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rt_improvement_by_post-processing

RT Improvement by Post-Processing

Basic Principle

  • bunch of charged particles excites damped oscillation in electronic circuit of the RT
  • oscillation amplitude is proportional to total charge of particle bunch
  • existing GSI RT: signal fed to peak detector  prone to noise at maximum position
  • large dynamic range: ~ 120 dB.
  • typical resolution: ~10 pCRMS (6×10^7 protons)
  • for high current operation resolution drops to 100 nC (6×10^11 protons)

→ insufficient e.g. for transmission control

Bunch Charge determination

[from: “A High Stability Intensity Monitoring System”, M.A. Clarke-Gayther, RAL, Didcot (UK), presented on EPAC, Sitges (E) 1996]

Courtesy of A. Reiter

Post-Processing of RT Oscillation Data

  • idea: : resonant frequency ω0 and decay time constant λ, are fixed by hardware
  • omission of inexact peak detector

→ improved RT resolution by digitization of oscillation data, FFT filtering and envelope fit

Algorithm for bunch charge determination

  • FFT filtering and offset correction
  • identification of maxima and minima until preset S/N value crossed
  • robust estimator of exponential decay curve
  • evaluation of amplitude ~ total pulse charge

rt_improvement_by_post-processing.txt · Last modified: 2019/02/06 16:11 by vschaefer