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Sultana, Nasrin, and Abubakar Siddik. "Characterization of Visible Range Gain in Praseodymium Doped Fiber Amplifier." International Journal of Research and Review 11, no. 1 (2024): 140–46. http://dx.doi.org/10.52403/ijrr.20240115.

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In the optical (380-700 nm) region, a simulation study was conducted to assess the low-signal gain, power conversion efficiency (PCE), and optical output power of a praseodymium-doped fiber optic amplifier (PDFA). The PDFA performance was assessed using the optimized Pr3+ fiber length, Pr3+ ion concentration, and pump power. Additionally, the effects of input signal voltage and amplifier gain on amplified spontaneous emission (ASE) were investigated. A lower peak signal of roughly 1 dB at 635 nm was obtained with a shorter 5 m Pr3 + doped fiber and a higher pump power of 300 mW. The impact of
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Wang, Xiong, Pu Zhou, Xiaolin Wang, Hu Xiao, and Lei Si. "51.5 W monolithic single frequency 1.97 m Tm-doped fiber amplifier." High Power Laser Science and Engineering 1, no. 3-4 (2013): 123–25. http://dx.doi.org/10.1017/hpl.2013.20.

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AbstractWe demonstrate a monolithic single frequency Tm-doped fiber amplifier with output power of 51.5 W. A single frequency fiber laser at 1.97 $\mathrm {\mu} $m is amplified by a cascaded master oscillator power amplifier (MOPA) system with all-fiber configuration. The optical-to-optical conversion efficiency of the main fiber amplifier is 45%. No amplified spontaneous emission (ASE) or stimulated Brillouin scattering (SBS) effect is observed in the fiber amplifier. The output power could be further scaled by launching more pump power.
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Столяров, Д. А., Д. А. Коробко, И. О. Золотовский та А. А. Сысолятин. "Лазерный комплекс с центральной длиной волны 1.55 μm для генерации импульсов с энергией более 1 μJ и суперконтинуума диапазоном около 2 октав". Журнал технической физики 126, № 6 (2019): 717. http://dx.doi.org/10.21883/os.2019.06.47764.306-18.

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A fiber laser system of telecommunication range with simple block structure is considered. The main elements of the system are pulsed erbium fiber laser and several fiber amplifires. Including a fiber stretcher with a high normal dispersion the system works as a generator of high energy pulses. The characteristics of the high-power output amplifier and the pre-amplifiers are matched in such a way that the system is simply reconfigured into a supercontinuum source of the range from 600 to 2400 nm generated at the output of highly nonlinear fiber.
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Wang, Xiaolei, Xinqiang Ma, Yuan Ren, Jingwen Wang, and Wei Cheng. "Fiber Coupled High Power Nd:YAG Laser for Nondestructive Laser Cleaning." Photonics 10, no. 8 (2023): 901. http://dx.doi.org/10.3390/photonics10080901.

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In this study, a fiber coupled high power side-pumped Nd:YAG laser system for laser cleaning is presented. Based on the two-rod structure and two stages amplifiers, the maximum average output power of 783 W with corresponding pulse energy of 52 mJ at 15 kHz has been achieved. The fiber coupling efficiencies after the master oscillator, one stage amplifier and two stages amplifiers reach to 99%, 98.3% and 94%, respectively. A laser cleaning machine prototype composed of the master oscillator and one stage amplifier with an average output power of greater than 500 W has been developed and achiev
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Wang, Tingting, Jing Wang, Meng Zhao, et al. "Compact 15 mJ Fiber–Solid Hybrid Hundred-Picosecond Laser Source for Laser Ablation on Copper." Applied Sciences 12, no. 19 (2022): 9621. http://dx.doi.org/10.3390/app12199621.

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We report on a millijoule-level fiber–solid hybrid hundred-picosecond laser system with a stable performance and compact structure. The laser system is based on a master oscillator power amplifier structure containing an all-fiber master oscillator, a quasi-continuous-wave side-pumped Nd:YAG regenerative amplifier, and a double-pass amplifier. By using the filtering effect of fiber Bragg grating and the dispersion characteristics of single-mode fiber stretcher, the spectrum broadening caused by self-phase modulation effect is effectively suppressed. Thus, the gain linewidth of the Yb-doped fib
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Agrawal, Lalita, Atul Bhardwaj, Dinesh Ganotra, and Hari Babu Srivastava. "Estimation and Management of Performance Limiting Factors in the Development of 1 kW Peak Power Pulsed Fiber MOPA at 1550 nm." Defence Science Journal 71, no. 2 (2021): 222–30. http://dx.doi.org/10.14429/dsj.71.16203.

