Add to ORKGA technique is described for non-destructive measurement and monitoring of the steering offset of the electron and positron beams at the interaction point of the SLC, based on using stripline beam-position monitors to measure the centroid of one beam as it is deflected by the opposing beam. This tech-nique is also expected to provide diagnostic information related to the spot rise of the micron-rise beams. 1
Collimators with adjustable jaws are used in the SLC linac, arcs, and ®nal focus to eliminate the ta...
With the switch to flat beam operation in the SLC during the 1993 run, it has become necessary to de...
The Stanford Linear Collider is a pulsed machine with a repetition rate of 120 Hz. By using fast dev...
As soon as two SLC beams make it to the intersection region, both transverse offsets, spot sizes and...
The Stanford Linear Collider requires special Beam Position Monitors near the Interaction Point (IP)...
In the SLC main linac a train of three bunches is accelerated. The leading positron bunch is followe...
The Next Linear Collider (NLC) is proposed to study e+ e- collisions in the TeV energy region. The s...
The requirements of RF acceleration in the SLC Linac to produce high energy beams are complicated by...
To achieve maximum luminosity at the SLC, both the electron and positron beams must reach their mini...
Bremsstrahlung gamma rays are emitted in a narrow forward cone while the electron and positron beams...
Beam size estimates made using beam-beam deflections are used for optimization of the Stanford Linea...
To achieve maximum integrated luminosity at the SLAC Linear Collider, a method of noninvasive beam t...
In the SLC linac, low emittance beams with typical transverse dimensions less than 0.2 mm must be ac...
Beam position monitors are an important diagnostics tool for particle accelerator operation and rela...
With the switch to flat beam operation in the SLC during the 1993 run [1], it has become necessary t...
Collimators with adjustable jaws are used in the SLC linac, arcs, and ®nal focus to eliminate the ta...
With the switch to flat beam operation in the SLC during the 1993 run, it has become necessary to de...
The Stanford Linear Collider is a pulsed machine with a repetition rate of 120 Hz. By using fast dev...
As soon as two SLC beams make it to the intersection region, both transverse offsets, spot sizes and...
The Stanford Linear Collider requires special Beam Position Monitors near the Interaction Point (IP)...
In the SLC main linac a train of three bunches is accelerated. The leading positron bunch is followe...
The Next Linear Collider (NLC) is proposed to study e+ e- collisions in the TeV energy region. The s...
The requirements of RF acceleration in the SLC Linac to produce high energy beams are complicated by...
To achieve maximum luminosity at the SLC, both the electron and positron beams must reach their mini...
Bremsstrahlung gamma rays are emitted in a narrow forward cone while the electron and positron beams...
Beam size estimates made using beam-beam deflections are used for optimization of the Stanford Linea...
To achieve maximum integrated luminosity at the SLAC Linear Collider, a method of noninvasive beam t...
In the SLC linac, low emittance beams with typical transverse dimensions less than 0.2 mm must be ac...
Beam position monitors are an important diagnostics tool for particle accelerator operation and rela...
With the switch to flat beam operation in the SLC during the 1993 run [1], it has become necessary t...
Collimators with adjustable jaws are used in the SLC linac, arcs, and ®nal focus to eliminate the ta...
With the switch to flat beam operation in the SLC during the 1993 run, it has become necessary to de...
The Stanford Linear Collider is a pulsed machine with a repetition rate of 120 Hz. By using fast dev...