While the long-pulse, coasting beam model is often used in analysis and simulation of self-amplified spontaneous emission (SASE) free-electron lasers (FELs), many current SASE demonstration experiments employ relatively short electron bunches whose pulse length is on the order of the radiation slippage length. In particular, the low-energy undulator test line (LEUTL) FEL at the Advanced Photon Source has recently lased and nominally saturated in both visible and near-ultraviolet wavelength regions with a sub-ps pulse length that is somewhat shorter than the total slippage length in the 22-m undulator system. In this paper we explore several characteristics of the short pulse regime for SASE FELs with the multidimensional, time-dependent sim...
Optical lasers cannot produce x-rays of photons and high-gain free-electron lasers (FELs) are being ...
An RF linear accelerator can produce ultra-short electron pulses on the order of a picosecond. In a...
The Darmstadt IR FEL is designed to generate wavelengths between 3 and 10 mm and driven by the super...
Free-electron lasers (FELs) operate at wavelengths from millimeter waves through hard x-rays. At x-r...
This work studies the production and measurement of longitudinally coherent, ultrashort pulses of li...
Self-amplified spontaneous emission (SASE) free-electron lasers (FELs) deliver ultrashort pulses wit...
This paper investigates various properties of the "microspikes" associated with self-ampli...
Free-electron lasers (FELs) are among the world's most intense artificial artificial sources of cohe...
This paper investigates various properties of the ``microspikes`` associated with self-amplified spo...
Influence of a linear energy chirp in the electron beam on a self-amplified spontaneous emission (SA...
We discuss the use of tapered undulators to enhance the performance of free-electron lasers (FELs) b...
A self-consistent theory of a free electron laser (FEL) with slowly varying beam and undulator param...
High-gain Free-Electron Lasers (FEL) constitute a powerful source of intense, short radiation pulses...
Ultrashort electron bunches from laser-driven plasma accelerators hold promise as drivers for short-...
AbstractA method to achieve High-Brightness Self-Amplified Spontaneous Emission (HB-SASE) in the Fre...
Optical lasers cannot produce x-rays of photons and high-gain free-electron lasers (FELs) are being ...
An RF linear accelerator can produce ultra-short electron pulses on the order of a picosecond. In a...
The Darmstadt IR FEL is designed to generate wavelengths between 3 and 10 mm and driven by the super...
Free-electron lasers (FELs) operate at wavelengths from millimeter waves through hard x-rays. At x-r...
This work studies the production and measurement of longitudinally coherent, ultrashort pulses of li...
Self-amplified spontaneous emission (SASE) free-electron lasers (FELs) deliver ultrashort pulses wit...
This paper investigates various properties of the "microspikes" associated with self-ampli...
Free-electron lasers (FELs) are among the world's most intense artificial artificial sources of cohe...
This paper investigates various properties of the ``microspikes`` associated with self-amplified spo...
Influence of a linear energy chirp in the electron beam on a self-amplified spontaneous emission (SA...
We discuss the use of tapered undulators to enhance the performance of free-electron lasers (FELs) b...
A self-consistent theory of a free electron laser (FEL) with slowly varying beam and undulator param...
High-gain Free-Electron Lasers (FEL) constitute a powerful source of intense, short radiation pulses...
Ultrashort electron bunches from laser-driven plasma accelerators hold promise as drivers for short-...
AbstractA method to achieve High-Brightness Self-Amplified Spontaneous Emission (HB-SASE) in the Fre...
Optical lasers cannot produce x-rays of photons and high-gain free-electron lasers (FELs) are being ...
An RF linear accelerator can produce ultra-short electron pulses on the order of a picosecond. In a...
The Darmstadt IR FEL is designed to generate wavelengths between 3 and 10 mm and driven by the super...