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Relevant bibliographies by topics / Raman fiber lasers

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Academic literature on the topic 'Raman fiber lasers'

Author: Grafiati

Published: 6 September 2023

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Journal articles on the topic "Raman fiber lasers"

1

Li, Ziyan, Wenxi Pei, Hao Li, Wei Huang, Xuanxi Li, Zefeng Wang, and Jinbao Chen. "D2-Filled Hollow-Core Fiber Gas Raman Laser at 2.15 μm." Photonics 9, no. 10 (October 11, 2022): 753. http://dx.doi.org/10.3390/photonics9100753.

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Fiber lasers around 2 µm band have attractive applications, such as coherent detecting, material processing, pump source for mid-IR lasers based on nonlinear frequency shift, etc. Fiber gas Raman lasers (FGRLs) based on the stimulated Raman scattering of the gas molecules filled in the hollow-core fibers (HCFs) have been proved an efficient method to enrich the wavelengths of fiber lasers. In this paper, we demonstrated a deuterium-filled fiber gas Raman laser working at 2147 nm. The pump laser is directly coupled into the HCF through the fusion splice between the HCF and the solid-core fiber. By adjusting the pressure, fiber length as well as the repetition frequency of the 1971 nm pump laser, a maximum average Raman power of ~2.57 W was obtained, with corresponding efficiency of ~40%. This work provides a simple and compact configuration for 2.1 µm fiber lasers, which is significant for their application.

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Pei, Wenxi, Hao Li, Wei Huang, Meng Wang, and Zefeng Wang. "All-Fiber Gas Raman Laser by D2-Filled Hollow-Core Photonic Crystal Fibers." Photonics 8, no. 9 (September 9, 2021): 382. http://dx.doi.org/10.3390/photonics8090382.

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We report here an all-fiber structure tunable gas Raman laser based on deuterium-filled hollow-core photonic crystal fibers (HC-PCFs). An all-fiber gas cavity is fabricated by fusion splicing a 49 m high-pressure deuterium-filled HC-PCF with two solid-core single-mode fibers at both ends. When pumped with a pulsed fiber amplifier seeded by a tunable laser diode at 1.5 μm, Raman lasers ranging from 1643 nm to 1656 nm are generated. The maximum output power is ~1.2 W with a Raman conversion efficiency of ~45.6% inside the cavity. This work offers an alternative choice for all-fiber lasers operating at 1.6–1.7 μm band.

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Sirleto, Luigi. "Fiber Raman Amplifiers and Fiber Raman Lasers." Micromachines 11, no. 12 (November 27, 2020): 1044. http://dx.doi.org/10.3390/mi11121044.

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Supradeepa, V. R., Yan Feng, and Jeffrey W. Nicholson. "Raman fiber lasers." Journal of Optics 19, no. 2 (January 4, 2017): 023001. http://dx.doi.org/10.1088/2040-8986/19/2/023001.

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Sirleto, Luigi, and Maria Antonietta Ferrara. "Fiber Amplifiers and Fiber Lasers Based on Stimulated Raman Scattering: A Review." Micromachines 11, no. 3 (February 26, 2020): 247. http://dx.doi.org/10.3390/mi11030247.

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Nowadays, in fiber optic communications the growing demand in terms of transmission capacity has been fulfilling the entire spectral band of the erbium-doped fiber amplifiers (EDFAs). This dramatic increase in bandwidth rules out the use of EDFAs, leaving fiber Raman amplifiers (FRAs) as the key devices for future amplification requirements. On the other hand, in the field of high-power fiber lasers, a very attractive option is provided by fiber Raman lasers (FRLs), due to their high output power, high efficiency and broad gain bandwidth, covering almost the entire near-infrared region. This paper reviews the challenges, achievements and perspectives of both fiber Raman amplifier and fiber Raman laser. They are enabling technologies for implementation of high-capacity optical communication systems and for the realization of high power fiber lasers, respectively.

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Li, Jun, Hao Li, and Zefeng Wang. "Application of Hollow-Core Photonic Crystal Fibers in Gas Raman Lasers Operating at 1.7 μm." Crystals 11, no. 2 (January 27, 2021): 121. http://dx.doi.org/10.3390/cryst11020121.

