To detect individual bunch phase oscillations a standard toroidal intensity monitor with about 30 MHz bandwidth is used. The bunch selection is done with track & hold devices. At DESY III the revolution frequency changes by a factor of 3 due to the momentum change. To manage t,his variation, the beam signals are converted up to a fixed intermediate frequency of 60 MHz. Crystal filters for noise suppression are used to optimize resolution for longitudinal dipole oscillations. Quadrature detectors in conjunction with low pass filtering deliver analog phase signals from each of t,he 11 bunches.
A direct way of obtaining intra bunch charge distribu-tions is to measure the amplitude roll off as ...
The maximum beam particle intensity and minimum emittance that can be injected, accelerated and stor...
This paper is intended to present the newly implemented wideband (100MHz) bunch oscillation measurem...
A system for bunch-by-bunch detection of transverse proton and antiproton coherent oscillations in t...
A system for bunch-by-bunch detection of transverse proton and antiproton coherent oscillations in t...
Turn-by-turn and bunch-by-bunch diagnostic systems were set up to support various studies. The beam ...
A system was developed for bunch-by-bunch detection of transverse proton and antiproton coherent osc...
The main purpose of the CTF3 preliminary phase is to demonstrate the bunch frequency multiplication....
Measurement of time of arrival of a particle bunch is a fundamental beam diagnostic. The PEP-II/ALS/...
An electronic system is presented which detects synchrotron oscillations of individual bunches with ...
A system for bunch-by-bunch detection of transverse proton and antiproton coherent oscillations in t...
The LHC and SPS transverse dampers use beam position electronics with I,Q detection at 400 MHz and 2...
We discuss the circuit design of a digital multiradian phase detector that measures the phase differ...
A method for computing transverse multibunch growth rates and frequency shifts in rings, which has b...
At the Cornell Electron/Positron Storage Ring, a fast luminosity monitor has been implemented. The m...
A direct way of obtaining intra bunch charge distribu-tions is to measure the amplitude roll off as ...
The maximum beam particle intensity and minimum emittance that can be injected, accelerated and stor...
This paper is intended to present the newly implemented wideband (100MHz) bunch oscillation measurem...
A system for bunch-by-bunch detection of transverse proton and antiproton coherent oscillations in t...
A system for bunch-by-bunch detection of transverse proton and antiproton coherent oscillations in t...
Turn-by-turn and bunch-by-bunch diagnostic systems were set up to support various studies. The beam ...
A system was developed for bunch-by-bunch detection of transverse proton and antiproton coherent osc...
The main purpose of the CTF3 preliminary phase is to demonstrate the bunch frequency multiplication....
Measurement of time of arrival of a particle bunch is a fundamental beam diagnostic. The PEP-II/ALS/...
An electronic system is presented which detects synchrotron oscillations of individual bunches with ...
A system for bunch-by-bunch detection of transverse proton and antiproton coherent oscillations in t...
The LHC and SPS transverse dampers use beam position electronics with I,Q detection at 400 MHz and 2...
We discuss the circuit design of a digital multiradian phase detector that measures the phase differ...
A method for computing transverse multibunch growth rates and frequency shifts in rings, which has b...
At the Cornell Electron/Positron Storage Ring, a fast luminosity monitor has been implemented. The m...
A direct way of obtaining intra bunch charge distribu-tions is to measure the amplitude roll off as ...
The maximum beam particle intensity and minimum emittance that can be injected, accelerated and stor...
This paper is intended to present the newly implemented wideband (100MHz) bunch oscillation measurem...