Littérature scientifique sur le sujet « Gigahertz repetition rate laser source »
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Articles de revues sur le sujet "Gigahertz repetition rate laser source"
Shang, Jingcheng, Shengzhi Zhao, Yizhou Liu, Kejian Yang, Chun Wang, Yuefeng Zhao, Yuzhi Song et al. « Gigahertz-repetition rate, high power, ultrafast Tm-doped fiber laser source ». Optics & ; Laser Technology 153 (septembre 2022) : 108206. http://dx.doi.org/10.1016/j.optlastec.2022.108206.
Texte intégralShang, Jingcheng, Shengzhi Zhao, Yizhou Liu, Kejian Yang, Chun Wang, Yuefeng Zhao, Yuzhi Song et al. « Gigahertz-repetition rate, high power, ultrafast Tm-doped fiber laser source ». Optics & ; Laser Technology 153 (septembre 2022) : 108206. http://dx.doi.org/10.1016/j.optlastec.2022.108206.
Texte intégralXiang, Chao, Junqiu Liu, Joel Guo, Lin Chang, Rui Ning Wang, Wenle Weng, Jonathan Peters et al. « Laser soliton microcombs heterogeneously integrated on silicon ». Science 373, no 6550 (1 juillet 2021) : 99–103. http://dx.doi.org/10.1126/science.abh2076.
Texte intégralStormont, B., I. G. Cormack, M. Mazilu, C. T. A. Brown, D. Burns et W. Sibbett. « Low-threshold, multi-gigahertz repetition-rate femtosecond Ti:sapphire laser ». Electronics Letters 39, no 25 (2003) : 1820. http://dx.doi.org/10.1049/el:20031187.
Texte intégralWeingarten, K. J., U. Keller, D. C. Shannon et R. W. Wallace. « Two-gigahertz repetition-rate, diode-pumped, mode-locked Nd:YLF laser ». Optics Letters 15, no 17 (1 septembre 1990) : 962. http://dx.doi.org/10.1364/ol.15.000962.
Texte intégralKemp, A. J., B. Stormont, B. Agate, C. T. A. Brown, U. Keller et W. Sibbett. « Gigahertz repetition-rate from directly diode-pumped femtosecond Cr:LiSAF laser ». Electronics Letters 37, no 24 (2001) : 1457. http://dx.doi.org/10.1049/el:20011008.
Texte intégralYu, C. X., H. A. Haus, E. P. Ippen, W. S. Wong et A. Sysoliatin. « Gigahertz-repetition-rate mode-locked fiber laser for continuum generation ». Optics Letters 25, no 19 (1 octobre 2000) : 1418. http://dx.doi.org/10.1364/ol.25.001418.
Texte intégralSong, Jiazheng, Yuanshan Liu et Jianguo Zhang. « L-band mode-locked femtosecond fiber laser with gigahertz repetition rate ». Applied Optics 58, no 27 (18 septembre 2019) : 7577. http://dx.doi.org/10.1364/ao.58.007577.
Texte intégralCheng, Huihui, Wei Lin, Zhengqian Luo et Zhongmin Yang. « Passively Mode-Locked Tm3+-Doped Fiber Laser With Gigahertz Fundamental Repetition Rate ». IEEE Journal of Selected Topics in Quantum Electronics 24, no 3 (mai 2018) : 1–6. http://dx.doi.org/10.1109/jstqe.2017.2657489.
Texte intégralSchellhorn, Martin, Marc Eichhorn, Christelle Kieleck et Antoine Hirth. « High repetition rate mid-infrared laser source ». Comptes Rendus Physique 8, no 10 (décembre 2007) : 1151–61. http://dx.doi.org/10.1016/j.crhy.2007.09.007.
Texte intégralThèses sur le sujet "Gigahertz repetition rate laser source"
Messineo, Giuseppe. « The MIR experiment : quantum vacuum and dynamical Casimir effect ». Doctoral thesis, Università degli studi di Trieste, 2011. http://hdl.handle.net/10077/4572.