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 An all-fiber three-stage master oscillator power amplifier (MOPA), based on Erbium and Erbium-Ytterbium co-doped fibers, has been designed and developed. The performance of such a laser is primarily limited by amplified spontaneous emission (ASE), Yb bottlenecking, and non-linear effects. Other important factors, that need to be considered towards performance improvement, are fiber bend diameter and heat generated in the fiber. This paper describes the methodology for the estimation and management of these limiting factors for each amplifier stage. The work presented here
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Li, Qianglong, Feng Li, Hongjun Liu, et al. "Sub-50 fs pulses generation from an all-fiber monolithic gain-managed nonlinear amplifier with CFBG-based pre-compressor." Laser Physics Letters 21, no. 4 (2024): 045101. http://dx.doi.org/10.1088/1612-202x/ad291f.

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Abstract We demonstrate an all-fiber monolithic laser source from a gain-managed nonlinear (GMN) fiber amplifier with a CFBG-based pre-compressor that generates high-contrast pulses with a repetition rate of 80 MHz, average power of 1.6 W, and pulse duration of sub-50 fs. The compressed pulse quality can be optimized by tuning the parameters of the seed pulses injected into the GMN amplifier by controlling the pump power of the fiber pre-amplifier. This compact and cost-effective laser system is a simplified design of the GMN amplification-based femtosecond fiber laser systems. With alignment-
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Li, Dong Juan, Guang Hua Cheng, Zhi Yang, and Yi Shan Wang. "Ultrafast Laser Machine Based on All-Fiber Femtosecond Laser System." Advanced Materials Research 652-654 (January 2013): 2374–77. http://dx.doi.org/10.4028/www.scientific.net/amr.652-654.2374.

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A femtosecond laser machine consisting of femtosecond fiber laser, trepanning head, linear motor stages system and Siemens 840D system has been integrated for industry application. The femtosecond laser source is all fiber system which contains a fiber mode-lock laser at 1053 nm with a repetition rate of 3.9 MHz, a double-cladding gain fiber amplifiers and a PCF amplifier. An acoustical modulator has employed to tune repetition rate from 3.9 MHz to 100 KHz. An in-line fiber chirped grating is used to stretch the pulse duration to 700 ps. After the PCF amplifier pulse is compressed to sub-ps wi
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Xue, Mingyuan, Cunxiao Gao, Linquan Niu, et al. "A 20 W, Less-Than-1-kHz Linewidth Linearly Polarized All-Fiber Laser." Applied Sciences 8, no. 12 (2018): 2593. http://dx.doi.org/10.3390/app8122593.

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We report a continuous-wave high-output power and narrow-linewidth all-fiber laser at 1550 nm with the master oscillator power amplifier (MOPA) configuration. An all-fiber distributed feedback seed laser was boosted by three cascaded fiber amplifiers. In the experiment, we adopted a large-mode-area (LMA) Er3+:Yb3+-co-doped polarization-maintaining fiber to increase nonlinear thresholds and avoided the broadening of the laser linewidth. A linear-polarization fiber laser with average output power of 20 W, linewidth of 0.88 kHz, and power jitter less than 2% was finally achieved.
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Dissertations / Theses on the topic "Fiber laser amplifier"

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Currey, Ronnie. "Investigation of Specialized Laser and Optical Techniques to Improve Precision Atomic Spectroscopy of Helium." Thesis, University of North Texas, 2020. https://digital.library.unt.edu/ark:/67531/metadc1703412/.

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The aim of this thesis is to develop both Yb and Tm fiber laser sources with all fiber cavities. Both wavelength ranges provide useful laser sources for optical pumping of helium. The goal is to develop Tm laser sources operating at 2058 nm to optically quench 3He (2058.63 nm) and 4He (2058.69 nm) singlets (21S0). We also have developed Yb laser sources at 1083 nm to optical pump the triplet states of helium and laser cool an atomic beam of helium.
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Zhou, Renjie. "Developments of Narrow-Linewidth Q-switched Fiber Laser, 1480 nm Raman Fiber Laser, and Free Space Fiber Amplifier." Thesis, The University of Arizona, 2011. http://hdl.handle.net/10150/202931.

