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tuning_the_s800_xdt [2015/10/26 14:11]
pereira [Analysis line classic PPAC setup (Focus optics only)]
tuning_the_s800_xdt [2015/10/27 14:24]
pereira [Setting up Reaction Settings]
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   * Adjust MCFD threshold:   * Adjust MCFD threshold:
-      * Open configuration file **MCFD16.tcl** in **/user/s800/operations/daq/usb/Configs** +      * Using the [[s800 daq tools#Mesytec CFD gui|Mesytec CFD GUI]], open the configuration file **MCFD16.tcl**  in directory **/user/operations/daq/usb/Configs**
       * The OBJ signal feeding this module is not patched out to data U6       * The OBJ signal feeding this module is not patched out to data U6
-      * The OBJ signal from MCFD-16 module goes to the Mesytec MTDC32 module and scaler (channel OBJ.MCFD.Scint) +      * The OBJ signal from MCFD module goes to the Mesytec MTDC module and scaler (channel OBJ.MCFD.Scint) 
       * Make sure that the threshold of the XFP MCFD channel is reasonable. Rates in scaler channels XFP.Scint and XFP.MCFD.Scint should be comparable       * Make sure that the threshold of the XFP MCFD channel is reasonable. Rates in scaler channels XFP.Scint and XFP.MCFD.Scint should be comparable
       * Adjust MCFD OBJ threshold looking at scalers. The ratio of OBJ to XFP scaler rates (channels OBJ.MCFD.Scint and XFP.MCFD.Scint) should reflect the transmission of the cocktail beam               * Adjust MCFD OBJ threshold looking at scalers. The ratio of OBJ to XFP scaler rates (channels OBJ.MCFD.Scint and XFP.MCFD.Scint) should reflect the transmission of the cocktail beam        
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 ==== Setting Optimization ==== ==== Setting Optimization ====
- 
-=== Focused optics === 
  
   * Expectations for A1900 FP to S800 FP transmission   * Expectations for A1900 FP to S800 FP transmission
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       * Want to balance losses between S800 analysis line and Transfer Hall (the S800 analysis line is typically slightly worse)       * Want to balance losses between S800 analysis line and Transfer Hall (the S800 analysis line is typically slightly worse)
       * Best diagnostic is scalers from S800 FP, object scintillator and XF scintillator       * Best diagnostic is scalers from S800 FP, object scintillator and XF scintillator
-      * Tweak y-quads (while watching scalers) in front of dipole gaps (this works both for Transfer Hall and analysis line); choose elements that have biggest effect with smallest ratio change+      * Using the knob box and the NCS application **QtKM** (file **BLSetup_A1900.gkm**), tweak y-quads (while watching scalers) in front of dipole gaps (this works both for Transfer Hall and analysis line); choose elements that have biggest effect with smallest ratio change
  
   * Document optimized transmission with another run to disk to measure rate of fragment of interest at S800 FP   * Document optimized transmission with another run to disk to measure rate of fragment of interest at S800 FP
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-====== Dispersion Matching tuning ======+====== Dispersion Matching Mode ======
  
 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. 
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        {{:wiki:XG-ALLGATES.png?650|XG.}}        {{:wiki:XG-ALLGATES.png?650|XG.}}
         * The leftmost peak corresponds to reactions with H. The central peak are reaction with C. The goal of the tweak is to make these peaks as narrow as possible         * The leftmost peak corresponds to reactions with H. The central peak are reaction with C. The goal of the tweak is to make these peaks as narrow as possible
-  * Open the NCS application **QtKM** in the Applications Menu. Open file **BLSetup_A1900.gkm**. The magnetic elements that are typically tweaked with the knob box seating on the left side of u6pc5 are **I232TA**, **I236TC**, and **I245TC** which can be found on page **S800 BLine+Spectrograph**. Other elements used to improve the focusing in the object point, and the transmission are **I172QA** and **I174QB**. The goal of the dispersion-matching tuning is to find a compromise between transmission and resolution.+  * Open the NCS application **QtKM** in the Applications Menu. Open file **BLSetup_A1900.gkm**. The magnetic elements that are typically tweaked with the knob box sitting on the left side of u6pc5 are **I232TA**, **I236TC**, and **I245TC** which can be found on page **S800 BLine+Spectrograph**. Other elements used to improve the focusing in the object point, and the transmission are **I172QA** and **I174QB**. The goal of the dispersion-matching tuning is to find a compromise between transmission and resolution.
        {{:wiki:QtKM.png?650|XG.}}        {{:wiki:QtKM.png?650|XG.}}
          * The two figures below show the spectrum **CRDC1.XG!FOI-AFP-BFP** before (top) and after (bottom) the dispersion-matching tuning for a typical experiment. Be aware that the width given by SpecTcl for the selected peak is not too reliable. It is more convenient to do a real gaussian fit. Unfortunatelly this is not an option included in the current version of SpecTcl. That's why some device physicists prefer SpecTk for this type of tuning          * The two figures below show the spectrum **CRDC1.XG!FOI-AFP-BFP** before (top) and after (bottom) the dispersion-matching tuning for a typical experiment. Be aware that the width given by SpecTcl for the selected peak is not too reliable. It is more convenient to do a real gaussian fit. Unfortunatelly this is not an option included in the current version of SpecTcl. That's why some device physicists prefer SpecTk for this type of tuning
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   * Reaction setting to FP    * Reaction setting to FP 
       * Start with Attenuator setting of unreacted beam and step up in intensity       * Start with Attenuator setting of unreacted beam and step up in intensity
-      * Set up beam blocker, if necessary+      * Looking at **CRDC1.RAWS** and/or **CRDC2.RAWS** SpecTcl spectra (shown in **S800_CRDCS.WIN**), set up beam blocker (labeled I255 Slits) in the S3 page of Barney, if necessary 
 +          * Expected "open" values for top and bottom slits are CT ~6.8 and CB ~3.2, respectively 
           * Expect to see unreacted beam if reaction setting is within +/- 3% of unreacted beam setting           * Expect to see unreacted beam if reaction setting is within +/- 3% of unreacted beam setting
           * Should have to move only one of the two blockers unless charge states are present           * Should have to move only one of the two blockers unless charge states are present
-          * A graphic tool is available to help (not yet calibrated) 
           * Try to cut only as much as necessary; depends on           * Try to cut only as much as necessary; depends on
               * What rate limits allow               * What rate limits allow
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           * Probably smaller typical S800 delay needed for HiRA           * Probably smaller typical S800 delay needed for HiRA
       * An example of experiments where auxiliary detectors are not used and, thus, setting up coincidence timing is not an issue are the experiments with tritons run by the charge exchange group       * An example of experiments where auxiliary detectors are not used and, thus, setting up coincidence timing is not an issue are the experiments with tritons run by the charge exchange group
-      * It is not clear whether coincidence setup gets logged as “XDT” or “EXR” +     
   * Choice of setting to be used for coincidence timing setup   * Choice of setting to be used for coincidence timing setup
       * The reaction of interest for the experiment can be used to setup coincidences only if the rate of coincidences is high enough       * The reaction of interest for the experiment can be used to setup coincidences only if the rate of coincidences is high enough
tuning_the_s800_xdt.txt · Last modified: 2023/09/22 15:15 by swartzj