this paper, we present some of the jitter measurements and discuss the results of studies aimed at isolating its source. In particular, we examine the positron jitter since the analysis of the electron jitter is complicated by its dependence on the positron motion via long-range wakefields. However, the electron results do not differ greatly
In this report we study the effects of injection jitter on emittance growth, and hence on luminosity...
The Stanford Linear Collider is a pulsed machine with a repetition rate of 120 Hz. By using fast dev...
Electron beam quality is an important factor in the performance of a free electron laser (FEL). Para...
We present model-independent measurements of the vertical trajectory jitter of the positron beam in ...
The pulse-to-pulse behavior of the beams in the SLC linac is dominated by wakefields which can ampli...
The positron beam in the SLC injector linac is a high current (7*1010particles /bunch), large transv...
The pulse-to-pulse behavior of the beams in the SLC linac is dominated by wakefields which can ampli...
In the SLC main linac a train of three bunches is accelerated. The leading positron bunch is followe...
At the SLC, a train consisting of one positron bunch followed by two electron bunches is accelerated...
At the SLC, a train consisting of one positron bunch followed by two electron bunches is accelerated...
Transverse pulse-to-pulse trajectory instability, ‘jitter’, in the linac of the SLAC Linear Collider...
Pulse-to-pulse variation of the transverse beam orbit, frequently referred to as jitter, has long be...
The Linac Coherent Light Source (LCLS) at SLAC is an x-ray Free Electron Laser (FEL) with wavelength...
The Linac Coherent Light Source (LCLS) at SLAC is an x-ray Free Electron Laser (FEL) with wavelength...
The requirements of RF acceleration in the SLC Linac to produce high energy beams are complicated by...
In this report we study the effects of injection jitter on emittance growth, and hence on luminosity...
The Stanford Linear Collider is a pulsed machine with a repetition rate of 120 Hz. By using fast dev...
Electron beam quality is an important factor in the performance of a free electron laser (FEL). Para...
We present model-independent measurements of the vertical trajectory jitter of the positron beam in ...
The pulse-to-pulse behavior of the beams in the SLC linac is dominated by wakefields which can ampli...
The positron beam in the SLC injector linac is a high current (7*1010particles /bunch), large transv...
The pulse-to-pulse behavior of the beams in the SLC linac is dominated by wakefields which can ampli...
In the SLC main linac a train of three bunches is accelerated. The leading positron bunch is followe...
At the SLC, a train consisting of one positron bunch followed by two electron bunches is accelerated...
At the SLC, a train consisting of one positron bunch followed by two electron bunches is accelerated...
Transverse pulse-to-pulse trajectory instability, ‘jitter’, in the linac of the SLAC Linear Collider...
Pulse-to-pulse variation of the transverse beam orbit, frequently referred to as jitter, has long be...
The Linac Coherent Light Source (LCLS) at SLAC is an x-ray Free Electron Laser (FEL) with wavelength...
The Linac Coherent Light Source (LCLS) at SLAC is an x-ray Free Electron Laser (FEL) with wavelength...
The requirements of RF acceleration in the SLC Linac to produce high energy beams are complicated by...
In this report we study the effects of injection jitter on emittance growth, and hence on luminosity...
The Stanford Linear Collider is a pulsed machine with a repetition rate of 120 Hz. By using fast dev...
Electron beam quality is an important factor in the performance of a free electron laser (FEL). Para...