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sales@uhightech.com
No. 186 West road, cuarta circunvalación sur, Distrito de fengtai, Beijing
La transmisión de pulsos no lineales se vuelve fácil
Fiberdesk es un software utilizado para la transmisión de pulsos lineales y no lineales. Se basa en la solución de la ecuación Schrödinger no lineal extendida a través del método de transformación de Ft paso a paso y puede combinarla con la simulación de la ecuación de velocidad.
Cada unoSoftware fiberdeskLas licencias están protegidas por perros de cifrado de hardware. Se puede ordenar como una clave USB local sin conductor para el ordenador y es necesario mantener el Estado de inserción en el ordenador mientras se ejecuta el software fiberdesk.



Última actualización: 20 de septiembre de 2022
Inserte el perro cifrado fiberdesk. Descargar el último paquete y simplemente ejecutar el ejecutable.
Enlace de descarga de fiberdesk
Los últimos paquetes de software incluyen versiones de 64 bits:
– versión 7.0 de fiberdesk
– lector Python para archivos fiberdesk, por ejemplo personalizado
– lista de funciones


[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, Clément chan, Antoine dubrouil, jérò 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] Victor distler, Friedrich möller, Benjamin yildiz, marco plötner, céntrico 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, Saïd idlahcen, mincheng tang, Adil haboucha, Benoit barviau, frédé 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 Möller 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 plötner, Florian christaller, Hao zhang, Annika belz, Benjamin heinrich, Harald kübler, Robert löw, Tilman pfau, till walbaum, Thomas schreiber, y Andreas tünnermann, "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 Sö 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. plötner, T. schreiber, R. eberhardt, A. tütner 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, y Henrik tü 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 ü 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 ünchen: Fakultät für 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 "Laser Physics letters, 15 (11), 115103 (2018).
[50] delagnes, J. c., royon, r., lhhermite, j., santarelli, g., muña 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 - CM - 1 ", luz: Science & Appliances 7, 17180 (2018).
[45] O. de vries, T. schreiber, R. eberhardt, A. tünnermann, M. windmüller, J. riedel, M. röß 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 müller, Robert klas, tino eidam, Jens limbert, y Andreas tüller 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, jö 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] marco plö tner, Victor Bock, Tim Schultze, Franz Beier, Thomas Schreiber, Ramona Eberhardt, and Andreas T ü 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. hädrich, c. jauregui, J. limbert, y A. tünnermann, "high average Power nonline Comprehension to 4 gw, subb - 50 FS pulse at 2 Mu M wavelength", opt. lett. 42, 747 - 750.
[38] Steffen hädrich, marco kienel, Michael Münch ller, Arno Klenke, Jan Rothhardt, Robert Klas, Thomas Gottschall, Tino Eidam, Andr Más drozdy, piéter jójárt, Zoltán váralkay, Eric cormier, károlly osvay, Andreas tünnermann, y Jens limbert, "energic suba - 2 - cycle laster with 216 W average power", opt. lett. 41, 4332 - 4335 (2016).
[37] Martin gebhardt, Christian gaida, Fabian stutzki, Steffen hä 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. février, A. hideur, N. ducros, "2 micras 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. limbert, y A. tüll 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. jauegui, J. limpert, y A. tünnermann, "self - Comprehension in a solid Firm to 24 MW peak power with few - cycle pulse at 2 Mu M wavelength", opt. lett. 40, 5160 - 5163 (2015)
[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, Jürgen pop, Jens limbert, y Andreas tü 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. hädrich, F. stutzki, c. jauregui, J. limbert, y A. türich 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, Steffen hädrich, César jauregui, Jens limbert, y Andreas tüdrich 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. limbert, y A. türtz 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 ünnermann, "1009 nm continuus - Wave yterbium - dupled Fiber AMPLIFIER emitting 146 Min 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 Naan 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 ; Flavin liégeois; 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 μj Faber laser a 976 nm ", 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. hädrich, J. rothhardt, F. röser, T. gottschall, J. limbert, y A. tüser nnermann, “Degenerate optical parametric amplifier delivering sub 30 fs pulses with 2GW peak power,” Opt. Express 16, 19812-19820 (2008)
[11] T. eidam, F. röser, O. schmidt, J. limbert y A. tüser 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. ortaç, c. lechaplain, A. hideur, T. schreiber, J. limbert, y A. tü nnermann, “Passively mode-locked single-polarization microstructure fiber laser,” Opt. Express 16, 2122-2128 (2008)
[9] T. schreiber, D. schimpf, D. müller, F. röser, J. limbert, y A. tüller 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. ortaç, J. limbert, y A. tü 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 ü nnermann, “Parametric amplification and compression to ultrashort pulse duration of resonant linear waves,” Opt. Express 15, 5699-5710 (2007)
[6] B. ortac, M. plötner, T. schreiber, J. limbert, y A. tütner 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 ü 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, bülend ortac, Jens limbert, y Andreas tülen nnermann, “Microjoule-level all-polarization-maintaining femtosecond fiber source,” Opt. Lett. 31, 574-576 (2006)
[3] T. schreiber, T. V. andersen, D. schimpf, J. limbert, y A. tüssen 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. limbert, c. aguergaray, S. montant, I. manek - hö 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. limbert, H. zellmer, A. tüller 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. limbert, T. schreiber, T. clausnitzer, K. zöllner, H. - J. fuchs, E. - B. kley, H. zellmer, y A. tüllner nnermann, “High-power femtosecond Yb-doped fiber amplifier,” Opt. Express 10, 628-638 (2002).
Si tiene algún problema al usar el software, Háganos saber que estamos a su disposición para ayudarlo. También consulte la Sección de preguntas y respuestas frecuentes para saber qué información necesitamos y si hay problemas técnicos.
Puede reservar cursos en línea. Por favor, indique el número de participantes y lo que le gusta. Volveremos a ofrecerle.

