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[81] Bao, Y., Dai, L., Jiang, J., Huang, Z., Huang, Q., Rozhin, A., Mou, C., Humidity Resistant Carbon Nanotubes-Styrene Methyl-Methacrylate Polymer Composite for Ultrafast Laser. Adv. Optical Mater. 2022, 2200461.
[ 80 ] William Renard , Cl é ment Chan , Antoine Dubrouil , J é r ô me Lhermite, Giorgio Santarelli and Romain Royon, “Agile femtosecond synchronizable laser source from a gated CW laser,” Laser Phys. Lett. 19, 075105, (2022).
[79] Atsushi Ishizawa, Kota Kawashima, Rai Kou, Xuejun Xu, Tai Tsuchizawa, Takuma Aihara, Koki Yoshida, Tadashi Nishikawa, Kenichi Hitachi, Guangwei Cong, Noritsugu Yamamoto, Koji Yamada, and Katsuya Oguri, “Direct f-3f self-referencing using an integrated silicon-nitride waveguide,” Opt. Express 30, 5265-5273 (2022).
[78] D. Marion, G. Duchateau, and J.-C. Delagnes, “Control of nonlinear processes using versatile random photonic sources: Application to the energy deposition in a dielectric material,” Phys. Rev. A 105, 013525 (2022).
[77] Yu Zhang, Yaoyao Qi, Song Yang, Nannan Luan, Zhenxu Bai, Jie Ding, Yulei Wang, Zhiwei Lu,
High pulse energy, narrow-linewidth all-fiber 1064 nm picosecond master oscillator power amplifier system, Optics & Laser Technology, Volume 147, p.107636 (2022).
[76] Xuzhuo Jia, Yuanqi Song, Li Yan, Qimeng Lin, Lei Hou, Xiaoqiang Feng and Jintao Bai, “Yb-doped polarization-maintaining femtosecond fiber laser using Gires–Tournois interferometers for dispersion management,” Appl. Phys. Express 14 112007 (2021).
( 75 ) فيكتور ديستلر ، فريدريك مولر ، بنيامين يلدز ، ماركو بلوتنر ، سي . sar Jauregui, Till Walbaum, and Thomas Schreiber, “Experimental analysis of Raman-induced transverse mode instability in a core-pumped Raman fiber amplifier,” Opt. Express 29, 16175-16181 (2021).
[74] Y. W. Lee, J. Y. Chuang, C. C. Lin, M. C. Paul, S. Das, and A Dhar, “High-efficiency picosecond mode-locked laser using a thulium-doped nanoengineered yttrium-alumina-silica fiber as the gain medium,” Opt. Express 29, 14682-14693 (2021).
[73] Lee, YW., Chen, CM., Chuang, WH. et al. Highly efficient mode-locked and Q-switched Er3+-doped fiber lasers using a gold nanorod saturable absorber. Sci Rep 11, 20079 (2021).
[72] Pia Fuertjes, Lorenz von Grafenstein, Dennis Ueberschaer, Chao Mei, Uwe Griebner, and Thomas Elsaesser, “Compact OPCPA system seeded by a Cr:ZnS laser for generating tunable femtosecond pulses in the MWIR,” Opt. Lett. 46, 1704-1707 (2021).
[71] Paul Repgen, Generation of High-Energy Pulses by Managing the Kerr-Nonlinearity in Fiber-Based Laser Amplifiers, Dissertation (2021).
[70] T. Zhou, Q. Du, D. Li, E. Esarey, C. Schroeder, C. Geddes, and R. Wilcox, “Distributed Spectral Filtering for Ultrafast Fiber Lasers,” in Laser Congress 2020 (ASSL, LAC), P. Schunemann, C. Saraceno, S. Mirov, S. Taccheo, J. Nilsson, A. Petersen, D. Mordaunt, and J. Trbola, eds., OSA Technical Digest (Optical Society of America, 2020), paper JTu5A.11.
( 69 ) Rezki Becheker , Mohamed Touil , Said Idlahcen , Mincheng Tang , Adil Haboucha , Benoit Barviau , Fr é d é ric Grisch, Patrice Camy, Thomas Godin, and Ammar Hideur, “High-energy normal-dispersion fiber optical parametric chirped-pulse oscillator,” Opt. Lett. 45, 6398-6401 (2020)
[68] Zhang, Z., Han, H., Tian, W. et al. A fully stabilized low-phase-noise Kerr-lens mode-locked Yb:CYA laser frequency comb with an average power of 1.5 W. Appl. Phys. B 126, 134 (2020).
