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Relevant bibliographies by topics / Saturable pulse transformer

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Journal articles
Dissertations / Theses
Conference papers

Academic literature on the topic 'Saturable pulse transformer'

Author: Grafiati

Published: 7 September 2024

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Journal articles on the topic "Saturable pulse transformer"

1

Zhuang, Longyu, Kai Zhu, Junfeng Rao, and Jie Zhuang. "Solid-state Marx generator based on saturable pulse transformer and fast recovery diodes." Journal of Instrumentation 18, no. 10 (2023): P10036. http://dx.doi.org/10.1088/1748-0221/18/10/p10036.

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Abstract Solid-state compact Marx generator using saturable pulse transformer (SPT) and fast recovery diodes has been proposed. The primary circuit is switched by three MOSFETs connected in parallel. The SPT functions as a step-up transformer to increase the voltage amplitude and as a closing switch for the secondary circuit. Meanwhile, all the SPTs share the same magnetic core to achieve a compact structure and ensure good synchronization. The energy storage capacitors on the secondary sides are charged through the unsaturated SPT. When the SPT saturates, the capacitors firstly transfer a lit

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2

Rong, Li, and Qi Rong. "Research on pulse power based on saturable pulse transformer and magnetic switch." Journal of Engineering 2018, no. 10 (2018): 1384–88. http://dx.doi.org/10.1049/joe.2018.5026.

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Zhang, Yu, and Jinliang Liu. "High-voltage pulse modulator based on cylindrical self-coupling saturable pulse transformer and solid-state Marx generator." Laser and Particle Beams 32, no. 1 (2014): 99–108. http://dx.doi.org/10.1017/s0263034613001031.

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AbstractHigh-voltage pulse modulator has broad applications in industry. In order to pursue the qualities of compactness, solidification, and long life time, a high-voltage pulse modulator based on a helical Blumlein pulse forming line (HBPFL),a Marx generator and a self-coupling saturable pulse transformer (SPT) with fully cylindrical coaxial conductors is put forward and investigated in this paper. A new method that the fully cylindrical SPT simultaneously works as the charging pulse transformer and magnetic switch of the HBPFL is put forward and demonstrated. Traditional spark gap is substi

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Kurihara, K., S. Kobayashi, I. Satoh, et al. "Magnetic pulse compressor using saturable transformer to excite excimer lasers." Review of Scientific Instruments 63, no. 4 (1992): 2138–40. http://dx.doi.org/10.1063/1.1143180.

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Liu, Jinliang, Xuliang Fan, and Yu Zhang. "Nanosecond-range multi-pulses synchronization based on magnetic switch and saturable pulse transformer." Review of Scientific Instruments 83, no. 12 (2012): 124703. http://dx.doi.org/10.1063/1.4769086.

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Fan, Xuliang, and Jinliang Liu. "A 70 kV solid-state high voltage pulse generator based on saturable pulse transformer." Review of Scientific Instruments 85, no. 2 (2014): 024708. http://dx.doi.org/10.1063/1.4864194.

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Masugata, K., S. Tsuchida, H. Saitou, K. Yatsui, K. Shibata, and M. Shigeta. "Fast-charging Blumlein pulse forming line." Laser and Particle Beams 15, no. 2 (1997): 249–57. http://dx.doi.org/10.1017/s0263034600010570.

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A fast-charging, discharge-switch-free Blumlein pulse forming line has been developed for high-voltage pulsed power generation. In the BL, a saturable charging inductor (CI) of amorphous metallic core is utilized and, as a result, fast-charging (charging time ≈220 ns) is obtained with a reduced prepulse. In addition, by using CI as a step-up transformer, the impedance of the output pulse can be converted to 4Z, Z, Z/4. By using the BL with a Marx generator of 300 kV and 1.1 kJ, an output of —580 kV at 24 kA and a pulse length of 60 ns are obtained, with a current rise time of less than 16 ns.

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Chu, Xu, Jinliang Liu, Langning Wang, Tao Xun, Xinbing Cheng, and Hanwu Yang. "A new solid-state LC-Marx generator based on saturable pulse transformer." Review of Scientific Instruments 92, no. 5 (2021): 054712. http://dx.doi.org/10.1063/5.0039117.

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9

Liu, Yi, Siwei Liu, Yibo Han, Yafeng Ge, Qin Zhang, and Fuchang Lin. "Optimization Design of a Repetitive Nanosecond Pulse Generator Based on Saturable Pulse Transformer and Magnetic Switch." IEEE Transactions on Plasma Science 43, no. 9 (2015): 3277–85. http://dx.doi.org/10.1109/tps.2015.2459102.