Pregunta 1:
¿¿ se puede usar el software fiberdesk para pulsos nanosegundos o luz continua?
En principio, la ecuación no lineal Schrödinger permite la transmisión de pulsos largos. Sin embargo, la dispersión de brillion no se logró. Se puede simular la dispersión de raman. Para la luz continua, la tasa de repetición debe establecerse en función del tamaño del tiempo para que el pico y la Potencia media sean iguales. A partir de fiberdeskv5.0, se proporciona la función del cuadro de diálogo "crear pulso", con la opción "cw", que equilibra automáticamente la tasa de repetición a la ventana de tiempo.
Además, el ancho de banda espectral se da por la resolución temporal (ventana temporal del número de puntos de datos). Por ejemplo, para el número máximo de puntos de datos, se puede procesar con un ancho de banda de ~. 100nm@1 El pulso de 80 NS de la longitud de onda central de Mu M tiene la desventaja de ser muy lento. Además, sin la ecuación Schrödinger no lineal, la luz NS y Cw se pueden simular con la ecuación de velocidad proporcionada por el software fiberdesk.

Pregunta 2:
¿¿ qué debo hacer si la protección del disco USB hace que el software no se pueda iniciar o se cometa un error?
El criptomonedo USB después de 2020 no requiere la instalación del controlador, se proporcionará automáticamente con ms windows.
Sin embargo, si es necesario instalar un controlador de perro cifrado usb, como acceder a la página de información necesaria para la próxima pregunta común, realice los siguientes pasos:
0. retire la memoria USB e inicie su computadora con permisos de administrador
1. descargar Sentinel HASP / LDK - instalación en tiempo de ejecución de la línea de órdenes
2. descomprimir desde la línea de órdenes e iniciar el archivo incluido haspdinst.exe para desinstalar completamente todos los conductores anteriores:
haspdinst -purge
3. de nuevo, desde la línea de órdenes, instale un nuevo conductor
Haspdinst - instalación
4. inserte la memoria USB y inicie fiberdesk
Si todavía tiene preguntas, Póngase en contacto con nosotros.

Pregunta 3:
¿Todavía recibiendo mensajes erróneos?
Por favor, use https: / / localhost: 1947 en su navegador web y Envíenos una captura de pantalla o número de función de la clave.

Pregunta 4:
Fiberdesk no arranca incluso si el perro cifrado USB funciona correctamente. ¿¿ qué más se puede hacer?
Primero, mira la carpeta
C:/Users/%USER%/AppData/Roaming/fiberdesk
Y envíanos el archivo "fiberdesk 0.log". Además, inicie fiberdesk desde la línea de órdenes (la tecla Windows luego ingrese "cmd" + para volver, cambie a la carpeta fiberdesk e inicie fiberdesk). A continuación, envíe una captura de pantalla de la salida de la línea de órdenes al soporte, consulte el ejemplo en la imagen.