In this report we study the effects of injection jitter on emittance growth, and hence on luminosity, in the improved linac with stronger focusing, and for the new bunch parameters. We consider both cases when Landau damping has been invoked, and when it has not been
Loss of Landau damping leading to a single bunch longitudinal instability has been observed in the L...
In the compact linear collider (CLIC) the tolerances on dynamic imperfections are tight in themain l...
At the SLC, a train consisting of one positron bunch followed by two electron bunches is accelerated...
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...
this paper, we present some of the jitter measurements and discuss the results of studies aimed at i...
The positron beam in the SLC injector linac is a high current (7*1010particles /bunch), large transv...
Transverse wakefield (or BNS’) damping has been successfully used in the linac of the Stanford Linea...
The transverse emittances in the SLAC Linear Collider can be severely diluted by collective wakefiel...
The requirements of RF acceleration in the SLC Linac to produce high energy beams are complicated by...
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 beam for FACET (Facility for Advanced aCcelerator Experimental Tests) at SLAC requires an energy...
Dynamic imperfections in future linear colliders can lead to a significant luminosity loss. We discu...
Emittance growth of accelerated beams in the 50 GeV linear accelerator of the Stanford Linear Collid...
Loss of Landau damping leading to a single bunch longitudinal instability has been observed in the L...
In the compact linear collider (CLIC) the tolerances on dynamic imperfections are tight in themain l...
At the SLC, a train consisting of one positron bunch followed by two electron bunches is accelerated...
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...
this paper, we present some of the jitter measurements and discuss the results of studies aimed at i...
The positron beam in the SLC injector linac is a high current (7*1010particles /bunch), large transv...
Transverse wakefield (or BNS’) damping has been successfully used in the linac of the Stanford Linea...
The transverse emittances in the SLAC Linear Collider can be severely diluted by collective wakefiel...
The requirements of RF acceleration in the SLC Linac to produce high energy beams are complicated by...
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 beam for FACET (Facility for Advanced aCcelerator Experimental Tests) at SLAC requires an energy...
Dynamic imperfections in future linear colliders can lead to a significant luminosity loss. We discu...
Emittance growth of accelerated beams in the 50 GeV linear accelerator of the Stanford Linear Collid...
Loss of Landau damping leading to a single bunch longitudinal instability has been observed in the L...
In the compact linear collider (CLIC) the tolerances on dynamic imperfections are tight in themain l...
At the SLC, a train consisting of one positron bunch followed by two electron bunches is accelerated...
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