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A 1.7 μm pulsed laser plays an important role in bioimaging, gas detection, and so on. Fiber gas Raman lasers (FGRLs) based on hollow-core photonic crystal fibers (HC-PCFs) provide a novel and effective method for fiber lasers operating at 1.7 μm. Compared with traditional methods, FGRLs have more advantages in generating high-power 1.7 μm pulsed lasers. This paper reviews the studies of 1.7 μm FGRLs, briefly describes the principle and characteristics of HC-PCFs and gas-stimulated Raman scattering (SRS), and systematical characterizes 1.7 μm FGRLs in aspects of output spectral coverage, power-limiting factors, and a theoretical model. When the fiber length and pump power are constant, a relatively high gas pressure and appropriate pump peak power are the key to achieving high-power 1.7 μm Raman output. Furthermore, the development direction of 1.7 μm FGRLs is also explored.

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Hu, Chunhua, and Ping Sun. "Intra-Cavity Raman Laser Operating at 1193 nm Based on Graded-Index Fiber." Photonics 10, no. 1 (December 28, 2022): 33. http://dx.doi.org/10.3390/photonics10010033.

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Nonlinear Raman frequency conversion is an important technical scheme to obtain special optical band lasers based on conventional ion-doped lasers. In our work, we designed an intra-cavity Raman fiber laser based on graded index fiber (GRIF) as the Raman gain medium. Based on the fundamental-frequency 1080-nanometer laser, efficient first-order and second-order Stokes Raman lasers were obtained, respectively. When the power of the fundamental-frequency 1080-nanometer laser was 33.4 W, the output power of the second-order 1193-nanometer laser was 11.39 W. The corresponding conversion efficiency was 34.1%. To our knowledge, this is the first report of a second-order Raman output based on a GRIF and intra-cavity structure. In the experiment, the spectrum-purification process with the increase in power was also observed. Our experimental results prove that the intracavity Raman-laser system based on graded index fiber with a high optical conversion efficiency has important application potential for obtaining new special-application bands.

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Pei, Wenxi, Hao Li, Wei Huang, Meng Wang, and Zefeng Wang. "All-Fiber Tunable Pulsed 1.7 μm Fiber Lasers Based on Stimulated Raman Scattering of Hydrogen Molecules in Hollow-Core Fibers." Molecules 26, no. 15 (July 28, 2021): 4561. http://dx.doi.org/10.3390/molecules26154561.

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Fiber lasers that operate at 1.7 μm have important applications in many fields, such as biological imaging, medical treatment, etc. Fiber gas Raman lasers (FGRLs) based on gas stimulated Raman scattering (SRS) in hollow-core photonic crystal fibers (HC-PCFs) provide an elegant way to realize efficient 1.7 μm fiber laser output. Here, we report the first all-fiber structure tunable pulsed 1.7 μm FGRLs by fusion splicing a hydrogen-filled HC-PCF with solid-core fibers. Pumping with a homemade tunable pulsed 1.5 μm fiber amplifier, efficient 1693~1705 nm Stokes waves are obtained by hydrogen molecules via SRS. The maximum average output Stokes power is 1.63 W with an inside optical–optical conversion efficiency of 58%. This work improves the compactness and stability of 1.7 μm FGRLs, which is of great significance to their applications.

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Ismail, Aiman, Hazwani Mohammad Helmi, Md Zaini Jamaludin, Fairuz Abdullah, Abdul Hadi Sulaiman, and Ker Pin Jern. "Erbium-Doped Fiber Amplification Assisted Multi-Wavelength Brillouin-Raman Fiber Laser." International Journal of Engineering & Technology 7, no. 4.35 (November 30, 2018): 854. http://dx.doi.org/10.14419/ijet.v7i4.35.26269.

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Multi-wavelength fiber laser based on Brillouin scattering in optical fiber has the potential of application in dense wavelength division multiplexing (DWDM) system. To enhance the performance of the fiber lasers, researchers proposed usages of erbium, or Raman amplification techniques. In an earlier work, it was reported that extracting residual Raman pump out of the laser cavity improves the performance of a multi-wavelength Raman fiber laser. In this paper, we proposed a setup utilizing the residual Raman pump to pump an erbium-doped fiber in multi-wavelength Brillouin-Raman fiber laser. Results show that the additional erbium-doped fiber is capable of amplifying the propagating Brillouin Stokes by more than 15-dB. This in turn helps in achieving lower stimulated Brillouin threshold and subsequently allow for higher number of Brillouin Stokes lines to be generated.