( 67 ) Victor Distler , Friedrich M ö ller, Maximilian Strecker, Gonzalo Palma-Vega, Till Walbaum, and Thomas Schreiber, “Transverse mode instability in a passive fiber induced by stimulated Raman scattering,” Opt. Express 28, 22819-22828 (2020)
( 66 ) Oliver de vries , Marco Pl ö tner , Florian Christaller , Hao Zhang , Annika Belz , Benjamin Heinrich , Harald K ü bler , Robert L ö w , Tilman Pfau , Till Walbaum , Thomas Schreiber , and Andreas T ü nnermann , “ Highly Customized 1010 ” nm, ns-pulsed Yb-doped fiber amplifier as a key tool for on-demand single-photon generation,” Opt. Express 28, 17362-17373 (2020)
[65] Paul Repgen, Benedikt Schuhbauer, Moritz Hinkelmann, Dieter Wandt, Andreas Wienke, Uwe Morgner, J سومر rg Neumann, and Dietmar Kracht, “Mode-locked pulses from a Thulium-doped fiber Mamyshev oscillator,” Opt. Express 28, 13837-13844 (2020)
[64] Craig Ingram, Huy Tuong Cao, Sebastian Ng, Daniel D. Brown, David Ottaway, Peter Veitch, Adam Gambell, Nikita Simakov, Alexander Hemming, “High precision measurement of optical absorption in low-OH fused silica at 2 micron,” Proc. SPIE 11200, AOS Australian Conference on Optical Fibre Technology (ACOFT) and Australian Conference on Optics, Lasers, and Spectroscopy (ACOLS) 2019, 1120031 (30 December 2019)
( 63 ) O . De Vries , M . Pl ö tner , T . Schreiber , R . Eberhardt , A . T ü nnermann, „Fiber lasers: a power-scalable coherent light source for applications in space“,
[62] T. P. Butler, N. Lilienfein, J. Xu, N. Nagl, C. Hofer, D. Gerz, K. F. Mak, C. Gaida, T. Heuermann, M. Gebhardt, J. Limpert, F. Krausz and I. Pupeza, Multi-octave spanning, Watt-level ultrafast mid-infrared source, Journal of Physics: Photonics, Volume 1, Number 4 (2019)
[61] Yu Li, Longfei Wang, Meisong Liao, Long Zhang, Wanjun Bi, Tianfeng Xue, Yinyao Liu, Renli Zhang, Yasutake Ohishic, “Suspended-core fluoride fiber for broadband supercontinuum generation,” Optical Materials, Volume 96, October 2019, 109281
( 60 ) Masaki Tokurakawa , Hiromu Sagara , and Henrik T ü nnermann, “All-normal-dispersion nonlinear polarization rotation mode-locked Tm:ZBLAN fiber laser,” Opt. Express 27, 19530-19535 (2019).
[59] Nathalie Nagl, Ka Fai Mak, Qing Wang, Vladimir Pervak, Ferenc Krausz, and Oleg Pronin, “Efficient femtosecond mid-infrared generation based on a Cr:ZnS oscillator and step-index fluoride fibers,” Opt. Lett. 44, 2390-2393 (2019).
[58] S. Kuhn, S. Hein, C. Hupel, J. Nold, F. Stutzki, N. Haarlammert, T. Schreiber, R. Eberhardt, A. T ش > ? nnermann, “High-power fiber laser materials: influence of fabrication methods and codopants on optical properties,” Proc. SPIE 10914, Optical Components and Materials XVI, 1091405 (27 February 2019).
[57] Seidel, Marcus (2018): A new generation of high-power, waveform controlled, few-cycle light sources. Dissertation, LMU M ü nchen : Fakult ä t f ü r Physik
[56] Ruihong Dai, Yafei Meng, Yao Li, Jiarong Qin, Shining Zhu, and Fengqiu Wang, “Nanotube mode-locked, wavelength and pulsewidth tunable thulium fiber laser,” Opt. Express 27, 3518-3527 (2019).
[55] M. Seidel, X. Xiao and A. Hartung, “Solid-Core Fiber Spectral Broadening at Its Limits,” in IEEE Journal of Selected Topics in Quantum Electronics, vol. 24, no. 5, pp. 1-8, Sept.-Oct. 2018.
