The Novosibirsk free electron laser facility

Shevchenko, O.A.; Vinokurov, Nikolay; Arbuzov, V. S.; Chernov, K. N.; Deichuly, O. I.; Dementyev, E. N.; Dovzhenko, B. A.; Getmanov, Ya. V.; Gorbachev, Ya. I.; Knyazev, B. A.; Kondakov, A. A.; Козак, В. Р.; Kozyrev, E.V.; Krutikhin, S. A.; Kubarev, V. V.; Кулипанов, Г.Н.; Купер, Э. А.; Kuptsov, I. V.; Kurkin, G.Ya.; Medvedev, L. E.; Motygin, Sergey; Ovchar, V. K.; Osipov, V. N.; Petrov, V.M.; Pilan, A. M.; Popik, V. M.; Repkov, V. V.; Salikova, T. V.; Scheglov, M.A.; Sedlyarov, I. K.; Serednyakov, S. S.; Skrinsky, A.N.; Tararyshkin, S. V.; Tribendis, Alexey; Tcheskidov, V. G.; Volkov, Vladimir

doi:10.1063/5.0031513

Cited by 15 publications

(6 citation statements)

References 3 publications

Supporting

Mentioning

Contrasting

Unclassified

Order By: Relevance

“…Мы продемонстрируем также генерацию радиально и азимутально поляризованных вихревых пучков, а также приведем пример использования векторных вихревых пучков. Эксперименты выполнены с использованием мощного излучения Новосибирского лазера на свободных электронах (НЛСЭ) [14].…”

Section: электрическое поле идеального бесселева пучка описывается вы...unclassified

Terahertz Bessel and "perfect" vortex beams generated with a binary axicon and axicon with continuous relief

et al. 2022

View full text Add to dashboard Cite

Comparative studies of characteristics of Bessel and "perfect" vortex beams with a topological charge 9, created using a binary silicon axicon and a "holographic" diamond axicon with continu-ous profile at a wavelength of 141 μm, are carried out. Beams with linear and radial polarization are investigated. An example of the use of a perfect radially polarized beam for the excitation of vortex plasmon-polaritons on a cylindrical conductor is given.

show abstract

Section: электрическое поле идеального бесселева пучка описывается вы...unclassified

Terahertz Bessel and "perfect" vortex beams generated with a binary axicon and axicon with continuous relief

et al. 2022

View full text Add to dashboard Cite

show abstract

“…The generation of optical vortices in the terahertz (THz) range is not as well studied as it is in the visible range, where liquid crystal spatial light modulators are commonly used 6 . However, these modulators cannot be employed to form OAM beams when using high-power THz radiation from gyrotrons 7,8 or free electron lasers 9,10 . In such cases, diffractive optical elements (DOEs) are a suitable technique.…”

Section: Introductionmentioning

confidence: 99%

Combined high-power terahertz vortex Bessel beams: formation and identification

Osintseva,

Gerasimov,

Choporova

et al. 2023

Infrared, Millimeter-Wave, and Terahertz Technologies X

View full text Add to dashboard Cite

“…Finally, the average and peak power are, to a large extent, determined by the accelerator technology. Superconducting energy recovery linacs are the primary drivers for high average power FEL oscillators [64][65][66][67][68][69][70]; however, other types of FEL oscillators have used various techniques to increase the output pulse energy including, but not limited to, optical klystrons [34,36,48,57,58,60,63,[71][72][73][74][75][76], cavity dumping [77][78][79][80][81], pulse stacking in an external cavity [82][83][84], electron beam energy ramping [85,86] or dynamic cavity desynchronization [87][88][89][90][91][92]. Tapering of the undulator [93][94][95] has also been used to improve the peak power in the pulse [96][97][98][99][100], however, tapering of the undulator in FEL oscillators leads to complicated dynamics and a strong dependence on system parameters…”

Section: Introductionmentioning

confidence: 99%

Three-Dimensional, Time-Dependent Analysis of High- and Low-Q Free-Electron Laser Oscillators

Slot

Freund

2021

Applied Sciences

View full text Add to dashboard Cite

Free-electron lasers (FELs) have been designed to operate over virtually the entire electromagnetic spectrum, from microwaves through to X-rays, and in a variety of configurations, including amplifiers and oscillators. Oscillators can operate in both the low and high gain regime and are typically used to improve the spatial and temporal coherence of the light generated. We will discuss various FEL oscillators, ranging from systems with high-quality resonators combined with low-gain undulators, to systems with a low-quality resonator combined with a high-gain undulator line. The FEL gain code MINERVA and wavefront propagation code OPC are used to model the FEL interaction within the undulator and the propagation in the remainder of the oscillator, respectively. We will not only include experimental data for the various systems for comparison when available, but also present, for selected cases, how the two codes can be used to study the effect of mirror aberrations and thermal mirror deformation on FEL performance.

show abstract

The Novosibirsk free electron laser facility

Cited by 15 publications

References 3 publications

Terahertz Bessel and "perfect" vortex beams generated with a binary axicon and axicon with continuous relief

Terahertz Bessel and "perfect" vortex beams generated with a binary axicon and axicon with continuous relief

Combined high-power terahertz vortex Bessel beams: formation and identification

Three-Dimensional, Time-Dependent Analysis of High- and Low-Q Free-Electron Laser Oscillators

Contact Info

Product

Resources

About