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Chen, Yizhu, Chenchen Fan, Tianfu Yao, Hu Xiao, Jiangming Xu, Jinyong Leng, Pu Zhou, et al. "Comparison of multimode GRIN-fiber Raman lasers with FBG and random DFB cavity." Journal of Physics: Conference Series 2249, no. 1 (April 1, 2022): 012015. http://dx.doi.org/10.1088/1742-6596/2249/1/012015.

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Abstract Raman lasing in multimode GRIN fibers is accompanied by sufficient improvement of the output beam quality in comparison with that for pump radiation, which offers opportunities to wavelength-agile fiber lasers of new type. Here we compare power scaling and brightness enhancement capabilities of Raman laser based on multimode GRIN-fiber of 62.5/125 um core/cladding diameters pumped by ∼700 W multimode source with beam quality M2∼10, performed in two different cavity configurations: 1) linear cavity based on two fiber Bragg gratings and 2) half-open cavity with one FBG and random distributed feedback via Rayleigh backscattering along the GRIN fiber.

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Dissertations / Theses on the topic "Raman fiber lasers"

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Gapontsev, Denis Valentinovitch. "Fiber Raman lasers and amplifiers and their applications." Thesis, Imperial College London, 1999. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.322403.

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Berberoglu, Halil. "Numerical Simulations On Stimulated Raman Scattering For Fiber Raman Amplifiers And Lasers Using Spectral Methods." Phd thesis, METU, 2007. http://etd.lib.metu.edu.tr/upload/3/12608986/index.pdf.

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Optical amplifiers and lasers continue to play its crucial role and they have become an indispensable part of the every fiber optic communication systems being installed from optical network to ultra-long haul systems. It seems that they will keep on to be a promising future technology for high speed, long-distance fiber optic transmission systems. The numerical simulations of the model equations have been already commercialized by the photonic system designers to meet the future challenges. One of the challenging problems for designing Raman amplifiers or lasers is to develop a numerical method that meets all the requirements such as accuracy, robustness and speed. In the last few years, there have been much effort towards solving the coupled differential equations of Raman model with high accuracy and stability. The techniques applied in literature for solving propagation equations are mainly based on the finite differences, shooting or in some cases relaxation methods. We have described a new method to solve the nonlinear equations such as Newton-Krylov iteration and performed numerical simulations using spectral methods. A novel algorithm implementing spectral method (pseuodspectral) for solving the two-point boundary value problem of propagation equations is proposed, for the first time to the authors'
knowledge in this thesis. Numerical results demonstrate that in a few iterations great accuracy is obtained using fewer grid points.

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Zhu, Gongwen. "Q-switched and Mode-locked Mid-IR Fiber Lasers." Diss., The University of Arizona, 2015. http://hdl.handle.net/10150/578593.

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Mid-infrared (IR) lasers (2-12 μm) have found tremendous applications in medical surgeries, spectroscopy, remote sensing, etc. Nowadays, mid-IR emissions are usually generated from semiconductor lasers, gas lasers, and solid-state lasers based on nonlinear wavelength conversion. However, they usually have disadvantages including poor beam quality, low efficiency, and complicated configurations. Mid-IR fiber lasers have the advantages of excellent beam quality, high efficiency, inherent simplicity, compactness, and outstanding heat-dissipating capability, and have attracted significant interest in recent years. In this dissertation, I have studied and investigated Q-switched and mode-locked fiber lasers in the mid-IR wavelength region. My dissertation includes six chapters: In Chapter 1, I review the background of mid-IR lasers and address my motivation on the research of mid-IR fiber lasers; In Chapter 2, I present the experimental results of microsecond and nanosecond Er³⁺-doped and Ho³⁺-doped fiber lasers in the 3 μm wavelength region Q-switched by Fe²⁺:ZnSe and graphene saturable absorbers. In Chapter 3, Q-switched 3 μm laser fiber amplifiers are investigated experimentally and theoretically and their power scaling are discussed. In Chapter 4, a graphene mode-locked Er³⁺-doped fiber lasers at 2.8 μm with a pulse width < 50 ps is presented. In Chapter 5, extending the spectral range of mid-IR fiber lasers by use of nonlinear wavelength conversion is addressed and discussed. I have proposed 10-watt-level 3-5 μm Raman lasers using tellurite fibers as the nonlinear gain medium and pumped by our Er³⁺-doped fiber lasers at 2.8 μm. In the last chapter, the prospect of mid-IR fiber laser is addressed and further research work is discussed.

