The authors report on measurements of the bunch energy spectrum at the end of the SLAC linac. Using the spectra obtained for two different linac rf phases they obtain both the bunch induced voltage and the longitudinal distribution of the bunch. The measurement results are compared with theoretical predictions. In particular, the induced voltage is in good agreement with that obtained using the calculated wake function for the SLAC linac. This measurement technique may be useful for monitoring changes of the linac bunch shape in the SLC
We report the first studies of bunch length in collision in an operating linear collider, making use...
When a beam travels near collimator jaws, it gets an energy loss and a transverse kick due to the ba...
The linac at the Stanford Linear Accelerator (SLAC) runs routinely with a beam loading of around 12%...
In the E164 Experiment at the Stanford Linear Acceler-ator Center (SLAC), we drive plasma wakes for ...
In the E164 Experiment at that Stanford Linear Accel-erator Center (SLAC), we drive plasma wakes for...
In the E164 Experiment at that Stanford Linear Accelerator Center (SLAC), we drive plasma wakes for ...
We report measurements of the profile of the wakefield-induced energy loss of the beam along the 1.2...
In the SLC main linac a train of three bunches is accelerated. The leading positron bunch is followe...
The Gun Test Facility (GTF) was built to test high-brightness sources for the proposed Linac Coheren...
Beam emittance dilution by self induced transverse fields (wakefields) in accelerating structures is...
Coherent Smith-Purcell radiation has been demonstrated as a technique for measuring the longitudinal...
The linac at the Stanford Linear Accelerator Center (SLAC) can provide beams to different experiment...
The development of future free electron lasers (FEL) and linear colliders requires high brightness e...
Beam emittance dilution caused by wakefield effects is one of the important issues in the SLC linac....
The Linac Coherent Light Source (LCLS) [1] is an x-ray FEL project with a 1-nC electron bunch compre...
We report the first studies of bunch length in collision in an operating linear collider, making use...
When a beam travels near collimator jaws, it gets an energy loss and a transverse kick due to the ba...
The linac at the Stanford Linear Accelerator (SLAC) runs routinely with a beam loading of around 12%...
In the E164 Experiment at the Stanford Linear Acceler-ator Center (SLAC), we drive plasma wakes for ...
In the E164 Experiment at that Stanford Linear Accel-erator Center (SLAC), we drive plasma wakes for...
In the E164 Experiment at that Stanford Linear Accelerator Center (SLAC), we drive plasma wakes for ...
We report measurements of the profile of the wakefield-induced energy loss of the beam along the 1.2...
In the SLC main linac a train of three bunches is accelerated. The leading positron bunch is followe...
The Gun Test Facility (GTF) was built to test high-brightness sources for the proposed Linac Coheren...
Beam emittance dilution by self induced transverse fields (wakefields) in accelerating structures is...
Coherent Smith-Purcell radiation has been demonstrated as a technique for measuring the longitudinal...
The linac at the Stanford Linear Accelerator Center (SLAC) can provide beams to different experiment...
The development of future free electron lasers (FEL) and linear colliders requires high brightness e...
Beam emittance dilution caused by wakefield effects is one of the important issues in the SLC linac....
The Linac Coherent Light Source (LCLS) [1] is an x-ray FEL project with a 1-nC electron bunch compre...
We report the first studies of bunch length in collision in an operating linear collider, making use...
When a beam travels near collimator jaws, it gets an energy loss and a transverse kick due to the ba...
The linac at the Stanford Linear Accelerator (SLAC) runs routinely with a beam loading of around 12%...
Add to ORKG