We present experimental studies of the gain length and saturation power level from 1.5 nm to 1.5 {angstrom} at the Linac Coherent Light Source (LCLS). By disrupting the FEL process with an orbit kick, we are able to measure the X-ray intensity as a function of undulator length. This kick method is cross-checked with the method of removing undulator sections. We also study the FEL-induced electron energy loss after saturation to determine the optimal taper of the undulator K values. The experimental results are compared to theory and simulations
The free electron laser (FEL) amplifier is implemented in x-ray FEL facilities to generate short wav...
The free electron laser (FEL) amplifier is implemented in x-ray FEL facilities to generate short wav...
The free electron laser (FEL) amplifier is implemented in x-ray FEL facilities to generate short wav...
We present experimental studies of the gain length and saturation power level from 1.5 nm to 1.5 Ang...
We present experimental studies of the gain length and saturation power level from 1.5 nm to 1.5 Ang...
We present experimental studies of the gain length and saturation power level from 1.5 nm to 1.5 A ̊...
For X-ray Free-Electron Lasers such as LCLS and TESLA FEL, a change in the electron energy while amp...
The Linac Coherent Light Source (LCLS) is an X-ray free-electron laser (FEL) project based on the SL...
The Linac Coherent Light Source (LCLS) Free-Electron Laser will operate in the wavelength range of 1...
ABSTRACT The Linac Coherent Light Source (LCLS) as the world's first hard x-ray free electron l...
The Linac Coherent Light Source (LCLS) is an x-ray Free-electron Laser (FEL) being commissioned at S...
The very bright electron beam required for an x-ray free-electron laser (FEL), such as the Linac Coh...
In the present work the influence of tapering with respect of the FEL efficiency has been systematic...
Technique of undulator tapering in the post-saturation regime is used at the existing X-ray FELs for...
Technique of undulator tapering in the post-saturation regime is used at the existing X-ray FELs for...
The free electron laser (FEL) amplifier is implemented in x-ray FEL facilities to generate short wav...
The free electron laser (FEL) amplifier is implemented in x-ray FEL facilities to generate short wav...
The free electron laser (FEL) amplifier is implemented in x-ray FEL facilities to generate short wav...
We present experimental studies of the gain length and saturation power level from 1.5 nm to 1.5 Ang...
We present experimental studies of the gain length and saturation power level from 1.5 nm to 1.5 Ang...
We present experimental studies of the gain length and saturation power level from 1.5 nm to 1.5 A ̊...
For X-ray Free-Electron Lasers such as LCLS and TESLA FEL, a change in the electron energy while amp...
The Linac Coherent Light Source (LCLS) is an X-ray free-electron laser (FEL) project based on the SL...
The Linac Coherent Light Source (LCLS) Free-Electron Laser will operate in the wavelength range of 1...
ABSTRACT The Linac Coherent Light Source (LCLS) as the world's first hard x-ray free electron l...
The Linac Coherent Light Source (LCLS) is an x-ray Free-electron Laser (FEL) being commissioned at S...
The very bright electron beam required for an x-ray free-electron laser (FEL), such as the Linac Coh...
In the present work the influence of tapering with respect of the FEL efficiency has been systematic...
Technique of undulator tapering in the post-saturation regime is used at the existing X-ray FELs for...
Technique of undulator tapering in the post-saturation regime is used at the existing X-ray FELs for...
The free electron laser (FEL) amplifier is implemented in x-ray FEL facilities to generate short wav...
The free electron laser (FEL) amplifier is implemented in x-ray FEL facilities to generate short wav...
The free electron laser (FEL) amplifier is implemented in x-ray FEL facilities to generate short wav...