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El, bassri Farid. "Sources lasers déclenchées nanosecondes : Applications à la spectroscopie Raman cohérente sous champ électrique." Thesis, Limoges, 2014. http://www.theses.fr/2014LIMO0060/document.

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Du fait de leur compacité, leur robustesse et leur faible coût, les microlasers impulsionnels nanosecondes constituent des sources particulièrement attractives pour de nombreux systèmes de détection et d'analyse, en particulier les cytomètres en flux ou les dispositifs pour la spectroscopie CARS (Coherent Raman Anti Stokes Scattering). Cependant, ces applications nécessitent des performances améliorées en ce qui concerne la gigue temporelle et la cadence de répétition accessible. Dans sa première partie, cette thèse propose des solutions originales pour atteindre les performances requises à partir de microlasers passivement déclenchés, grâce à la mise en oeuvre d'une cavité hybride couplée, pompée par une onde modulée en intensité. Une cadence de répétition supérieure à 30 kHz avec une gigue demeurant inférieure à 200 ns est atteinte. Le potentiel de microlasers à fibres déclenchés par modulation du gain pour monter en cadence est aussi évalué, montrant que des impulsions à faible gigue, à une cadence de plus de 2 MHz peuvent être produites. Enfin, la dernière partie est consacrée à la mise au point et à l'exploitation d'un nouveau système de spectroscopie CARS assisté par une excitation électrique haute tension. Ce dispositif, réalisé à partir d'un microlaser amplifié, permet de s'affranchir du bruit de fond non résonnant des mesures et de réaliser une analyse spectroscopique fine de la réponse de différents milieux d'intérêt sous champ continu ou impulsionnel, pouvant conduire à une nouvelle méthode de microdosimétrie de champ. Diverses applications, dont la granulométrie à l'échelle micro ou nanométrique ou l'identification de marqueurs pour la biologie, sont démontrées
Thanks to their compactness, robustness and low cost, pulsed nanosecond microlasers are particularly attractive sources for different detection and analysis systems, particularly flow cytometers or devices for CARS (Coherent Anti Raman Stokes Scattering) spectroscopy. However, these applications require reduced time jitter and increased repetition rate. The first part of this thesis proposes novel solutions to achieve the required performance from passively Q-switched microlasers, which are based on an hybrid coupled-cavity and intensitymodulated pump wave. A repetition rate greater than 30 kHz with jitter remaining lower than 200 ns is reached. Pulsed fiber microlasers operating by gain switching are also studied, showing that pulses with low timing jitter, at a repetition rate of more than 2 MHz can be obtained. The last part is devoted to the development and the implementation of a new system of CARS spectroscopy assisted by a high-voltage electrical stimulation. This device, based on an amplified microlaser, allows to substract the non-resonant background noise in the measurements. Thus, a fine spectroscopic analysis of the response of different environments of interest in continuous or pulsed field can be achieved. It may lead to a new method for field microdosimetry. Various applications, including granulometry at the micro or nanometric scale and the identification of markers for biology, are shown

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Nishizawa, Norihiko, Youta Ito, and Toshio Goto. "0.78-0.90-μm wavelength-tunable femtosecond soliton pulse generation using photonic crystal fiber." IEEE, 2002. http://hdl.handle.net/2237/6769.

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Benoit, Aurélien. "Sources laser fibrées hybrides de haute puissance : Amplification et conversion de fréquences." Thesis, Limoges, 2015. http://www.theses.fr/2015LIMO0024/document.