Texte intégralThis thesis concerns one of the few low energy experimental efforts aiming to test Quantum Electrodynamics. The experiment MIR (Motion Induced Radiation) studies the quantum vacuum in the presence of accelerated boundaries. According to Quantum Electrodynamics, a non-uniformly accelerated mirror in vacuum feels a friction force due to the interaction with the vacuum photons. As a consequence, real photons are produced in the process, which is known as dynamical Casimir effect. The radiated energy is emitted at the expense of the mechanical energy of the mirror. The effect has never been observed experimentally, since it is very feeble. Only recently a few experimental approaches have been proposed. The theory of the dynamical Casimir effect has been treated extensively in literature. According to the models proposed, for harmonic oscillations the effect is proportional to the oscillation frequency. As all the papers refer to frequencies of the order of a gigahertz, it is not possible to tackle the problem of obtaining a moving boundary with a purely mechanical approach, for example employing piezoelectric transducers or acoustic excitations, due to the large amount of energy required to keep a massive object in motion. A solution to this problem was proposed at the end of the 80's and has been adopted in the MIR experiment. In this framework the moving boundary is a semiconductor slab that switches periodically from complete transparency to total reflection when illuminated by a train of laser pulses. In this way one obtains a time variable mirror which mimics a physical oscillation, without the burden of overcoming the inertia of the mirror. Even so, the number of photons expected is extremely small. The MIR experimental strategy to enhance the photon production is to have the mirror as the wall of a resonating cavity. In this case, if the repetition rate of the laser is about twice a resonance frequency of the cavity, a parametric amplification process occurs, resulting in an enhancement of the number of photons by a factor which depends on the Q-value of the cavity. To this end, superconducting cavities are employed in the experiment.
Questa tesi riguarda uno dei pochi esperimenti di bassa energia dedicati allo studio dell'Elettrodinamica Quantistica. L'esperimento MIR (Motion Induced Radiation) studia il vuoto quantistico in presenza di condizioni al contorno accelerate. Secondo l'Elettrodinamica Quantistica, uno specchio non uniformemente accelerato nel vuoto risente di una forza di attrito dovuta all'interazione con i fotoni del vuoto. In conseguenza di ciò in questo processo, noto come effetto Casimir dinamico, vi è produzione di fotoni reali. L'energia irradiata viene emessa a scapito dell'energia meccanica dello specchio. L'effetto è molto debole e non è mai stato osservato sperimentalmente. Solo di recente sono stati proposti alcuni approcci sperimentali, mentre gli aspetti teorici sono stati trattati ampiamente in letteratura. Secondo i modelli proposti, nel caso di oscillazioni armoniche l'effetto è proporzionale alla frequenza di oscillazione. Poiché tutti gli articoli fanno riferimento a frequenze dell'ordine di un gigahertz, con un approccio puramente meccanico, ad esempio impiegando trasduttori piezoelettrici o eccitazioni acustiche, non è possibile risolvere il problema di ottenere uno specchio in movimento a causa della grande quantità di energia richiesta per mantenere un oggetto massivo in moto. Una soluzione a questo problema è stata proposta alla fine degli anni '80 ed è stata adottata nell'esperimento MIR. L'idea è che la parete in movimento possa essere sostituita da un lastra di semiconduttore che periodicamente passa da uno stato di totale trasparenza ad uno di alta riflettività, per illuminazione da parte di un treno di impulsi laser. In tal modo è possibile ottenere un specchio variabile nel tempo che riproduce una oscillazione fisica, senza la necessità di superare l'inerzia dello specchio. Anche in questo caso tuttavia, il numero di fotoni previsto è estremamente ridotto. La strategia sperimentale di MIR per aumentare la produzione di fotoni è quella di utilizzare lo specchio variabile come parete di una cavità risonante. Se la frequenza di ripetizione del laser è circa due volte la frequenza di risonanza della cavità, si verifica un processo di amplificazione parametrica, con un conseguente aumento del numero di fotoni prodotti. Poiché questo incremento dipende dal Q-valore della cavità, nell'esperimento vengono impiegate cavità superconduttrici.
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Häring, Reto Andreas. « Miniature pulsed laser sources : repetition rates from Kilohertz to Gigahertz / ». Zürich, 2001. http://e-collection.ethbib.ethz.ch/show?type=diss&nr=14454.
Texte intégralGao, Ying [Verfasser], et Jörg [Akademischer Betreuer] Schreiber. « High repetition rate laser driven proton source and a new method of enhancing acceleration / Ying Gao ; Betreuer : Jörg Schreiber ». München : Universitätsbibliothek der Ludwig-Maximilians-Universität, 2020. http://d-nb.info/1214180353/34.
Texte intégralBonamis, Guillaume. « Conception et réalisation d’une source laser femtoseconde GHz et applications au régime d’ablation très haute cadence ». Thesis, Bordeaux, 2020. http://www.theses.fr/2020BORD0293.
