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Related papers: The Free Electron Laser Klystron Amplifier Concept

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High-gain free-electron lasers (FELs) are becoming important light sources at short wavelengths such as the EUV and X-ray regimes. A particularly promising concept is the regenerative amplifier FEL (RAFEL), which can greatly increase the…

Accelerator Physics · Physics 2023-11-23 River R. Robles , Aliaksei Halavanau , Gabriel Marcus , Zhirong Huang

A Free Electron Laser (FEL) facility utilizing a recirculated Superconducting Radio Frequency (SRF) linear accelerator (linac) provides the opportunity to achieve about five times greater photon energy than an unrecirculated linac of…

Accelerator Physics · Physics 2015-06-17 R. C. York

We propose a new scheme for high gain harmonic generation free electron lasers (HGHG FELs), which is seeded by a pair of intersecting laser beams to interact with an electron beam in a modulator undulator located in a dispersive section.…

Accelerator Physics · Physics 2017-03-17 Takashi Tanaka , Ryota Kinjo

In the framework of the Compact Light XLS project, a short ultra-high gradient linearizer working on the third harmonic of the main LINAC frequency is requested. Increasing gradients and reducing dimensions are requirements for XLS and all…

Accelerator Physics · Physics 2021-04-27 Mostafa Behtouei , Bruno Spataro , Franco Di Paolo , Alberto Leggieri

Advanced technical solution for the design of a low perveance electron gun with a high quality beam dedicated to high power Ka-band klystrons is presented in this paper. The proposed electron gun can be used to feed linear accelerating…

Accelerator Physics · Physics 2021-09-09 M. Behtouei , B. Spataro , L. Faillace , M. Carillo , A. Leggieri , L. Palumbo , M. Migliorati

CLIC is a linear $e^+e^-$ ($\gamma\gamma$) collider project which uses a drive beam to accelerate the main beam. The drive beam provides RF power for each corresponding unit of the main linac through energy extracting RF structures. CLIC…

Accelerator Physics · Physics 2007-05-23 Husnu Aksakal

It is reported that [Z. Huang et al., Phys. Rev. Lett. 109, 204801 (2012)], high-gain free-electron laser (FEL) can be generated by transverse-dispersed electron beams from laser-plasma accelerators (LPAs) using transverse-gradient…

Accelerator Physics · Physics 2016-08-11 G. Zhou , Y. Jiao , J. Wu , T. Zhang

Various scientific and industrial researches such as spectroscopy and advanced nano-technologies have been demanding high flux and fully coherent EUV and X-ray radiation. These demands can be commendably satisfied with a MHz-level…

Accelerator Physics · Physics 2024-04-29 Xiaofan Wang , Chao Feng , Bart Faatz , Weiqing Zhang , Zhentang Zhao

Beam premodulation on free electron laser (FEL) offers considerable enhancement in gain and efficiency when the phase of the premodulated beam is -pi/2 and the beam is highly modulated implying the maximum beam oscillatory velocity due to…

Plasma Physics · Physics 2007-05-23 Vivek Beniwal , Suresh C. Sharma , Satoshi Hamaguchi

Free-electron lasers (FELs) have been built ranging in wavelength from long-wavelength oscillators using partial wave guiding through ultraviolet through hard x-ray FELs that are either seeded or start from noise (SASE). Operation in the…

Accelerator Physics · Physics 2021-05-18 Henry P. Freund , Peter van der Slot , Yuri Shvyd'ko

This report is a primer introduction on the sources of coherent syncrotron radiation from FELs compared to conventional lasers. Even though the underlying mechanisms are different, FELs can be considered a laser source to all effects. In…

Accelerator Physics · Physics 2010-10-27 G. Dattoli , M. Del Franco , M. Labat , P. L. Ottaviani , S. Pagnutti

It is shown via theory and simulation that the resonant frequency of a Free Electron Laser may be modulated to obtain an FEL interaction with a frequency bandwidth which is at least an order of magnitude greater than normal FEL operation.…

Accelerator Physics · Physics 2017-06-07 L. T. Campbell , B. W. J. McNeil

The successful operation of the hard x-ray self-seeding experiment at the LCLS opens the era of fully coherent hard x-ray free electron lasers (FELs). However, the shot-to-shot radiation fluctuation is still a serious issue. In this paper,…

Accelerator Physics · Physics 2013-05-07 Haixiao Deng , Chao Feng

Phonon lasers, as their photon counterparts, rely on the physics of stimulated emission. Arguably, because light does not require a material substrate to propagate, while sound does, the impact of the two technologies has however been…

Externally seeded free-electron lasers (FELs) are promising approaches for generating fully coherent soft-X-ray radiation. Their extension to shorter wavelengths and MHz-level repetition rates is, however, constrained by the limited…

Accelerator Physics · Physics 2026-05-29 Hanxiang Yang , Nanshun Huang , Zheng Qi , Tao Liu , Haixiao Deng , Bo Liu

X-ray free-electron laser (XFEL) facilities require progressive compression of electron bunches as they are accelerated from an injector to the undulators. This is necessary to achieve the peak currents required for efficient lasing,…

Accelerator Physics · Physics 2026-03-10 Adam Dixon , Peter Williams , Sara Thorin , Andrzej Wolski , Alexander Brynes , Tessa Charles , Ian Bailey

The motion and photon emission of electrons in a superlattice may be described as in an undulator. Therefore, there is a close analogy between ballistic electrons in a superlattice and electrons in a free electron laser (FEL). Touching upon…

Accelerator Physics · Physics 2017-05-23 I. V. Dovgan

Fine time-resolved analysis of matter - i.e. spectroscopy and photon scattering - in the linear response regime requires a fs-scale pulsed, high repetition rate, fully coherent X-ray source. A seeded Free-Electron Laser (FEL) driven by a…

Accelerator Physics · Physics 2021-06-09 N. S. Mirian , M. Opromolla , G. Rossi , L. Serafini , V. Petrillo

The collective and single-electron amplification regimes of a non-collinear free electron laser are analyzed within the framework of dispersion equations. The small-signal gain and the conditions for self-amplified excitations are found.…