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10

Geng, Jiu-yuan, Jian-hua Yang, Xin-bing Cheng, Rong Chen, and Ting Shu. "A compact, low jitter, high voltage trigger generator based on fractional-turn ratio saturable pulse transformer and its application." Review of Scientific Instruments 93, no. 8 (2022): 084709. http://dx.doi.org/10.1063/5.0090998.

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In this paper, an all-solid-state high voltage trigger generator is developed, which is aimed at triggering a several gigawatts three-electrode spark gap of an intense electron beam accelerator (IEBA). As one of the most important parts for triggering the IEBA precisely, it is developed based on a fractional-turn ratio saturable pulse transformer and a compact six-stage Marx generator. A pulse of rising time 141 ns and amplitude 79.6 kV is obtained on the 1000 Ω dummy load. The trigger is operated at pulsed repetition frequency over 10 Hz for testing its operational stability. The jitter count

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Dissertations / Theses on the topic "Saturable pulse transformer"

1

Degnon, Mawuena. "Étude des commutateurs semi-conducteurs à ouverture destinés à des applications de puissance pulsée avec des tensions de sortie allant jusqu'à 500 kV." Electronic Thesis or Diss., Pau, 2024. https://theses.hal.science/tel-04685830.

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Dans les systèmes de hautes puissances pulsées, le stockage inductif présente un avantage indéniable vis-à-vis du stockage capacitif du fait de sa plus forte densité d’énergie. L’exploitation de cet avantage nécessite toutefois l'utilisation d'un interrupteur à ouverture pour générer l'impulsion de tension. En outre, compte tenu de la demande croissante de générateurs impulsionnels fiables, en particulier pour les applications industrielles, il devient indispensable de recourir aux composants semi-conducteurs. La diode SOS (Semiconductor Opening Switch), développée dans les années 1990 à l'Ins

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Conference papers on the topic "Saturable pulse transformer"

1

Li, Y., L. Zhuang, T. Sugai, and W. Jiang. "Relation Between Output Rise Time and Efficiency of Pulsed Power Generation Circuit Using Saturable Pulsed Transformer." In 2024 IEEE International Conference on Plasma Science (ICOPS). IEEE, 2024. http://dx.doi.org/10.1109/icops58192.2024.10625898.

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2

Zhang, Dongdong, Ping Yan, Jue Wang, and Yuan Zhou. "Magnetic characteristics of saturable pulse transformer in magnetic pulse compression system." In 2009 IEEE Pulsed Power Conference (PPC). IEEE, 2009. http://dx.doi.org/10.1109/ppc.2009.5386352.

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3

Molva, E., Ph Thony, L. Fulbert, J. Marty, M. Rabarot, and B. Ferrand. "Microchip Lasers and Micro-Optics Technologies." In The European Conference on Lasers and Electro-Optics. Optica Publishing Group, 1996. http://dx.doi.org/10.1364/cleo_europe.1996.cfh7.

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Microchip lasers are the most compact (~1mm3) and the simplest diode pumped solid state lasers The mirrors of the optical cavity are directly deposited on the polished faces of a thin (-1mm) laser material. They are fabricated using collective fabrication processes allowing a low cost mass production. A microchip laser has a typical size of 1×1×0.5 mm3. It is very reliable and simple to use. The microchip laser is a kind of optical transformer which transforms a poor quality laser diode beam to a diffraction limited TEM00 and single frequency laser beam Moreover, by active or passive Q-switchi

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4

Yakymyshyn, Christopher P., and William T. Lotshaw. "Ultrashort pulse generation in lasers containing an antiresonant ring." In OSA Annual Meeting. Optica Publishing Group, 1990. http://dx.doi.org/10.1364/oam.1990.thy8.

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Mode locking with an antiresonant ring is a powerful technique for producing stable trains of ultrashort pulses. This structure1 was first applied to visible dye lasers by placing a saturable absorber within an antiresonant ring that forms the high-reflectivity end mirror of a linear laser cavity. Nearly transform-limited 65 fs pulses have been generated with enhanced pulse stability.2 By using the additive pulse mode-locking (APM) representation, we describe the antiresonant ring (ARR) as a pulse-shaping reflector, which returns a temporally narrowed pulse to the main laser cavity. When a non

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Khrushchev, I. Yu, E. M. Dianov, A. G. Deryagin, D. V. Kuksenkov, V. I. Kuchinskii, and E. L. Portnoi. "Soliton generation employing passively mode-locked laser diode and erbium-fiber amplifier." In The European Conference on Lasers and Electro-Optics. Optica Publishing Group, 1994. http://dx.doi.org/10.1364/cleo_europe.1994.ctue1.

