Fast beam losses, due to a vertical coherent instability of high frequency, have been observed in the PS near transition energy, with the high-intensity single-bunch beam for the neutron Time-of-Flight facility (n-ToF). By increasing the longitudinal emittance, the beam could be stabilised. These phenomena can be described by the beam breakup theory, since near transition the longitudinal positions of particles are almost frozen, as in the linac case. Comparison between observations and theory, using Brandt and Gareyte’s formula for single-bunch beam breakup in circular accelerators, shows good agreement.
At high intensities and at certain working points, an instability develops in the CERN PS Booster an...
In linear accelerators the maximum achievable beam current is often limited by the Beam Breakup (BBU...
Cumulative beam breakup (BBU) instability for a single bunch beam in a linear accelerator arises due...
The CERN Proton Synchrotron (PS) routinely crosses transition energy at around 6 GeV in order to acc...
Machine study experiments have been performed at the CERN PS during the week of June 18th, 2012, wit...
The CERN PS crosses transition energy at about 6 GeV by using a second order gamma jump performed wi...
The CERN Proton Synchrotron (PS) routinely crosses transition energy at around 6 GeV in order to acc...
Beams up to 1013 protons were kept circulating for more than 100 ms at various magnet field levels n...
Transition crossing in the CERN PS is critical for the stability of high intensity beams, even with ...
Transition crossing in the CERN PS is critical for the stability of high intensity beams, even with ...
Instabilities driven by the transverse impedance are proven to be one of the limitations for the hig...
Instabilities driven by the transverse impedance are proven to be one of the limitations for the hig...
Since 2003, high-intensity single-bunch proton beams with low longitudinal emittance have been affec...
Analytic and numerical calculations of the beam breakup instability in rf linac cavities are present...
We have developed an analytical model of cumulative beam breakup in linear accelerators that predict...
At high intensities and at certain working points, an instability develops in the CERN PS Booster an...
In linear accelerators the maximum achievable beam current is often limited by the Beam Breakup (BBU...
Cumulative beam breakup (BBU) instability for a single bunch beam in a linear accelerator arises due...
The CERN Proton Synchrotron (PS) routinely crosses transition energy at around 6 GeV in order to acc...
Machine study experiments have been performed at the CERN PS during the week of June 18th, 2012, wit...
The CERN PS crosses transition energy at about 6 GeV by using a second order gamma jump performed wi...
The CERN Proton Synchrotron (PS) routinely crosses transition energy at around 6 GeV in order to acc...
Beams up to 1013 protons were kept circulating for more than 100 ms at various magnet field levels n...
Transition crossing in the CERN PS is critical for the stability of high intensity beams, even with ...
Transition crossing in the CERN PS is critical for the stability of high intensity beams, even with ...
Instabilities driven by the transverse impedance are proven to be one of the limitations for the hig...
Instabilities driven by the transverse impedance are proven to be one of the limitations for the hig...
Since 2003, high-intensity single-bunch proton beams with low longitudinal emittance have been affec...
Analytic and numerical calculations of the beam breakup instability in rf linac cavities are present...
We have developed an analytical model of cumulative beam breakup in linear accelerators that predict...
At high intensities and at certain working points, an instability develops in the CERN PS Booster an...
In linear accelerators the maximum achievable beam current is often limited by the Beam Breakup (BBU...
Cumulative beam breakup (BBU) instability for a single bunch beam in a linear accelerator arises due...