[54] Li, F., Yang, Z., Wang, Y., Lv, Z., Wei, Y., Wang, X., … & Zhao, W. (2018). Nonlinear compression of ultrashort-pulse laser to 36fs with 556MW peak power. IEEE Photonics Technology Letters.
[53] Yang, K., Zheng, S., Wu, Y., Ye, P., Huang, K., Hao, Q., & Zeng, H. (2018). Low-repetition-rate all-fiber integrated optical parametric oscillator for coherent anti-Stokes Raman spectroscopy. Optics Express, 26(13), 17519-17528.
[52] Tang, M., Becheker, R., Hanzard, P. H., Tyazhev, A., Oudar, J. L., Mussot, A., … & Hideur, A. (2018). Low Noise High-Energy Dissipative Soliton Erbium Fiber Laser for Fiber Optical Parametric Oscillator Pumping. Applied Sciences, 8(11), 2161.
[51] Becheker, R., Tang, M., Hanzard, P. H., Tyazhev, A., Mussot, A., Kudlinski, A., Hideur, A. “High-energy dissipative soliton-driven fiber optical parametric oscillator emitting at 1.7 ميكرومتر " الليزر رسائل فيزيائية ، 15 ( 11 ) ، 115103 ( 2018 ) .
( 50 ) Delagnes , J . C . , Royon , R . , Lhermite , J . , Santarelli , G . , Mu ñ a oz, H., Grosz, T., Cormier, E. “High-power widely tunable ps source in the visible light based on four wave mixing in optimized photonic crystal fibers,” Opt. Expr. 26(9), 11265-11275 (2018).
[49] H. Sagara, A. Suzuki, S. KItajima, and M. Tokurakawa, “Two micron All-normal-dispersion NPR mode-locked Tm:ZBLAN fiber laser,” in Laser Congress 2018 (ASSL), OSA Technical Digest (Optical Society of America, 2018), paper ATu2A.25.
[48] Niu, F., Li, J., Yang, W., Zhang, Z., & Wang, A. “Fiber-Based High-Energy Femtosecond Pulses Tunable From 920 to 1030 nm for Two-Photon Microscopy,” IEEE Photonics Technology Letters, 30(16), 1479-1482 (2018).
[47] Zaharit Refaeli, Yariv Shamir, Atara Ofir, Gilad Marcus, “Nearly fully compressed 1053 nm pulses directly obtained from 800 nm laser-seeded photonic crystal fiber below zero dispersion point”, Proc. SPIE 10516, Nonlinear Frequency Generation and Conversion: Materials and Devices XVII, 1051607 (15 February 2018).
[46] Jinwei Zhang, Ka Fai Mak, Nathalie Nagl, Marcus Seidel, Dominik Bauer, Dirk Sutter, Vladimir Pervak, Ferenc Krausz & Oleg Pronin, “Multi-mW, few-cycle mid-infrared continuum spanning from 500 to 2250 سم - 1 " ، الضوء : العلوم والتطبيقات 7 , 17180 ( 2018 ) .
( 45 ) O . De Vries , T . Schreiber , R . Eberhardt , A . T ü nnermann , M . Windm ü ller , J . Riedel , M . R öß ler, F. Kolb, “Design optimization of fiber amplifiers exposed to high gamma-radiation doses,” Proc. SPIE 10562, International Conference on Space Optics — ICSO 2016, 105620M (25 September 2017).
[44] Hao Luo, Li Zhan, Zhiqiang Wang, Liang Zhang, Cheng Feng, and Xuehao Shen, “All-Fiber Generation of Sub-30 fs Pulses at 1.3-μm via Cherenkov Radiation With Entire Dispersion Management,” J. Lightwave Technol. 35, 2325-2330 (2017)
( 43 ) Joachim Buldt , Michael M ü ller , Robert Klas , Tino Eidam , Jens Limpert , and Andreas T ü ll . nnermann, “Temporal contrast enhancement of energetic laser pulses by filtered self-phase-modulation-broadened spectra,” Opt. Lett. 42, 3761-3764 (2017).
( 42 ) Moritz Hinkelmann , Dieter Wandt , Uwe Morgner , J ö rg Neumann, and Dietmar Kracht, “Mode-locked Ho-doped laser with subsequent diode-pumped amplifier in an all-fiber design operating at 2052 nm,” Opt. Express 25, 20522-20529 (2017).