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Recent progress in laser diodes with an ion-implanted fast saturable absorber resulted in generation of ultrashort optical pulses both in the gain-switching and in the passive mode-locking regimes.1-3 Normally, an implanted laser generates low intensity non-transform-limited pulses or pulse trains. Application of a fiber amplifier to increase the signal intensity and to improve the pulse quality is a promising way of obtaining soliton-like pulses.

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Fork, R. L., J. P. Gordon, and J. A. Valdmanis. "Laser Pulse Formation by Balanced Self Phase Modulation, Group Velocity Dispersion, Saturable Absorption, and Saturable Gain." In Instabilities and Dynamics of Lasers and Nonlinear Optical Systems. Optica Publishing Group, 1985. http://dx.doi.org/10.1364/idlnos.1985.fc2.

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We examine, experimentally and theoretically, the nonlinear dynamics of a laser which generates pulses as short as 27 fs directly from the laser (1), Fig. 1 . The laser shapes the intracavity pulses by a balanced combination of self phase modulation, group velocity dispersion, saturable absorption, and saturable gain which appears different from the shaping mechanisms in earlier lasers where the pulse shaping was due principally to saturable absorption and gain (2), or to soliton-like mechanisms in an optical fiber (3). The shaping which we discuss also offers advantages over prior modelocking

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Agheb, E., K. Niayesh, E. Hashemi, J. Jadidian, and A. A. Shayegani-Akmal. "Magnetic pulse compression in pulse transformers with segmented saturable magnetic cores." In 2008 IEEE 35th International Conference on Plasma Science (ICOPS). IEEE, 2008. http://dx.doi.org/10.1109/plasma.2008.4591193.

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8

Hopkins, J.-M., G. J. Valentine, W. Sibbett, et al. "Ultralow-noise Battery Operated Passively Modelocked Cr3+:LiSAF laser." In The European Conference on Lasers and Electro-Optics. Optica Publishing Group, 1998. http://dx.doi.org/10.1364/cleo_europe.1998.cwm2.

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The combination of a GaAs semiconductor saturable absorbing mirror (SESAM)1 and a low-threshold laser geometry2 has allowed the efficient production of stable low-noise femtosecond pulses. The highly asymmetric 4-mirror Cr3+LiSAF laser was pumped by 2 polarisation-combined narrow-stripe AlGaInP laser diodes each providing a maximum available power of 40mW incident on the crystal facet. The cw oscillation threshold of the laser was 16mW and the pulse repetition frequency was 153MHz. When output coupling through a high reflecting (HR) end mirror, the laser produced stable, sub 70 fs transform li

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9

Soccolich, C. E., M. N. Islam, and K. R. German. "Extended tuning range for a passively mode-locked NaCl color-center laser." In OSA Annual Meeting. Optica Publishing Group, 1990. http://dx.doi.org/10.1364/oam.1990.mb4.

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We have doubled the tuning range of a passively mode-locked NaCl color-center laser by introducing a low-loss intracavity frequency filter and properly preparing the NaCl gain crystal. By using a collection of bulk and multiple-quantum-well III–V saturable absorbers and II–VI quantum-well saturable absorbers, we obtained passive mode-locked operation over the wavelength range of 1.5–1.7 µm. To provide sufficient wavelength restriction without introducing excess bandwidth limiting or loss, we replaced the biréfringent plate of previous systems1 with a tunable frequency filter,2 formed by a pair

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10

Mecozzi, A., H. A. Haus, and Y. Lai. "Noise of mode-locked lasers." In OSA Annual Meeting. Optica Publishing Group, 1991. http://dx.doi.org/10.1364/oam.1991.ms5.

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In recent years, many solid-state lasers have been mode-locked successfully, using the additive pulse mode-locking (APM) principle. It has been shown that, under appropriate approximations, the theory of APM is congruent with that of saturable absorber mode-locking, supplemented by self-phase modulation and group velocity dispersion. When the shortest pulses are achieved, the pulses behave like transform-limited solitons, perturbed by the gain-bandwidth limiting and the APM action. In this limit, a perturbation theory is feasible that is closely related to that of soliton perturbation theory.

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