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tuning_the_s800_xdt [2015/10/26 13:56]
pereira [Checking Particle ID and rate at S800 FP]
tuning_the_s800_xdt [2015/10/26 14:02]
pereira
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       * Adjust the TDC delays of E1 up, down using the Delay GUI       * Adjust the TDC delays of E1 up, down using the Delay GUI
       * In principle, the TACs delays don't need to be adjusted       * In principle, the TACs delays don't need to be adjusted
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 ==== Checking Particle ID and rate at S800 FP ==== ==== Checking Particle ID and rate at S800 FP ====
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       * Take a run on disk        * Take a run on disk 
       * Measure the beam intensity again and calculate the average value       * Measure the beam intensity again and calculate the average value
-      * In SpecTcl GUI, click **Attach to File** and select data file **run-xxxx-xx.evt** in directory **/user/s800/stagearea/experiment/runxxxx**, where xxxx stands for the run number+      * In [[s800 SpecTcl|SpecTcl GUI]], click **Attach to File** and select data file **run-xxxx-xx.evt** in directory **/user/s800/stagearea/experiment/runxxxx**, where xxxx stands for the run number
       * Check the run time and live time from the corresponding scaler file in directory **/user/s800/converged_daq/scalers**       * Check the run time and live time from the corresponding scaler file in directory **/user/s800/converged_daq/scalers**
       * Calculate the rate and purity and compare with the value in the A1900 FP to determine the transmission       * Calculate the rate and purity and compare with the value in the A1900 FP to determine the transmission
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 ==== Analysis line classic PPAC setup (Focus optics only) ==== ==== Analysis line classic PPAC setup (Focus optics only) ====
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   * "Classic" PPACs are the default detector, not TPPACs or CRDCs   * "Classic" PPACs are the default detector, not TPPACs or CRDCs
       * Classic PPACs have rate limitations from pileups       * Classic PPACs have rate limitations from pileups
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 ==== Setup beamline ==== ==== Setup beamline ====
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   * Object and XF scintillators and intermediate image PPACs inserted if they will be used   * Object and XF scintillators and intermediate image PPACs inserted if they will be used
       * If Object scintillator will not be used, there is no reason to look at beam on it unless to debug a problem with the transmission       * If Object scintillator will not be used, there is no reason to look at beam on it unless to debug a problem with the transmission
  
   * Set spectrograph Brho for unreacted fragment   * Set spectrograph Brho for unreacted fragment
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 ==== Start scalers ==== ==== Start scalers ====
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   * Use s800 account   * Use s800 account
  
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 === Focused optics === === Focused optics ===
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   * Expectations for A1900 FP to S800 FP transmission   * Expectations for A1900 FP to S800 FP transmission
       * 80% or better for mid-Z fragments       * 80% or better for mid-Z fragments
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 === Matched optics === === Matched optics ===
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   * Typically much more time is invested for optimizing optics for matched optics than for focused optics   * Typically much more time is invested for optimizing optics for matched optics than for focused optics
  
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 ==== Setting up Reaction Settings ==== ==== Setting up Reaction Settings ====
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   * Calculating reaction setting   * Calculating reaction setting
       * Center unreacted beam at S800 FP       * Center unreacted beam at S800 FP
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 ==== Coincidences ==== ==== Coincidences ====
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   * Overview   * Overview
       * Most experiments at the S800 involve setting up an auxiliary detector system (e.g. SeGA, HiRA, etc) to be used in coincidence with the standard detectors of the S800.       * Most experiments at the S800 involve setting up an auxiliary detector system (e.g. SeGA, HiRA, etc) to be used in coincidence with the standard detectors of the S800.
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 ====== Dispersion Matching tuning ====== ====== Dispersion Matching tuning ======
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 In the dispersion-matching optics, the S800 focal point is achromatic, i.e. the position of the beam in the dispersive direction does not depend on the momentum. As a consequence, the beam is momentum-dispersed on the target area (pivot point) with a dispersion of about 10 cm/%. The main goal of the tuning is to ensure that the position and angle dispersion are cancelled at the focal plane, thus maximizing the resolution at that point. We also want a good image in the object position, which will also contribute to increase the resolution at the focal plane.  In the dispersion-matching optics, the S800 focal point is achromatic, i.e. the position of the beam in the dispersive direction does not depend on the momentum. As a consequence, the beam is momentum-dispersed on the target area (pivot point) with a dispersion of about 10 cm/%. The main goal of the tuning is to ensure that the position and angle dispersion are cancelled at the focal plane, thus maximizing the resolution at that point. We also want a good image in the object position, which will also contribute to increase the resolution at the focal plane. 
  
tuning_the_s800_xdt.txt ยท Last modified: 2023/09/22 15:15 by swartzj