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Les lasers à fibre de haute puissance constituent depuis une dizaine d’année un outil pertinent pour un nombre croissant d’applications. Dans le cadre d’un contrat CIFRE entre la société Eolite Systems et le laboratoire Xlim (UMR 7252 du CNRS et de l’Université de Limoges), mon projet de thèse a consisté à développer les briques technologiques de futures sources lasers
High-power fiber lasers adress an increasing number of applications since ten years. In the frame of a CIFRE contract between the company Eolite Systems and Xlim (joint laboratory between CNRS and the University of Limoges), the goal of this PhD project was to develop the technological blocs to achieve all-fibre high-power lasers emiting out of the conventional spectral band covered by existing lasers.Modal instabilities in large mode area (LMA) fibers are currently the main limitation of the fiber lasers power scaling. We have experimentally demonstrated the relevance of inner cladding aperiodic structures to efficiently delocalize higher order modes outside the gain region. A systematic study of passive fibers based on such structures has shown the single propagation of the fundamental mode over a wide wavelength range from 1 to 2 µm for dimension of core up to 85 µm. This effective mode delocalization even extends up to a core dimension of 140 µm at a 2 µm wavelength.The combination of high power picosecond fiber laser with an average power of 22.7 W and a hydrogen-filled inhibited coupling Kagome fiber allowed us to generate two Raman combs over five frequency octaves from 321 nm to 12.5 µm. These two combs are controlled by the laser pump polarization and generated an average power of 10.1 W displayed over 70 laser lines for circular pump polarization and 8.6 W over 30 lines for linear polarization. Some laser lines within these combs have been generated for the first time from high-power fiber source in the mid-infrared range. We have also demonstrated the generation of high-power line by optimizing the first vibrational Stokes at 1.8 µm with an average power of 9.3 W and a quantum efficiency of the frequency conversion stage close to 80%

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Louot, Christophe. "Sources de supercontinuum pour la microspectroscopie Raman cohérente large-bande." Thesis, Limoges, 2018. http://www.theses.fr/2018LIMO0015/document.

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La microspectroscopie Raman cohérente (CARS) est une méthode d'analyse optique sans marqueur qui permet d'identifier des liaisons moléculaires dans un milieu d'intérêt (échantillon) pour permettre de déterminer la composition chimique de ce milieu. Elle nécessite l'excitation concomitante de l'échantillon par deux ondes spectralement décalées (onde pompe et onde Stokes) afin de faire entrer en résonance les liaisons à détecter. Pour la détection de plusieurs liaisons simultanément (microspectroscopie Raman cohérente large-bande ou Multiplex-CARS), la source Stokes monochromatique est remplacée par une source laser large-bande (supercontinuum). Les travaux effectués dans le cadre de cette thèse visent à proposer de nouvelles sources de supercontinuum émettant des faisceaux optimisés en termes d'élargissement spectral et de densité spectrale de puissance pour la microspectroscopie Multiplex-CARS. Pour ce faire, les moyens de développer des continuums spectraux performants ont été explorés dans trois fibres optiques différentes: une fibre microstructurées air/silice monomode à gros cœur dopé à l'ytterbium permettant une réamplification du signal tout au long de sa propagation ; une fibre monomode conventionnelle en régime de dispersion normale pour obtenir un élargissement spectral par saturation du gain Raman ; une fibre multimode dans laquelle le faisceau spectralement élargi par saturation du gain Raman à très forte puissance subit également un auto-nettoyage spatial par effet Kerr tout au long de sa propagation, produisant en sortie un faisceau de forte brillance dont le profil d’intensité est semblable à celui du mode fondamental. Une étude spectrotemporelle complète est présentée pour ces trois sources
Coherent Raman microspectroscopy (CARS) is an optical method used to identify molecular bonds in a sample in order to analyze and determine its complete composition. It requires the simultaneous excitation of the sample by two waves (the pump wave and the Stokes wave) in order to induce resonant vibration of the bond to be detected. For multiple bonds analysis (broadband coherent Raman microspectroscopy our Multiplex-CARS), the monochromatic Stokes wave must be replaced by a broadband beam (supercontinuum). The aim of this thesis was to design supercontinuum sources optimized for Multiplex-CARS application, in particular in terms of spectral bandwidth and spectral power density. Supercontinuum generation was investigated in three different optical fibers: (i) a microstructured single mode fiber with a large Yb doped core in which the input beam was re-amplified all along its propagation; (ii) a conventional singlemode fiber pumped in the normal dispersion regime in which spectral broadening was achieved by means of Raman gain saturation; (iii) a conventional graded-index multimode fiber in which the beam spectrally broadened by Raman gain saturation at very high power also experienced spatial self-cleaning by Kerr effect, resulting in a high brillance output beam with an,intensity profile close to that of the fundamental mode. A complete spectrotemporal study is achieved for each of these three sources

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Nishizawa, Norihiko, and Toshio Goto. "Widely wavelength-tunable ultrashort pulse generation using polarization maintaining optical fibers." IEEE, 2001. http://hdl.handle.net/2237/6864.

