with high precision using resonant depolarization. In a stor-age ring where the beam lifetime is dominated by large-angle intrabeam (Touschek) scattering, the relative beam polarization can be measured by relative changes in the beam lifetime because of the dependence of the Møller scattering rate on the polarization. In the fully Touschek-dominated regime, the change in lifetime at the ALS due to a complete depolarization is larger than 10%. The en-ergy calibration has been used at the ALS to perform high precision measurements of the machine stability, machine reproducibility and the momentum compaction factor.
Linear collider designs foresee some bends of about 5-10 mrad. The spin precession angle of one TeV ...
The CERN Large Electron Positron collider (LEP) has been dedicated to the measurement of the mass Mz...
AbstractAt the VEPP-4M collider the record accuracy of 10−6 of an absolute beam energy calibration w...
In addition to precise dipole field measurements the method of resonant electron spin depolarization...
The Set up for energy calibration of electron beam will be built by the method of resonant depolariz...
This paper presents measurements of the GeV-scale electron beam energy for the storage rings at the ...
Measurements of the beam energy of electron storage rings based on the resonant spin depolarization ...
Experiments on high precision mass measurement of particles require precise beam energy calibration....
Electron beam loss due to intra-beam scattering, the Tou-schek effect, in a storage ring depends on ...
Electron beam loss due to intra-beam scattering, the Touschek effect, in a storage ring depends on t...
The resonance depolarization method was very successfully used in the experiments at LEP, where the ...
The ANKA electron storage ring operates in the energy range from 0.5 to 2.5 GeV. An energy calibrati...
With a 7 T wiggler in operation all attempts to detect the resonant depolarization of the electro...
The ANKA electron storage ring operates in the energy range from 0.5 to 2.5 GeV. An energy calibrati...
The future medium energy physics program at the electron stretcher accelerator ELSA of Bonn Universi...
Linear collider designs foresee some bends of about 5-10 mrad. The spin precession angle of one TeV ...
The CERN Large Electron Positron collider (LEP) has been dedicated to the measurement of the mass Mz...
AbstractAt the VEPP-4M collider the record accuracy of 10−6 of an absolute beam energy calibration w...
In addition to precise dipole field measurements the method of resonant electron spin depolarization...
The Set up for energy calibration of electron beam will be built by the method of resonant depolariz...
This paper presents measurements of the GeV-scale electron beam energy for the storage rings at the ...
Measurements of the beam energy of electron storage rings based on the resonant spin depolarization ...
Experiments on high precision mass measurement of particles require precise beam energy calibration....
Electron beam loss due to intra-beam scattering, the Tou-schek effect, in a storage ring depends on ...
Electron beam loss due to intra-beam scattering, the Touschek effect, in a storage ring depends on t...
The resonance depolarization method was very successfully used in the experiments at LEP, where the ...
The ANKA electron storage ring operates in the energy range from 0.5 to 2.5 GeV. An energy calibrati...
With a 7 T wiggler in operation all attempts to detect the resonant depolarization of the electro...
The ANKA electron storage ring operates in the energy range from 0.5 to 2.5 GeV. An energy calibrati...
The future medium energy physics program at the electron stretcher accelerator ELSA of Bonn Universi...
Linear collider designs foresee some bends of about 5-10 mrad. The spin precession angle of one TeV ...
The CERN Large Electron Positron collider (LEP) has been dedicated to the measurement of the mass Mz...
AbstractAt the VEPP-4M collider the record accuracy of 10−6 of an absolute beam energy calibration w...