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In the first chapter, a Q-switched fiber laser that is capable of generating transform-limited pulses based on single-frequency fiber laser seeded ring cavity is demonstrated. The output pulse width can be tuned from hundreds of nanoseconds to several microseconds. This Q-switched ring cavity fiber laser can operate over the whole C-band. In addition, a theoretical model is developed to numerically study the pulse characteristics, and the numerical results are in good agreements with the experimental results. In the next chapter, a Raman fiber laser is developed for generating signal at 1480 n
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Song, Jiawei, and Jiawei Song. "Nd-doped Fiber Lasers and Fiber Amplifiers at 9xx nm." Thesis, The University of Arizona, 2016. http://hdl.handle.net/10150/620827.

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The lasers operating in the wavelength range of 900 - 1000 nm have caused intense attention because they are in great demands for: 1. Highpower blue and deep UV laser generation 2. High power single-mode pump laser source 3. Light detection and Lidar , etc. And now, there are actually many different types of lasers can generate laser in this wavelength range. For example, Nd and Yb doped fiber laser, Nd and Yb doped glass and crystal lasers, OPO and SHG laser, etc. Among all this options, we decided to study the Nd-doped fiber laser for their outstanding advantages: 1. As fiber laser, it posse
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Oppermann, Patrick [Verfasser]. "Characterization and stabilization of a high power fiber amplifier laser / Patrick Oppermann." Hannover : Technische Informationsbibliothek (TIB), 2017. http://d-nb.info/1136882707/34.

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Willis-Ott, Christina. "Ytterbium-doped fiber-seeded thin-disk master oscillator power amplifier laser system." Doctoral diss., University of Central Florida, 2013. http://digital.library.ucf.edu/cdm/ref/collection/ETD/id/5890.

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Lasers which operate at both high average power and energy are in demand for a wide range of applications such as materials processing, directed energy and EUV generation. Presented in this dissertation is a high-power 1 ?m ytterbium-based hybrid laser system with temporally tailored pulse shaping capability and up to 62 mJ pulses, with the expectation the system can scale to higher pulse energies. This hybrid system consists of a low power fiber seed and pre-amplifier, and a solid state thin-disk regenerative amplifier. This system has been designed to generate high power temporally t
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Natile, Michele. "High-repetition rate CEP-stable Yb-doped fiber amplifier for high harmonic generation." Electronic Thesis or Diss., Université Paris-Saclay (ComUE), 2019. http://www.theses.fr/2019SACLS149.

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Depuis une vingtaine d’années, la physique attoseconde, via le phénomène de génération d’harmoniques d’ordres élevés (HHG), a permis de nombreuses avancées dans la compréhension des phénomènes de dynamique ultra-rapide. Les lasers femtoseconde émettant des impulsions de fortes énergies et de durées de quelques cycles optiques sont les outils indispensables à cette physique. De plus, la phase entre la porteuse et l’enveloppe (CEP) des impulsions doit être contrôlée. Récemment les lasers basés sur les fibres dopées ytterbium ont permis de transposer les expériences d’HHG à haute cadence. La stab
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Natile, Michele. "High-repetition rate CEP-stable Yb-doped fiber amplifier for high harmonic generation." Thesis, Université Paris-Saclay (ComUE), 2019. http://www.theses.fr/2019SACLS149.

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Depuis une vingtaine d’années, la physique attoseconde, via le phénomène de génération d’harmoniques d’ordres élevés (HHG), a permis de nombreuses avancées dans la compréhension des phénomènes de dynamique ultra-rapide. Les lasers femtoseconde émettant des impulsions de fortes énergies et de durées de quelques cycles optiques sont les outils indispensables à cette physique. De plus, la phase entre la porteuse et l’enveloppe (CEP) des impulsions doit être contrôlée. Récemment les lasers basés sur les fibres dopées ytterbium ont permis de transposer les expériences d’HHG à haute cadence. La stab
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Leigh, Matthew. "HIGH POWER PULSED FIBER LASER SOURCES AND THEIR USE IN TERAHERTZ GENERATION&#8194." Diss., The University of Arizona, 2008. http://hdl.handle.net/10150/193797.

