Add to ORKGWe report the first studies of bunch length in collision in an operating linear collider, making use of a new rf bunch length monitor installed in the South Final Focus of the Stanford Linear Collider (SLC) prior to the 1997/98 lu-minosity run. The theoretical and measured monitor re-sponses to linac injection phase and bunch compressor voltage are described. Correlations with beamstrahlung and luminosity are discussed.
The measurement of electron bunch-length with sub-ps time resolution is mandatory for future X-ray f...
The Stanford Linear Collider is a pulsed machine with a repetition rate of 120 Hz. By using fast dev...
The SLAC Linac can deliver to End Station A (ESA) a high-energy test beam with similar beam paramete...
The production and measurement of short electron and positron bunches in the Stanford Linear Collide...
Amajor upgrade to the SLC final focus was installed in 1994 to eliminate the dominant third-order ab...
The development of future free electron lasers (FEL) and linear colliders requires high brightness e...
The Saskatchewan Accelerator Laboratory is a 300 MeV electron accelerator (Linac) and storage ring. ...
The Stanford Linear Collider requires special Beam Position Monitors near the Interaction Point (IP)...
The Stanford Linear Collider (SLC) was recently converted to flat beam operation (ye = = 10 my), pr...
The linac at the Stanford Linear Accelerator Center (SLAC) can provide beams to different experiment...
We report various accelerator physics studies and improvements from the 1997/98 run at the Stanford ...
The construction project for the SLAC Linear Collider (SLC) was officially completed in April 1987, ...
The authors report on measurements of the bunch energy spectrum at the end of the SLAC linac. Using ...
The Stanford Linear Collider (SLC) has been in operation for several years with the initial and acce...
The linac of the SLAC Linear Collider (SLC) is required to accelerate several intense electron and p...
The measurement of electron bunch-length with sub-ps time resolution is mandatory for future X-ray f...
The Stanford Linear Collider is a pulsed machine with a repetition rate of 120 Hz. By using fast dev...
The SLAC Linac can deliver to End Station A (ESA) a high-energy test beam with similar beam paramete...
The production and measurement of short electron and positron bunches in the Stanford Linear Collide...
Amajor upgrade to the SLC final focus was installed in 1994 to eliminate the dominant third-order ab...
The development of future free electron lasers (FEL) and linear colliders requires high brightness e...
The Saskatchewan Accelerator Laboratory is a 300 MeV electron accelerator (Linac) and storage ring. ...
The Stanford Linear Collider requires special Beam Position Monitors near the Interaction Point (IP)...
The Stanford Linear Collider (SLC) was recently converted to flat beam operation (ye = = 10 my), pr...
The linac at the Stanford Linear Accelerator Center (SLAC) can provide beams to different experiment...
We report various accelerator physics studies and improvements from the 1997/98 run at the Stanford ...
The construction project for the SLAC Linear Collider (SLC) was officially completed in April 1987, ...
The authors report on measurements of the bunch energy spectrum at the end of the SLAC linac. Using ...
The Stanford Linear Collider (SLC) has been in operation for several years with the initial and acce...
The linac of the SLAC Linear Collider (SLC) is required to accelerate several intense electron and p...
The measurement of electron bunch-length with sub-ps time resolution is mandatory for future X-ray f...
The Stanford Linear Collider is a pulsed machine with a repetition rate of 120 Hz. By using fast dev...
The SLAC Linac can deliver to End Station A (ESA) a high-energy test beam with similar beam paramete...