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Nishizawa, Norihiko, and Toshio Goto. "Compact system of wavelength-tunable femtosecond soliton pulse generation using optical fibers." IEEE, 1999. http://hdl.handle.net/2237/6767.

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Nishizawa, Norihiko, Ryuji Okamura, and Toshio Goto. "Simultaneous generation of wavelength tunable two-colored femtosecond soliton pulses using optical fibers." IEEE, 1999. http://hdl.handle.net/2237/6771.

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Books on the topic "Raman fiber lasers"

1

Feng, Yan, ed. Raman Fiber Lasers. Cham: Springer International Publishing, 2017. http://dx.doi.org/10.1007/978-3-319-65277-1.

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ZnO bao mo zhi bei ji qi guang, dian xing neng yan jiu. Shanghai Shi: Shanghai da xue chu ban she, 2010.

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Feng, Yan. Raman Fiber Lasers. Springer, 2017.

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Feng, Yan. Raman Fiber Lasers. Springer, 2018.

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Dixon, Nicholas Michael. Raman microscopy of laser damaged dielectric films and optical fibre inclusions. 1990.

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Book chapters on the topic "Raman fiber lasers"

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Feng, Yan, and Lei Zhang. "High Power Raman Fiber Lasers." In Raman Fiber Lasers, 1–33. Cham: Springer International Publishing, 2017. http://dx.doi.org/10.1007/978-3-319-65277-1_1.

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Supradeepa, V. R., and Jeffrey W. Nicholson. "Cascaded Raman Fiber Lasers." In Raman Fiber Lasers, 35–66. Cham: Springer International Publishing, 2017. http://dx.doi.org/10.1007/978-3-319-65277-1_2.

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Fortin, Vincent, Martin Bernier, and Réal Vallée. "Mid-Infrared Raman Fiber Lasers." In Raman Fiber Lasers, 67–116. Cham: Springer International Publishing, 2017. http://dx.doi.org/10.1007/978-3-319-65277-1_3.

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Islam, Mohammed N. "Infrared Super-continuum Light Sources and Their Applications." In Raman Fiber Lasers, 117–203. Cham: Springer International Publishing, 2017. http://dx.doi.org/10.1007/978-3-319-65277-1_4.

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Qin, Guanshi. "Specialty Optical Fibers for Raman Lasers." In Raman Fiber Lasers, 205–33. Cham: Springer International Publishing, 2017. http://dx.doi.org/10.1007/978-3-319-65277-1_5.

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Westbrook, Paul S., Kazi S. Abedin, and Tristan Kremp. "Distributed Feedback Raman and Brillouin Fiber Lasers." In Raman Fiber Lasers, 235–71. Cham: Springer International Publishing, 2017. http://dx.doi.org/10.1007/978-3-319-65277-1_6.

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Babin, Sergey A., Sergey I. Kablukov, Ekaterina A. Zlobina, Evgeniy V. Podivilov, Sofia R. Abdullina, Ivan A. Lobach, Alexey G. Kuznetsov, Ilya D. Vatnik, Dmitry V. Churkin, and Sergei K. Turitsyn. "Random Distributed Feedback Raman Fiber Lasers." In Raman Fiber Lasers, 273–354. Cham: Springer International Publishing, 2017. http://dx.doi.org/10.1007/978-3-319-65277-1_7.

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Westbrook, Paul S., Kazi S. Abedin, and Tristan Kremp. "Erratum to: Distributed Feedback Raman and Brillouin Fiber Lasers." In Raman Fiber Lasers, E1. Cham: Springer International Publishing, 2017. http://dx.doi.org/10.1007/978-3-319-65277-1_8.

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Lin, Chinlon. "Fiber Raman lasers." In Topics in Applied Physics, 279–301. Berlin, Heidelberg: Springer Berlin Heidelberg, 1992. http://dx.doi.org/10.1007/3-540-55571-4_7.

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Lin, Chinlon. "Fiber Raman Lasers." In Topics in Applied Physics, 279–301. Berlin, Heidelberg: Springer Berlin Heidelberg, 1987. http://dx.doi.org/10.1007/978-3-662-10635-8_7.