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In this dissertation I report the development of high power pulsed fiber laser systems. These systems utilize phosphate glass fiber for active elements, instead of the industry-standard silica fiber. Because the phosphate glass allows for much higher doping of rare-earth ions than silica fibers, much shorter phosphate fibers can be used to achieve the same gain as longer silica fibers.This single-frequency laser technology was used to develop an all-fiber actively Q-switched fiber lasers. A short cavity is used to create large spacing between longitudinal modes. Using this method, we demon
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Lesparre, Fabien. "Amplificateurs impulsionnels à base de fibres cristallines dopées Ytterbium." Thesis, Université Paris-Saclay (ComUE), 2017. http://www.theses.fr/2017SACLO001/document.

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Les lasers à impulsions ultra-courtes (< 10 ps) ont largement démontré leur intérêt pour de nombreuses applications scientifiques, industrielles ou encore médicales. Le domaine du micro-usinage par impulsions laser est l'un des domaines les plus actifs du moment. Les dernières avancées en la matière privilégient deux axes de recherche, l'augmentation du taux de répétition associé à de fortes puissances moyennes et une montée en énergie. Nos travaux s'inscrivent dans ce contexte et visent à développer des amplificateurs d'impulsions ultracourtes innovants à base de fibres cristallines Yb:YAG
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Tison, Guillaume. "Étude, réalisation et applications d’une chaîne amplificatrice laser compacte pour l’allumage de turbomoteurs." Thesis, Bordeaux 1, 2013. http://www.theses.fr/2013BOR14779/document.

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Ce travail porte sur l’étude et la réalisation d’une cellule d’allumage laser pour turbomoteurs. Une étude bibliographique nous a permis d’identifier les caractéristiques nécessaires : des impulsions nanosecondes d’au moins 10mJ. La spécificité de l’application impose de nombreuses contraintes qui ont influencé le choix d’une architecture avec deux étages amplificateurs : un amplificateur fibré suivi d’un amplificateur à base de fibre cristalline. Nous avons développé un code permettant de simuler l’amplification d’une impulsion nanoseconde dans ces milieux et ainsi déterminé les caractéristiques techn
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Books on the topic "Fiber laser amplifier"

1

Dutta, Niloy K. Fiber amplifiers and fiber lasers. World Scientific, 2015.

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Ter-Mikirtychev, Vartan V. Fundamentals of Fiber Lasers and Fiber Amplifiers. Springer International Publishing, 2019. http://dx.doi.org/10.1007/978-3-030-33890-9.

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Ter-Mikirtychev, Valerii. Fundamentals of Fiber Lasers and Fiber Amplifiers. Springer International Publishing, 2014. http://dx.doi.org/10.1007/978-3-319-02338-0.

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Desurvire, Emmanuel. Erbium-doped fiber amplifiers. Wiley, 1994.

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F, Digonnet Michel J., Automated Imaging Association, and Society of Photo-optical Instrumentation Engineers., eds. Fiber laser sources and amplifiers V: 7-8 September 1993, Boston, Massachusetts. SPIE, 1994.

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W, France P., ed. Optical fibre lasers and amplifiers. Blackie, 1991.

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F, Digonnet Michel J., ed. Rare earth doped fiber lasers and amplifiers. Marcel Dekker, 1993.

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F, Digonnet Michel J., ed. Rare-earth-doped fiber lasers and amplifiers. 2nd ed. Marcel Dekker, 2001.

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Desurvire, Emmanuel. Erbium-doped fiber amplifiers: Principles and applications. Wiley, 1994.

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Bjarklev, Anders. Optical fiber amplifiers: Design and system applications. Artech House, 1993.

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Book chapters on the topic "Fiber laser amplifier"

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Ter-Mikirtychev, Vartan V. "Main Optical Components for Fiber Laser/Amplifier Design." In Springer Series in Optical Sciences. Springer International Publishing, 2019. http://dx.doi.org/10.1007/978-3-030-33890-9_9.

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Ter-Mikirtychev, Valerii. "Main Optical Components for Fiber Laser/Amplifier Design." In Springer Series in Optical Sciences. Springer International Publishing, 2013. http://dx.doi.org/10.1007/978-3-319-02338-0_9.

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Burkley, Z., C. Rasor, S. F. Cooper, A. D. Brandt, and D. C. Yost. "Yb Fiber Amplifier at 972.5 nm with Frequency Quadrupling to 243.1 nm." In Exploring the World with the Laser. Springer International Publishing, 2018. http://dx.doi.org/10.1007/978-3-319-64346-5_3.

