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tuning_the_s800_xdt [2015/10/26 13:21]
pereira [Timing setup]
tuning_the_s800_xdt [2015/10/26 14:01]
pereira
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   * If necessary, adjust delays:   * If necessary, adjust delays:
-      * Using ULM GUI assign TDC-start to one of the Inspect Trigger channels and trigger the scope with it +      * Using the [[S800 DAQ tools#Trigger GUI|ULM trigger GUI]] assign TDC-start to one of the Inspect Trigger channels and trigger the scope with it 
-      * Select the timing signals (Delay inspect channels) E1 up, OBJ and XFP with the Delay GUI and look at them in the scope +      * Select the timing signals (Delay inspect channels) E1 up, OBJ and XFP with the [[S800 DAQ tools#Delay Window|Delay GUI]] and look at them in the scope 
-      * Adjust the TDC delays of OBJ and XFP using the delay boxes connected to the CANBERRA CFD in data U6+      * Adjust the TDC delays of OBJ and XFP using the delay boxes connected to the CANBERRA CFD 454 in data U6
       * 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
  
 ==== Checking Particle ID and rate at S800 FP ==== ==== Checking Particle ID and rate at S800 FP ====
-  Establish PID + 
-      * Refer to information on setting from A1900 FP +  * Select SpecTcl window **S800_PID.win** in directory **/user/s800/operations/spectcl/Windows**  
-      * dE-TOF +      * The three columns correspond to the PID determined with the **RF-FP** ToF (left), **OBJ-FP** (center), and **XFP-FP** (right) 
-           dE signal from Ion Chamber +      * The first (top) row corresponds to the Phillips TDC 
-           TOF from XF or Object scintillator to S800 FP +      The second row corresponds to the MTDC with just the first hit included 
-           Not necessary to implement dEor TOF-based corrections +      The third row corresponds to the ORTEC TACs. Note that there is not **RF-FP TAC** 
-      Document rate of fragment of interest with run to disk +      You might need to adjust the limits of the spectra to get a good resolution 
-          * Measure beam current with appropriate Faraday cups + 
-          Timed run+{{:wiki:SpecTcl-e14019-PID-r103.jpg?850|S800_PID.win page}} 
 + 
 + 
 +  Establish PID and measure rate 
 +      * Determine the blob that corresponds to the unreacted beam (refer to information on setting from A1900 FP) 
 +      * Take gates around the fragment of interest 
 +      * Measure the beam intensity the appropriate faraday cup 
 +      * Take a run on disk  
 +      * Measure the beam intensity again and calculate the average value 
 +      * 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** 
 +      * Calculate the rate and purity and compare with the value in the A1900 FP to determine the transmission 
 + 
 + 
 + 
 + 
 + 
 + 
  
  
  
 ==== Analysis line classic PPAC setup (Focus optics only) ==== ==== Analysis line classic PPAC setup (Focus optics only) ====
 +
   * "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 ====
 +
   * 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
 +
  
 ==== Start scalers ==== ==== Start scalers ====
 +
   * Use s800 account   * Use s800 account
  
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 === Focused optics === === Focused optics ===
 +
   * 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 ===
 +
   * 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 ====
 +
   * Calculating reaction setting   * Calculating reaction setting
       * Center unreacted beam at S800 FP       * Center unreacted beam at S800 FP
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 ==== Coincidences ==== ==== Coincidences ====
 +
   * 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 ======
 +
 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 · Last modified: 2023/09/22 15:15 by swartzj