Difference between revisions of "Spectrometer Optics First pass 48p8d"

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(Delta Scan with Proton Elastic (without sieve slit))
(Dummy Target Runs)
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* Move the target to "15 cm Dummy"
 
* Move the target to "15 cm Dummy"
 
* Take R-HRS run with same setting as previous step. We need at least 100 k events.
 
* Take R-HRS run with same setting as previous step. We need at least 100 k events.
* Take data with this setting for 2 hours
+
* Take data with this setting for 1 hour
 
<br>
 
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<table border="1"  style="width:80%">
 
<table border="1"  style="width:80%">
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     <td>0</td>
 
     <td>0</td>
 
     <td>13.2</td>
 
     <td>13.2</td>
     <td>2</td>
+
     <td>1</td>
     <td>100k events</td>
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     <td>50k events</td>
 
   </tr>
 
   </tr>
 
</table>
 
</table>

Revision as of 13:16, 23 February 2016

Procedure with Sieve-slit

  • Time estimate: 14 hours
* Trained personnel will be required to install the 1-inch tungsten sieve-slit collimator onto the front face of the HRS.
* If you need to increase the spectrometer momentum setting, make sure you cycle Q2 and Q3 as per the cycling procedure.
* Take sieve-slit runs with the multi-foil carbon target (optics) for the inelastic kinematics in the table.
* Electron rates assume 5 carbon foils, only 37 out of 155 sieve holes per foil have events (~ 0.4 mSr acceptance), and 8% delta acceptance.
* Electron rates assume 2 aluminum foils, only 43 out of 155 sieve holes per foil have events (~ 0.47 mSr acceptance), and 8% delta acceptance.
* Electron rates assume 15 cm LH2 target, only 45 out of 155 sieve holes have events (~ 0.49 mSr acceptance), and 8% delta acceptance.
* Before moving on to the next target, a GMp expert will determine online how many good electron events have been collected. 
Target Ebeam [GeV] P0 [GeV/c] Raster θe [deg] Q2 [GeV2] W [GeV] Rate [Hz] at 20 μA hours at 20 μA Good Electrons
Optics 2.301 0.75 Off 48.74 1.18 1.617 5.6 5 100k events
4 cm Dummy 2.301 0.75 1x1 mm2 48.74 1.18 1.617 3.5 4 50k events
Carbon single foil 2.301 0.75 Off 48.74 1.18 1.617 2.2 1.3 10.3k events
15 cm LH2 2.301 0.75 2x2 mm2 48.74 1.18 1.617 20.0 1.3 96k events


  • Wire Target Run
* After the above runs are completed, ask for the target group (call Dave Meekins) to insert the wire-target (we are not allowed to do it). 
* Target expert will need to go to the Hall and manually move the target in position, so ask for controlled access before starting this step  
* Take a run with the wire target with 2x2 mm2 rastered beam, and verify that the beam is horizontally centered on the wire target using spot++.
* If the beam in not centered, then ask MCC to move the beam until the rastered beam spot is centered horizontally.
* Once beam is centered on the wire target, have MCC turn off the raster.  Make sure the spectrometers still have rates above cosmics by checking the scaler rates.
* Take a run with the wire target with raster off.
* Electron rates assume 200 μm of tungsten, the rate is only for the central hole of the sieve slit (~ 0.023 mSr acceptance), and 8% delta acceptance.
* A GMp expert will determine when enough good electron events have been collected.
Target Raster Ebeam [GeV] P0 [GeV/c] θe [deg] Q2 [GeV2] W [GeV] Rate [Hz] at 1 μA hours at 1 μA Good Electrons
200 μm tungsten wire Off 2.301 0.75 48.74 1.18 1.617 0.015 4 200


  • After finishing this step ask for Controlled access and call the target expert to move the wire-target out of the way. Also call Hall-A Tech on-call to remove the R-HRS sieve-slit.


Delta Scan with Proton Elastic (without sieve slit)

  • Time estimate: 3 hours
* Trained personnel will be required to remove the 1-inch tungsten sieve-slit collimator from the front face of the HRS.
* Take runs with the 15 cm liquid hydrogen target for the elastic kinematics in the table.
* There will be a time lapse between settings until the right dipole reaches the desired momentum and is stable.
* If you need to increase the spectrometer momentum setting, make sure you cycle Q2 and Q3 as per the cycling procedure.
* Rate estimates only include elastic electrons and does not include rate from inelastic events or from the target endcaps. 
* The Q2 for these settings is 1.96 GeV2.
Ebeam (GeV) k' (GeV) Raster θe (deg) ΔP (%) Rate [Hz] at 20 μA minutes at 20 μA Good Electrons
2.301 1.304 2x2 mm2 48.74 -4 176 20 210k events
2.301 1.279 2x2 mm2 48.74 -2 176 20 210k events
2.301 1.254 2x2 mm2 48.74 0 176 50 500k events
2.301 1.229 2x2 mm2 48.74 +2 176 20 210k events
2.301 1.203 2x2 mm2 48.74 +4 176 20 210k events


Dummy Target Runs

  • Go back to the ΔP = 0% elastic setting. Make sure the R-HRS P0 = 1.254 GeV.
  • Move the target to "15 cm Dummy"
  • Take R-HRS run with same setting as previous step. We need at least 100 k events.
  • Take data with this setting for 1 hour


Ebeam (GeV) k' (GeV) Raster θe (deg) ΔP (%) Rate [Hz] at 20 μA hours at 20 μA Good Electrons
2.301 1.254 2x2 mm2 48.74 0 13.2 1 50k events


Procedure without Sieve-slit

  • Time estimate: 1 hour
* Take a run at the following kinematics without the sieve-slit collimator.
* If you need to increase the spectrometer momentum setting, make sure you cycle Q2 and Q3 as per the cycling procedure.
* Electron rates assume 5 carbon foils or 2 Al dummy foils, 5 mSr acceptance, and 8% delta acceptance.
* A GMp expert will check the data quality.

Target Ebeam [GeV] P0 [GeV/c] Right Q1 Current [A] θe [deg] Q2 [GeV2] W [GeV] Rate [Hz] at 20 μA minutes at 20 μA Good Electrons
Optics 2.301 0.75 153.36 48.74 1.18 1.617 70.5 12 50k events
4 cm Dummy 2.301 0.75 153.36 48.74 1.18 1.617 37.4 22 50k events