( [ 41 ] ) ماركو بلو . tner, Victor Bock, Tim Schultze, Franz Beier, Thomas Schreiber, Ramona Eberhardt, and Andreas T ش > ? nnermann, “High power sub-ps pulse generation by compression of a frequency comb obtained by a nonlinear broadened two colored seed,” Opt. Express 25, 16476-16483 (2017).
[40] L. Lavenu, M. Natile, F. Guichard, Y. Zaouter, M. Hanna, E. Mottay, and P. Georges, “High-energy few-cycle Yb-doped fiber amplifier source based on a single nonlinear compression stage,” Opt. Express 25, 7530-7537 (2017).
( 39 ) M . Gebhardt , C . Gaida , F . Stutzki , S . H ä drich , C . Jauregui , J . Limpert , and A . T ü nnermann , " high average power nonlinear compression to 4 غيغاواط ، sub - 50 خ م م م م م خ م م م م م م م م 8207
( 38 ) Steven H ä drich , Marco Kienel , Michael M ü r . ller, Arno Klenke, Jan Rothhardt, Robert Klas, Thomas Gottschall, Tino Eidam, Andr ( ) S . Drozdy , P é ter J ó j á rt , Zolt á n Varallyay , Eric Cormier , K á roly Osvay , Andreas T ü nnermann , and Jens Limpert , “ Energetic sub-2-cycle laser with216 W average power ” , Opt . Lett 41 , 4332-4335 ( 2016 ) .
( 37 ) Martin Gebhardt , Christian Gaida , Fabian Stutzki , Steffen H ä drich, Cesar Jauregui, Jens Limpert, Andreas Tuennermann, “Self-compression to 24 MW peak power in a fused silica solid-core fiber using a high-repetition rate thulium-based fiber laser system,” Proc. SPIE 9728, Fiber Lasers XIII: Technology, Systems, and Applications, 97282H (March 11, 2016).
( 36 ) D . Gaponov , L . Lavoute , S . F é vrier , A . Hideur , N . Ducros , “ 2 ميكروغرام . m all-fiber dissipative soliton master oscillator power amplifier.” Proc. SPIE 9728, Fiber Lasers XIII: Technology, Systems, and Applications, 972834 (March 11, 2016).
( 35 ) T . Gottschall , J . Limpert , and A . T . nnermann, “Widely tunable optical parametric oscillator based on four-wave mixing,” in Advanced Solid State Lasers, OSA Technical Digest (online) (Optical Society of America, 2015), paper ATu4A.9.
( 34 ) C . Gaida , M . Gebhardt , F . Stutzki , C . Jauregui , J . Limpert , and A . T ü nnermann , “ Self-Compression in a solid fiber to 24 mw peak power with few-cycle pulses at 2 1 1 1 1 1 1 1 40 wangth 51 60
[33] D. A. Gaponov, R. Dauliat, D. Darwich, T. Mansuryan, R. Jamier, S. Grimm, K. Schuster, and P. Roy, “High-power passively mode-locked dissipative soliton fiber laser featuring cladding-pumped non-CVD thulium-doped fiber,” J. Opt. Soc. Am. B 32, 1656-1659 (2015)
( 32 ) Thomas Gottschall , Tobias Meyer , Michael Schmitt , J ü rgen Popp , Jens Limpert , and Andreas T ü r . nnermann, “Four-wave-mixing-based optical parametric oscillator delivering energetic, tunable, chirped femtosecond pulses for non-linear biomedical applications,” Opt. Express 23, 23968-23977 (2015)
( 31 ) M . Gebhardt , C . Gaida , S . H ä drich , F . Stutzki , C . nnermann, “Nonlinear compression of an ultrashort-pulse thulium-based fiber laser to sub-70 fs in Kagome Photonic Crystal Fiber , “ Opt . Lett 40 , 2770-2773 ( 2015 )
( 30 ) Martin Gebhardt , Christian Gaida , Fabian Stutzki , Stefen H ä drich , Cesar Jauregui , Jens Limpert , and Andreas T ü r . nnermann, “Impact of atmospheric molecular absorption on the temporal and spatial evolution of ultra-short optical pulses,” Opt. Express 23, 13776-13787 (2015)
( 29 ) M . Gebhardt , C . Gaida , F . Stutzki , C . Jauregui , J . Limpert , and A . T ü nnermann, “Sub-200 fs, nJ-level stretched-pulse thulium-doped fiber oscillator at 23MHz repetition rate,” in Advanced Solid State Lasers, OSA Technical Digest (online) (Optical Society of America, 2014), paper AM5A.43.