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Conference papers on the topic "Raman fiber lasers"

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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. Washington, D.C.: 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 pulses from a TI°(1);KCI color center laser. To separate and better understand the amplification and compression, we used two different dispersion-shifted fibers in a two-stage configuration; the laser was tuned so that amplification occurred under normal GVD, while compression occurred under anomalous GVD. In this latter configuration we find that a steady-state pulse width is not achieved throughout the laser, and we also observe the soliton self-frequency shift.2 The strong XPM in an FRL favors the production of subpicosecond pulses, usually accompanied by a broad pedestal. Nevertheless, in special conditions, nearly pedestal-free (subpicosecond) pulses can be produced, even in the presence of XPM. We demonstrate such production in a two-stage FRL operating entirely in the anomalous GVD regime.

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2

Desurvire, E., B. Y. Kim, K. A. Fesler, and H. J. Shaw. "Reentrant Fiber Raman Gyroscope." In Conference on Lasers and Electro-Optics. Washington, D.C.: OSA, 1986. http://dx.doi.org/10.1364/cleo.1986.thu5.

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Wu, Tsai-wei, and Herbert G. Winful. "Raman Fiber Laser Arrays." In Conference on Lasers and Electro-Optics. Washington, D.C.: OSA, 2009. http://dx.doi.org/10.1364/cleo.2009.jthe23.

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Taniguchi, Atsushi, Tetsuro Kuwayama, Akira Shirakawa, Mitsuru Musha, Ken-ichi Ueda, and Mahendra Prabhu. "Raman fiber laser-pumped 2-μm fiber laser." In International Conference on Lasers, Applications, and Technologies 2002 Advanced Lasers and Systems, edited by Guenter Huber, Ivan A. Scherbakov, and Vladislav Y. Panchenko. SPIE, 2003. http://dx.doi.org/10.1117/12.517936.

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Gladyshev, A. V., A. F. Kosolapov, M. S. Astapovich, A. N. Kolyadin, A. D. Pryamikov, M. M. Khudyakov, M. E. Likhachev, and I. A. Bufetov. "Revolver Hollow-Core Fibers and Raman Fiber Lasers." In Optical Fiber Communication Conference. Washington, D.C.: OSA, 2018. http://dx.doi.org/10.1364/ofc.2018.m2j.7.

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Stolen, Roger. "Raman Fiber Lasers and Amplifiers." In Frontiers in Optics. Washington, D.C.: OSA, 2015. http://dx.doi.org/10.1364/fio.2015.fth3h.1.

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Grubb, Stephen G. "Cascaded Raman Fiber Lasers and Amplifiers." In Bragg Gratings, Photosensitivity, and Poling in Glass Fibers and Waveguides. Washington, D.C.: Optica Publishing Group, 1997. http://dx.doi.org/10.1364/bgppf.1997.bmc.1.

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Abstract:

The recent availability of high power cladding pumped fiber lasers and low loss fiber resonators enabled with fiber Bragg grating technology, have made efficient CW Raman frequency conversion extremely efficient. The technology of cascaded Raman lasers and amplifiers will be reviewed.

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Headley III, Clifford, Jean-Christophe Bouteiller, Marc Mermelstein, Khush Brar, and Christopher Horn. "Raman fiber lasers as pumps for Raman amplification." In ITCom 2002: The Convergence of Information Technologies and Communications, edited by Achyut K. Dutta, Abdul Ahad S. Awwal, Niloy K. Dutta, and Katsunari Okamoto. SPIE, 2002. http://dx.doi.org/10.1117/12.475529.

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Kafka, J. D., D. F. Head, and T. Baer. "Dispersion Compensated Fiber Raman Oscillator." In Conference on Lasers and Electro-Optics. Washington, D.C.: OSA, 1986. http://dx.doi.org/10.1364/cleo.1986.thu6.

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Shaw, L. B., P. C. Pureza, V. Q. Nguyen, J. S. Sanghera, I. D. Aggarwal, and P. A. Thielen. "Raman Amplification in As-Se Fiber." In Advanced Solid State Lasers. Washington, D.C.: OSA, 2002. http://dx.doi.org/10.1364/assl.2002.ma5.

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Reports on the topic "Raman fiber lasers"

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Ziegler, K. E. Fiber-Optic Laser Raman Spectroscopy Sensor. Office of Scientific and Technical Information (OSTI), September 2003. http://dx.doi.org/10.2172/815181.

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Mildren, Richard. High Average Power Raman Conversion in Diamond: 'Eyesafe' Output and Fiber Laser Conversion. Fort Belvoir, VA: Defense Technical Information Center, June 2015. http://dx.doi.org/10.21236/ada626805.

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