If the laser pulse driving photoinjectors could be arbitrarily shaped, the emittance growth induced by space charge effects could be totally compensated for. In particular, for RF guns the photo-electron distribution leaving the cathode should have a 3D-ellipsoidal shape. The emittance at the end of the injector could be as small as the cathode emittance. We explore how the emittance and the brightness can be optimized for photoinjector based on RF gun depending on the peak current requirements. Techniques available to produce those ideal laser pulse shapes are also discussed
The optimum design of an emittance compensated rf photoinjector is very complicated and time‐consumi...
High brightness photoinjectors operating in continuous wave (CW) mode are enabling many advanc...
To make full use of the photocathode material and improve its quantum efficiency lifetime, it can be...
If the laser pulse driving photoinjectors could be arbitrarily shaped, the emittance growth induced ...
The optimum photo-electron distribution from the cathode of an RF photoinjector producing a space ch...
Photo Injector Test Facility at DESY Zeuthen (PITZ) is a major challenge in optimizing a high bright...
Laser pulse length and laser shape should be optimized to minimize the beam emittance of photo-catho...
We report on the design of the RF photoinjector of the Linac Coherent Light Source. The RF photoinje...
In the last decades, photoinjector brightness has improved significantly, driven by the needs of fre...
In the last decades, photoinjector brightness has improved significantly, driven by the needs of fre...
The optimum design of an emittance compensated rf photoinjector is very complicated and time-consumi...
The use of high brightness electron beams in Free Electron Laser (FEL) applications is of increasing...
High brightness photoinjectors operating in continuous wave (CW) mode are enabling many advanc...
The optimum design of an emittance compensated rf photoinjector is very complicated and time‐consumi...
The use of high brightness electron beams in Free Electron Laser (FEL) applications is of increasing...
The optimum design of an emittance compensated rf photoinjector is very complicated and time‐consumi...
High brightness photoinjectors operating in continuous wave (CW) mode are enabling many advanc...
To make full use of the photocathode material and improve its quantum efficiency lifetime, it can be...
If the laser pulse driving photoinjectors could be arbitrarily shaped, the emittance growth induced ...
The optimum photo-electron distribution from the cathode of an RF photoinjector producing a space ch...
Photo Injector Test Facility at DESY Zeuthen (PITZ) is a major challenge in optimizing a high bright...
Laser pulse length and laser shape should be optimized to minimize the beam emittance of photo-catho...
We report on the design of the RF photoinjector of the Linac Coherent Light Source. The RF photoinje...
In the last decades, photoinjector brightness has improved significantly, driven by the needs of fre...
In the last decades, photoinjector brightness has improved significantly, driven by the needs of fre...
The optimum design of an emittance compensated rf photoinjector is very complicated and time-consumi...
The use of high brightness electron beams in Free Electron Laser (FEL) applications is of increasing...
High brightness photoinjectors operating in continuous wave (CW) mode are enabling many advanc...
The optimum design of an emittance compensated rf photoinjector is very complicated and time‐consumi...
The use of high brightness electron beams in Free Electron Laser (FEL) applications is of increasing...
The optimum design of an emittance compensated rf photoinjector is very complicated and time‐consumi...
High brightness photoinjectors operating in continuous wave (CW) mode are enabling many advanc...
To make full use of the photocathode material and improve its quantum efficiency lifetime, it can be...