[28] F. Beier, H.-J. Otto, C. Jauregui, O. de Vries, T. Schreiber, J. Limpert, R. Eberhardt, and A. T N ü nnermann , “ 1009 nm continuous-wave ytterbium-doped fiber amplifier emitting 146 w ” , Opt . Lett . 39 , 3725-3727 ( 2014 )
[27] Tongxiao Jiang, Aimin Wang, Guizhong Wang, Wei Zhang, Fuzeng Niu, Chen Li, and Zhigang Zhang, “Tapered photonic crystal fiber for simplified Yb:fiber laser frequency comb with low pulse energy and robust fceo singals,” Opt. Express 22, 1835-1841 (2014).
[26] Niu, F., Jiang, T., Wang, A., Wang, G., Li, C., & Zhang, Z. (2014, July). Design and fabrication of tapered photonic crystal fiber for astro-combs applications. In Optical Fibre Technology, 2014 OptoElectronics and Communication Conference and Australian Conference on (pp. 709-711). IEEE.
[25] Niu, F., Jiang, T., Wang, G., Li, C., Wang, A., & Zhang, Z. (2014, June). Green-enhanced super-continuum generation in a tapered photonic crystal fiber for efficient ك ceo detection. In Lasers and Electro-Optics (CLEO), 2014 Conference on (pp. 1-2). IEEE.
[24] Jiang, T., Wang, G., Wang, A., Zhang, W., Niu, F., Li, C., & Zhang, Z. (2014, July). Tapered photonic crystal fiber for simplified 500MHz Yb: Fiber laser frequency comb with no amplifier. In Optical Fibre Technology, 2014 OptoElectronics and Communication Conference and Australian Conference on (pp. 120-122). IEEE.
[23] Haxsen, F., Wienke, A., Wandt, D., Neumann, J., & Kracht, D. (2014). Tm-doped mode-locked fiber lasers. Optical Fiber Technology, 20(6), 650-656.
[22] Chi, J., Li, P., Liang, B., Yao, Y., Hu, H., Zhang, G., … & Ma, C. (2014). 100-W 430-ps all-fiber picosecond laser by using 10-/130-μm ytterbium-doped double-clad fiber and its application in SCS. Applied Physics B, 1-9.
[21] R. A. Sims, P. Kadwani, H. Ebendorff-Heideprem, L. Shah, T. M. Monro, M. Richardson, “Chirped pulse amplification in single mode Tm:fiber using a chirped Bragg grating,” Applied Physics B, May 2013, Volume 111, Issue 2, pp 299-304
[20] Tongxiao Jiang, Guizhong Wang, Wei Zhang, Chen Li, Aimin Wang, and Zhigang Zhang, “Octave-spanning spectrum generation in tapered silica photonic crystal fiber by Yb:fiber ring laser above 500 MHz,” Opt. Lett. 38, 443-445 (2013).
[19] J. Lecourt, S. Boivinet, and Y. Hernandez, “All-normal dispersion, all-fibered, PM mode-locked laser and its modeling,” in International Photonics and Optoelectronics Meetings, OSA Technical Digest (online) (Optical Society of America, 2012), paper STh4A.03.
[18] Terniche, S., et al. “ETUDE DE LA PROPAGATION D’UNE IMPULSION COURTE EN CAVITE LASER AVEC UN LOGICIEL DE SIMULATION NUMERIQUE.” Journal of Fundamental and Applied Sciences 4.1 (2012): 66-73.
[17] Anthony Bertrand ; Flavien Li é geois ; Yves Hernandez and Domenico Giannone “Efficient high-power narrow-linewidth all-fibred linearly polarized ytterbium laser source”, Proc. SPIE 8433, Laser Sources and Applications, 84330F (June 1, 2012).
[16] Masayuki Suzuki, Motoyoshi Baba, Shin Yoneya and Hiroto Kuroda, Efficient spectral broadening of supercontinuum in photonic crystal fiber with self-phase modulation induced by femtosecond laser pulse, Appl. Phys. Lett. 101, 191110 (2012).