Texte intégralThese last two decades, femtosecond laser technology has gained considerably in terms of maturity and reliability. These laser pulses enable materials micro-machining with minimal thermal collateral effects, thus allowing to work with an outstanding precision, even on materials highly sensitive to temperature. Nevertheless, the penetration of femtosecond processing into the industrial manufacturing market is limited due to an insufficient productivity. The current strategies consist of optimizing the processes on the one hand and increasing the average power of these laser sources on the other hand. Another way suggests increasing the femtosecond ablation process efficiency by delivering bursts of low-energy pulses instead of one highly energetic pulse.Recent works showed that using bursts of pulses at repetition rates on the order of GHz allows to reach ablation rates one order of magnitude higher than the ones obtained by standard femtosecond pulse machining. Nevertheless, these promising results are controversial, as other works point out levels of efficiency lower than expected, added to collateral thermal damages on the machined materials. A thorough study of this new ablation regime is thus necessary to ensure that its interest is justified on the one hand, and to point out the optimal configurations of its use on the other hand. Several optical oscillators delivering bursts of femtosecond pulses at GHz-level repetition rates and laser amplifiers have been developed to this purpose. These innovating laser systems benefit from great flexibility in terms of reachable laser parameters (pulse repetition rate and energy, number of pulses per burst notably). This flexibility allowed us to perform a thorough study of the GHz-ablation regime by numerous machining experiments on several materials of industrial interest. This study points out the influence of the different laser parameters and thus to explain the variety of results related to GHz-ablation and to guide the use of this regime under favorable conditions to reach an efficient and high-quality machining
Wu, Qian-Ying, et 吳芊縈. « Using a grating-coupled passively mode-locked quantum-dot laser to achieve a low repetition-rate and wavelength-tunable ultrashort pulse source at 1.3μm range ». Thesis, 2013. http://ndltd.ncl.edu.tw/handle/gy745r.
Texte intégral國立交通大學
電子工程學系 電子研究所
102
In this thesis, an external grating-coupled two-section J-shape waveguide quantum dot device was used as a multi-functional light source. The wavelength tuning range was over 140nm in 1.3 μm range when the two sections were shorted and in the same forward bias. The lasing wavelength can be continuously tuned from the ground state to the excited state of the quantum dots, while the linewidth was smaller than 0.1 nm, and the side mode suppression ratio (SMSR) is about 40 dB. When one of the two sections was reversely biased as a saturable absorber, the laser was passively mode-locked. The tuning range of the lasing wavelength was about 33 nm and 30 nm for the ground state and the excited state, respectively. The pulsewidth depended on the injection current and the absorber bias and was varied from 10 ps to 30 ps. With changing the length of the external cavity, the repetition rate was continuously tuned from 2 GHz to 87.2 MHz. To the best of our knowledge, the repetition rate of 87.2 MHz was the lowest frequency achieved to date for any passively mode-locked semiconductor laser, which can make major contribution to medical and bio-imaging applications.
Chapitres de livres sur le sujet "Gigahertz repetition rate laser source"
Turcu, I. C. E., G. J. Tallents, M. S. Schulz et A. G. Michette. « High Repetition Rate Laser-Plasma X-Ray Source for Microscopy ». Dans X-Ray Microscopy III, 54–57. Berlin, Heidelberg : Springer Berlin Heidelberg, 1992. http://dx.doi.org/10.1007/978-3-540-46887-5_9.
Texte intégralEgbert, A., B. Mader, B. Tkachenko, C. Fallnich et B. N. Chichkov. « Compact ultrashort hard-x-ray source driven by high-repetition rate femtosecond laser pulses ». Dans Ultrafast Phenomena XIII, 137–39. Berlin, Heidelberg : Springer Berlin Heidelberg, 2003. http://dx.doi.org/10.1007/978-3-642-59319-2_42.
Texte intégralZhavoronkov, N., Y. Gritsai, P. Mikheev, A. Savelev, R. Bernath, G. Korn et T. Elsaesser. « High Repetition Rate Femtosecond Laser Driven Hard X-Ray Source and its Application for Diffraction Experiments ». Dans Springer Series in OPTICAL SCIENCES, 325–28. New York, NY : Springer New York, 2004. http://dx.doi.org/10.1007/978-0-387-34756-1_41.
Texte intégralHada, Masaki, et Jiro Matsuo. « Development of Ultrafast Pulse X-ray Source in Ambient Pressure with a Millijoule High Repetition Rate Femtosecond Laser ». Dans Zero-Carbon Energy Kyoto 2009, 300–305. Tokyo : Springer Japan, 2010. http://dx.doi.org/10.1007/978-4-431-99779-5_47.
Texte intégralActes de conférences sur le sujet "Gigahertz repetition rate laser source"
Wang, Yan, Yizhou Liu, Zhigang Zhang et Franz X. Kartner. « 97-Watt, 1.08-Gigahertz repetition rate, Femtosecond Yb:fiber Laser Source ». Dans Conference on Lasers and Electro-Optics/Pacific Rim. Washington, D.C. : OSA, 2020. http://dx.doi.org/10.1364/cleopr.2020.c2a_2.