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Saule, T., S. Holzberger, O. De Vries, et al. "Phase-Stable, Multi-μJ Femtosecond Pulses from a Repetition-Rate Tunable Ti:Sa-Oscillator-Seeded Yb-Fiber Amplifier." In Exploring the World with the Laser. Springer International Publishing, 2018. http://dx.doi.org/10.1007/978-3-319-64346-5_14.

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Filippov, Valery, Juho Kerttula, and Oleg G. Okhotnikov. "Tapered Fiber Lasers and Amplifiers." In Fiber Lasers. Wiley-VCH Verlag GmbH & Co. KGaA, 2012. http://dx.doi.org/10.1002/9783527648641.ch6.

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Thyagarajan, K., and Ajoy Ghatak. "Doped Fiber Amplifiers and Lasers." In Lasers. Springer US, 2010. http://dx.doi.org/10.1007/978-1-4419-6442-7_12.

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Huang, Sheng-Lung. "Crystalline Fibers for Fiber Lasers and Amplifiers." In Handbook of Optical Fibers. Springer Singapore, 2018. http://dx.doi.org/10.1007/978-981-10-1477-2_52-1.

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Huang, Sheng-Lung. "Crystalline Fibers for Fiber Lasers and Amplifiers." In Handbook of Optical Fibers. Springer Singapore, 2019. http://dx.doi.org/10.1007/978-981-10-7087-7_52.

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Headley, C., M. Mermelstein, and J. C. Bouteiller. "Raman Fiber Lasers." In Raman Amplifiers for Telecommunications 2. Springer New York, 2004. http://dx.doi.org/10.1007/978-0-387-21585-3_2.

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Zoiros, K., T. Stathopoulos, K. Vlachos, et al. "Numerical Modeling of a High Repetition Rate Fiber Laser, Mode — Locked by External Optical Modulation of a Semiconductor Optical Amplifier." In IFIP Advances in Information and Communication Technology. Springer US, 2001. http://dx.doi.org/10.1007/978-0-387-35410-1_5.

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Conference papers on the topic "Fiber laser amplifier"

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Pertoldi, Andrea, Jakob M. Hauge, Poul Varming, and Patrick B. Montague. "Investigation of Stability in 2 µm Optical Fiber Amplifiers for Narrow-Linewidth Laser Sources." In CLEO: Science and Innovations. Optica Publishing Group, 2024. http://dx.doi.org/10.1364/cleo_si.2024.stu3d.3.

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Coherent backscatter causes noise and instability in fiber amplifiers when the wavelength of the laser is modulated. We investigate the effect of laser frequency, tuning speed, pumping scheme, dopant type, fiber length and amplifier gain.
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Yoshida, Mitsuhiro, Rui Zhang, Xiangyu Zhou, Arvydas Kausas, Hideki Ishizuki, and Takunori Taira. "Yb:YAG Fiber, Disk and DFC Hybrid Amplifier for DFG THz generation." In Laser Applications Conference. Optica Publishing Group, 2024. https://doi.org/10.1364/lac.2024.lth1b.2.

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The PPMgLN is currently best candidate for intense THz generation using both of the DFG and chirp and delay method. Yb disk and DFC(Distributed Face Cooling) laser are developed for the two wavelength laser or chirped pulsed laser for the DFC and chirp and delay respectively.
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Aleshkina, Svetlana S., Danila A. Davydov, Vladimir V. Velmiskin, et al. "1030 nm amplified spontaneous emission suppression in Yb-doped fiber amplifier operating near 976 nm." In 2024 International Conference Laser Optics (ICLO). IEEE, 2024. http://dx.doi.org/10.1109/iclo59702.2024.10624463.

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Yan, F., A. Ismaeel, I. O. Orekhov, et al. "Numerical simulation of supercontinuum generation in all-fiber Er-doped master oscillator fiber amplifier." In 2024 International Conference Laser Optics (ICLO). IEEE, 2024. http://dx.doi.org/10.1109/iclo59702.2024.10623989.

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Galvanauskas, A., M. E. Fermann, and D. Harter. "Use of Monolithic Tunable Laser Diodes for Chirped Pulse Amplification in Fiber Amplifiers." In International Conference on Ultrafast Phenomena. Optica Publishing Group, 1994. http://dx.doi.org/10.1364/up.1994.wc.30.

