We describe the bunch compression scheme for the TESLA Test Facility Free Electron Laser upgrade (TTF-2). The required peak current is 2.5 kA for operating the SASE-FEL within the saturation regime at a wavelength of 6 nm and with an electron beam energy of ∼1 GeV. The beam transverse slice emittance and the final energy spread should be held within the limit of 2.0 mm-mrad and ∼1 MeV respectively. We present a start-to-end simulation of the beam dynamics from the rf-gun up to the undulator entrance
This paper describes an effective frequency doubler scheme for SASE free electron lasers. It consist...
This paper describes an effective frequency doubler scheme for SASE free electron lasers. It consist...
Currently, a SASE-FEL in the VUV, driven by the TESLA test facility accelerator, is under constructi...
Phase 1 of the vacuum ultra-violet (VUV) free-electron laser (FEL) at the TESLA Test Facility (TTF) ...
Phase 1 of the vacuum ultra-violet (VUV) free-electron laser (FEL) at the TESLA test facility (TTF) ...
The free-electron laser (FEL) at the TESLA test facility (TTF2) produces laser-like radiation in the...
The TESLA Test Facility linac has been operated in the first half of 2002 with two bunch compressors...
For single-pass free-electron lasers (FEL), such as amplifiers and SASE devices, saturation of the r...
radiation. The design energy of the electron beam is 1 GeV, corresponding to a radiation wavelength ...
To perform a proof of principle experiment of a SASE based Free Electron Laser operating at waveleng...
The TTF Free Electron Laser requires high current electron bunches with small emittances. The beam i...
The TESLA Free Electron Laser (FEL) makes use of the high electron beam quality that can be provided...
We report the start-to-end modeling of our accelerator lattice design employing a laser-assisted bun...
High peak current (~40 A) electron beams with the macro-pulse duration of 2-5 μs are required for th...
An electron beam with a small energy spread (0.1%) and a small normalized emittance (2...
This paper describes an effective frequency doubler scheme for SASE free electron lasers. It consist...
This paper describes an effective frequency doubler scheme for SASE free electron lasers. It consist...
Currently, a SASE-FEL in the VUV, driven by the TESLA test facility accelerator, is under constructi...
Phase 1 of the vacuum ultra-violet (VUV) free-electron laser (FEL) at the TESLA Test Facility (TTF) ...
Phase 1 of the vacuum ultra-violet (VUV) free-electron laser (FEL) at the TESLA test facility (TTF) ...
The free-electron laser (FEL) at the TESLA test facility (TTF2) produces laser-like radiation in the...
The TESLA Test Facility linac has been operated in the first half of 2002 with two bunch compressors...
For single-pass free-electron lasers (FEL), such as amplifiers and SASE devices, saturation of the r...
radiation. The design energy of the electron beam is 1 GeV, corresponding to a radiation wavelength ...
To perform a proof of principle experiment of a SASE based Free Electron Laser operating at waveleng...
The TTF Free Electron Laser requires high current electron bunches with small emittances. The beam i...
The TESLA Free Electron Laser (FEL) makes use of the high electron beam quality that can be provided...
We report the start-to-end modeling of our accelerator lattice design employing a laser-assisted bun...
High peak current (~40 A) electron beams with the macro-pulse duration of 2-5 μs are required for th...
An electron beam with a small energy spread (0.1%) and a small normalized emittance (2...
This paper describes an effective frequency doubler scheme for SASE free electron lasers. It consist...
This paper describes an effective frequency doubler scheme for SASE free electron lasers. It consist...
Currently, a SASE-FEL in the VUV, driven by the TESLA test facility accelerator, is under constructi...