[15] J. Lhermite, C. Lecaplain, G. Machinet, R. Royon, A. Hideur, and E. Cormier, “Mode-locked 0.5 μ ي الألياف الليزر في 976 نانومتر " ، opt.lett 36 3819-3821 ( 2011 )
[14] Frithjof Haxsen, Dieter Wandt, Uwe Morgner, Joerg Neumann, and Dietmar Kracht, “Pulse characteristics of a passively mode-locked thulium fiber laser with positive and negative cavity dispersion,” Opt. Express 18, 18981-18988 (2010)
[13] Michael Mielke, David Gaudiosi, Kyungbum Kim, Tolga Yilmaz, Michael Greenberg, Sha Tong, Xinhua Gu, Mark Geusen, Robert Cline, Mark Slovick, Neill Allen, Michael Manning, Barry Schuler and Steven Sapers, “Pulse and Amplifier Dynamics in High Energy Fiber Optic Ultrashort Pulse Laser Systems,” Proc. SPIE Vol. 7214 (Feb. 6, 2009).
( 12 ) S . H ä drich , J . Rothhardt , F . R ö ser , T . Gottschall , J . Limpert , and A . T ü nnermann, “Degenerate optical parametric amplifier delivering sub 30 fs pulses with 2GW peak power,” Opt. Express 16, 19812-19820 (2008)
( 11 ) ت . eidam , F . R ö ser , O . Schmidt , J . Limpert and A . T ü nnermann, “57 W, 27 fs pulses from a fiber laser system using nonlinear compression,” Applied Physics B: Lasers and Optics, Vol. 92, 1, pp. 9-12 (2008)
( 10 ) B . Ortaca , C . Lecaplain , A . Hideur , T . Schreiber , J . Limpert , and A . T ü nnermann, “Passively mode-locked single-polarization microstructure fiber laser,” Opt. Express 16, 2122-2128 (2008)
( 9 ) T . Schreiber , D . Schimpf , D . M ü ller , F . R ö ser , J . Limpert , and A . T ü nnermann, “Influence of pulse shape in self-phase-modulation-limited chirped pulse fiber amplifier systems,” J. Opt. Soc. Am. B 24, 1809-1814 (2007)
( 8 ) T . Schreiber , B . Ortaca , J . Limpert , and A . T . nnermann, “On the study of pulse evolution in ultra-short pulse mode-locked fiber lasers by numerical simulations,” Opt. Express 15, 8252-8262 (2007)
[7] C. Aguergaray, T. V. Andersen, D. N. Schimpf, O. Schmidt, J. Rothhardt, T. Schreiber, J. Limpert, E. Cormier, and A. T ش > ? nnermann, “Parametric amplification and compression to ultrashort pulse duration of resonant linear waves,” Opt. Express 15, 5699-5710 (2007)
( 6 ) B . Ortac , M . P ö tner , T . Schreiber , J . Limpert , and A . T ü nnermann, “Experimental and numerical study of pulse dynamics in positive net-cavity dispersion modelocked Yb-doped fiber lasers,” Opt. Express 15, 15595-15602 (2007)
[5] T. V. Andersen, O. Schmidt, C. Bruchmann, J. Limpert, C. Aguergaray, E. Cormier, and A. T ش > ? nnermann, “High repetition rate tunable femtosecond pulses and broadband amplification from fiber laser pumped parametric amplifier,” Opt. Express 14, 4765-4773 (2006)
( 4 ) Thomas Schreiber , Carsten K . Nielsen , B ü lend Ortac , Jens Limpert , and Andreas T ü nnermann, “Microjoule-level all-polarization-maintaining femtosecond fiber source,” Opt. Lett. 31, 574-576 (2006)
t.schreiber t.v.andersen , d.schimpf , j.limpert , and a.t ü nnermann, “Supercontinuum generation by femtosecond single and dual wavelength pumping in photonic crystal fibers with two zero dispersion wavelengths,” Opt. Express 13, 9556-9569 (2005)
( 2 ) J . Limpert , C . Aguergaray , S . Montant , I . Manek-H ö nninger, S. Petit, D. Descamps, E. Cormier, and F. Salin, “Ultra-broad bandwidth parametric amplification at degeneracy,” Opt. Express 13, 7386-7392 (2005)
( 1 ) T . Schreiber , J . Limpert , H . Zellmer , A . T . nnermann, K.P. Hansen, “High average power supercontinuum generation in photonic crystal fibers,” Optics Communications, Volume 228, Issues 1–3, 2003, Pages 71-78,
[ 0 ] J . Limpert , T . Schreiber , T . Clausnitzer , K . Z ö llner , H . J . Fuchs , E . B . Kley , H . Zellmer , and A . T ü llner nnermann, “High-power femtosecond Yb-doped fiber amplifier,” Opt. Express 10, 628-638 (2002).