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Here we study the use of tunable three-section distributed-Bragg-reflector (DBR) diode lasers as pulse sources for chirped pulse amplification (CPA) in a fiber amplifier. The broad continuous-tuning range of the laser allows the generation of nanosecond linearly chirped pulses, which are amplified in a fiber amplifier up to microjoule energies and then compressed to transform-limited subpicosecond duration. The energy of these ultrashort pulses is more than two orders of magnitude higher than any previously reported energies from a compact diode laser and fiber source.
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Mito, Ikuo, та Kenji Endo. "1.48μm and 0.98μm High-Power Laser Diodes for Erbium-Doped Fiber Amplifiers". У Optical Amplifiers and Their Applications. Optica Publishing Group, 1991. http://dx.doi.org/10.1364/oaa.1991.wc1.

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The development of erbium-doped fiber amplifiers has recently progressed rapidly. Highly efficient power conversion for 1.48μm wavelength pumping enables a post-amplifier to achieve output power greater than 100mW1). When pumped in 0.98μm wavelength, the erbium-doped fiber amplifiers showed very low noise property2), which permits high receiver sensitivity as a pre-amplifier.
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Macomber, S. H., P. Akkapeddi, and A. Montroll. "Semiconductor Laser Power Amplifier." In Cambridge Symposium-Fiber/LASE '86, edited by Elliot G. Eichen. SPIE, 1987. http://dx.doi.org/10.1117/12.937680.

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Dergachev, Alex. "45-dB, Compact, Single-Frequency, 2-µm Amplifier." In Fiber Laser Applications. OSA, 2012. http://dx.doi.org/10.1364/filas.2012.fth4a.2.

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Islam, Mohammed N., L. F. Mollenauer, R. H. Stolen, J. R. Simpson, and H. T. Shang. "Amplifier/compressor fiber Raman lasers." In OSA Annual Meeting. Optica Publishing Group, 1987. http://dx.doi.org/10.1364/oam.1987.tuv3.

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When pump and Stokes pulses copropagate in a fiber Raman laser (FRL), the weaker Stokes spectrum is severely broadened through pump-induced cross-phase modulation (XPM).1 Thus, in an FRL during Raman amplification, the pulse is chirped through XPM, and then the linear anomalous dispersion of a fiber can compress the pulse. We first studied the output characteristics of single fiber and two-stage FRLs operating in the anomalous group velocity dispersion (GVD) regime. The lasers are made from single-mode polarization preserving dispersion-shifted fibers and are synchronously pumped by ~10-ps pul
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Brierley, Mike. "Prospects for Fiber Amplifiers at 1.3μm". У Optical Amplifiers and Their Applications. Optica Publishing Group, 1991. http://dx.doi.org/10.1364/oaa.1991.wb2.

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The erbium doped silica fiber amplifier for the 1.55μm telecommunications has now become a well established research laboratory tool. It offers high gain, high efficiency, low noise, low cross-talk, and high saturation power. It has been used in both land and under-sea systems demonstrations, and is commercially available from a number of manufacturers. In distribution experiments splits of up to 39 million ways have been demonstrated for only two stages of amplification [1]. In short it has revolutionised thinking on future optical fibre networks. Unfortunately the vast majority of current op
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Reports on the topic "Fiber laser amplifier"

1

Gosnell, T., Ping Xie, and N. Cockroft. Optical-fiber laser amplifier for ultrahigh-speed communications. Office of Scientific and Technical Information (OSTI), 1996. http://dx.doi.org/10.2172/231323.

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2

Messerly, M. Fiber Based Optical Amplifier for High Energy Laser Pulses, CRADA No. TC02100.0. Office of Scientific and Technical Information (OSTI), 2010. http://dx.doi.org/10.2172/1012487.

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3

Messerly, M., and P. Cunningham. Fiber Based Optical Amplifier for High Energy Laser Pulses Final Report CRADA No. TC02100.0. Office of Scientific and Technical Information (OSTI), 2017. http://dx.doi.org/10.2172/1396211.

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4

Teegarden, Kenneth J. Fiber Laser Amplifiers and Oscillators. Defense Technical Information Center, 1993. http://dx.doi.org/10.21236/ada274231.

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Fetterman, Harold. Advanced Optoelectronic Systems Using Fiber Amplifiers and Lasers. Defense Technical Information Center, 2001. http://dx.doi.org/10.21236/ada386882.

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6

Zhang, Lin. High Extinction Ratio In-Fibre Polarisers by Exploiting Tilted Fibre Bragg Grating Structures for Single-Polarisation High-Power Fibre Lasers and Amplifiers. Defense Technical Information Center, 2009. http://dx.doi.org/10.21236/ada524631.

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