Texte intégralLi, Duo, Umit Demirbas, Jonathan R. Birge, Gale S. Petrich, Leslie A. Kolodziejski, Alphan Sennaroglu, Franz X. Kärtner et James G. Fujimoto. « Diode-pumped Gigahertz Repetition Rate Femtosecond Cr:LiSAF Laser ». Dans Conference on Lasers and Electro-Optics. Washington, D.C. : OSA, 2010. http://dx.doi.org/10.1364/cleo.2010.ctuk3.
Texte intégralWANG, HE, Yiming Xu, Stefan Ulonska, Predrag Ranitovic et Robert A. Kaindl. « High repetition-rate XUV source for ultrafast photoemission ». Dans Laser Science. Washington, D.C. : OSA, 2013. http://dx.doi.org/10.1364/ls.2013.lth1i.2.
Texte intégralChan, Tian Seng, M. H. A. Wahid et P. Poopalan. « Gigahertz repetition rate ultrashort laser pulses from coherent external Fabry-Pérot cavity ». Dans THE 2ND INTERNATIONAL CONFERENCE ON APPLIED PHOTONICS AND ELECTRONICS 2019 (InCAPE 2019). AIP Publishing, 2020. http://dx.doi.org/10.1063/1.5142117.
Texte intégralChernikov, S. V., J. R. Taylor, P. V. Mamyshev et E. M. Dianov. « Generation of a Soliton Pulse Train in an Optical Fibre Using Two Cw, Single-Frequency, Diode Lasers ». Dans International Conference on Ultrafast Phenomena. Washington, D.C. : Optica Publishing Group, 1992. http://dx.doi.org/10.1364/up.1992.thc8.
Texte intégralHamrouni, Marin, François Labaye, Norbert Modsching, Valentin J. Wittwer et Thomas Südmeyer. « Powerful Sub-100-fs Diode-Pumped Solid-State Laser Oscillator Operating at Gigahertz Repetition Rate ». Dans CLEO : Science and Innovations. Washington, D.C. : Optica Publishing Group, 2022. http://dx.doi.org/10.1364/cleo_si.2022.sf4e.3.
Texte intégralGolz, Torsten, Gregor Indorf, Mihail Petev, Jan-Heye Buss, Jan-C. Deinert, Ivanka Grguras, Michael Schulz et Robert Riedel. « High repetition rate extreme ultraviolet source and Terahertz driver laser ». Dans CLEO : Science and Innovations. Washington, D.C. : OSA, 2021. http://dx.doi.org/10.1364/cleo_si.2021.sth2b.4.
Texte intégralAnderson, T., I. V. Tomov et P. M. Rentzepis. « High repetition rate picosecond x-ray source ». Dans OSA Annual Meeting. Washington, D.C. : Optica Publishing Group, 1992. http://dx.doi.org/10.1364/oam.1992.mp5.
Texte intégralSheng, W. D., X. F. Li, H. W. Liu, X. J. Fang et J. Q. Yao. « High Repetition Rate LDP-SHG Nd:YAG Laser ». Dans Solid State Lasers : Materials and Applications. Washington, D.C. : Optica Publishing Group, 1997. http://dx.doi.org/10.1364/sslma.1997.tuc4.
Texte intégralNatile, Michele, Anna Golinelli, Florent Guichard, Marc Hanna, Yoann Zaouter, Ronic Chiche et Patrick Georges. « High repetition rate CEP-stable Yb-doped laser source for attoscience ». Dans High Intensity Lasers and High Field Phenomena. Washington, D.C. : OSA, 2020. http://dx.doi.org/10.1364/hilas.2020.hf1b.4.
Texte intégralRapports d'organisations sur le sujet "Gigahertz repetition rate laser source"
Anderson, Scott L. DURIP 99 High Repetition Rate Laser Vaporization Source for Cluster Ion Beam Deposition. Fort Belvoir, VA : Defense Technical Information Center, août 2000. http://dx.doi.org/10.21236/ada381571.
Texte intégralBayramian, A. High Energy Repetition-Rate Average-Power Laser Driver (HERALD) for the Dynamic Compression Sector (DCS) at the Advanced Photon Source (APS). Office of Scientific and Technical Information (OSTI), juin 2013. http://dx.doi.org/10.2172/1088458.
Texte intégralMacDonald, James D., Aharon Abeliovich, Manuel C. Lagunas-Solar, David Faiman et John Kabshima. Treatment of Irrigation Effluent Water to Reduce Nitrogenous Contaminants and Plant Pathogens. United States Department of Agriculture, juillet 1993. http://dx.doi.org/10.32747/1993.7568092.bard.
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