Pulse-to-pulse variation of the transverse beam orbit, frequently referred to as jitter, has long been a major problem in SLC operation. It impairs the SLC luminosity both by reducing the average beam overlap at the IP and by hampering precision tuning of the final focus. The origin of the fast orbit variation is not fully understood. Measurements during the 1994/95 SLC run showed that it is random from pulse to pulse, increases strongly with current and grows steadily along the SLAC linac, with a typical final rms amplitude of about half the beam size. In this paper, they investigate possible sources of the vertical orbit jitter
In this report we study the effects of injection jitter on emittance growth, and hence on luminosity...
The positron beam in the SLC injector linac is a high current (7*1010particles /bunch), large transv...
The beam for FACET (Facility for Advanced aCcelerator Experimental Tests) at SLAC requires an energy...
Transverse pulse-to-pulse trajectory instability, ‘jitter’, in the linac of the SLAC Linear Collider...
The pulse-to-pulse behavior of the beams in the SLC linac is dominated by wakefields which can ampli...
The pulse-to-pulse behavior of the beams in the SLC linac is dominated by wakefields which can ampli...
The Linac Coherent Light Source (LCLS) at SLAC is an x-ray Free Electron Laser (FEL) with wavelength...
We present model-independent measurements of the vertical trajectory jitter of the positron beam in ...
The Linac Coherent Light Source (LCLS) at SLAC is an x-ray Free Electron Laser (FEL) with wavelength...
this paper, we present some of the jitter measurements and discuss the results of studies aimed at i...
For future linear colliders the precise control and mitigation of pulse-to-pulse orbit jitter will b...
The Stanford Linear Collider is a pulsed machine with a repetition rate of 120 Hz. By using fast dev...
Pulse-to-pulse orbit jitter, if not controlled, can drastically degrade the luminosity in future lin...
Pulse-to-pulse orbit jitter, if not controlled, can drastically degrade the luminosity in future lin...
The beta function around an accelerator determines the shape and size of the beam. The LHC has demon...
In this report we study the effects of injection jitter on emittance growth, and hence on luminosity...
The positron beam in the SLC injector linac is a high current (7*1010particles /bunch), large transv...
The beam for FACET (Facility for Advanced aCcelerator Experimental Tests) at SLAC requires an energy...
Transverse pulse-to-pulse trajectory instability, ‘jitter’, in the linac of the SLAC Linear Collider...
The pulse-to-pulse behavior of the beams in the SLC linac is dominated by wakefields which can ampli...
The pulse-to-pulse behavior of the beams in the SLC linac is dominated by wakefields which can ampli...
The Linac Coherent Light Source (LCLS) at SLAC is an x-ray Free Electron Laser (FEL) with wavelength...
We present model-independent measurements of the vertical trajectory jitter of the positron beam in ...
The Linac Coherent Light Source (LCLS) at SLAC is an x-ray Free Electron Laser (FEL) with wavelength...
this paper, we present some of the jitter measurements and discuss the results of studies aimed at i...
For future linear colliders the precise control and mitigation of pulse-to-pulse orbit jitter will b...
The Stanford Linear Collider is a pulsed machine with a repetition rate of 120 Hz. By using fast dev...
Pulse-to-pulse orbit jitter, if not controlled, can drastically degrade the luminosity in future lin...
Pulse-to-pulse orbit jitter, if not controlled, can drastically degrade the luminosity in future lin...
The beta function around an accelerator determines the shape and size of the beam. The LHC has demon...
In this report we study the effects of injection jitter on emittance growth, and hence on luminosity...
The positron beam in the SLC injector linac is a high current (7*1010particles /bunch), large transv...
The beam for FACET (Facility for Advanced aCcelerator Experimental Tests) at SLAC requires an energy...