إذا كان لديك أي مشاكل مع هذا البرنامج ، من فضلك قل لنا ، ونحن دائما على استعداد لمساعدتك . انظر أيضا أسئلة وأجوبة القسم لمعرفة ما هي المعلومات التي نحتاج إليها وما إذا كان هناك أي مشاكل تقنية .
يمكنك حجز الدورات عبر الإنترنت . يرجى تحديد عدد المشاركين و المحتوى الذي تريد . سوف نعود لكم مع اقتباس .

السؤال الأول :
يمكن استخدام برامج fiberdesk نبضات النانوسيكند أو الضوء المستمر ؟
من حيث المبدأ ، غير الخطية Schr ö dinger المعادلة يسمح انتقال نبضات طويلة . . . . . . . ومع ذلك ، بريليون نثر لم تتحقق . يمكن محاكاة تشتت رامان . على ضوء مستمر ، يجب أن يكون معدل تكرار تعيين وفقا لحجم الوقت بحيث الذروة ومتوسط الطاقة على قدم المساواة . بدءا من fiberdeskv5.0 ، فإنه يوفر القدرة على خلق نبض مربع الحوار ، ويوفر خيار CW تلقائيا يوازن بين معدل التكرار إلى نافذة الوقت .
وعلاوة على ذلك ، فإن عرض النطاق الترددي الطيفية تعطى من وقت القرار ( نافذة الوقت من عدد من نقاط البيانات ) . على سبيل المثال ، لأقصى عدد من نقاط البيانات ، يمكنك التعامل مع عرض النطاق الترددي ~ 100nm@1 م ، العيب هو بطيء جدا . وعلاوة على ذلك ، في غياب معادلة شرودنجر غير الخطية ، م و CW الضوء يمكن محاكاة مع قيم المعادلة التي قدمها fiberdesk البرمجيات .

السؤال الثاني :
يو القرص حماية البرمجيات لا يمكن أن تبدأ أو خطأ ؟
الناقل التسلسلي العام التشفير الكلب بعد عام 2020 لا تحتاج إلى تثبيت برنامج التشغيل ، وسوف تكون متاحة تلقائيا مع مايكروسوفت ويندوز .
ومع ذلك ، إذا كنت بحاجة إلى تثبيت الناقل التسلسلي العام سائق الكلب مشفرة ، مثل الوصول إلى صفحة المعلومات المطلوبة للإجابة على السؤال التالي ، اتبع الخطوات التالية :
0 . إزالة يو القرص وبدء تشغيل جهاز الكمبيوتر الخاص بك مع امتيازات المسؤول
1 . تحميل sentinel hasp / LDK - سطر الأوامر وقت التشغيل المثبت
2 . فك الضغط من سطر الأوامر وبدء تشغيل ملف يحتوي على haspdinst.exe لإلغاء تثبيت جميع السائقين السابقين تماما :
haspdinst -purge
3 . مرة أخرى ، تثبيت برنامج تشغيل جديد من سطر الأوامر
هاسبدينست - تركيب
4 . إدراج يو القرص ، بدء fiberdesk
إذا كنت لا تزال لديها مشاكل ، يرجى الاتصال بنا .

السؤال الثالث :
لا تزال تتلقى رسالة خطأ ؟
يرجى استخدام http : / / localhost : 1947 في متصفح الويب الخاص بك ، وإرسال لقطة من مفتاح أو وظيفة عدد لنا .

السؤال الرابع :
حتى لو كان الناقل التسلسلي العام التشفير الكلب يعمل بشكل صحيح ، fiberdesk لن تبدأ . ماذا يمكن أن أفعل ؟
أولا ، يرجى عرض المجلد
C:/Users/%USER%/AppData/Roaming/fiberdesk
و ترسل لنا ملف " u fiberdesk \\ \\ u 0.log " . بدلا من ذلك ، تبدأ fiberdesk من سطر الأوامر ( مفتاح ويندوز ثم أدخل كمد + دخول ، التبديل إلى مجلد fiberdesk وبدء fiberdesk ) . ثم إرسال لقطة من الناتج سطر الأوامر إلى الدعم ، انظر الأمثلة في الصورة .