Difference between revisions of "Fall 2016 LHRS optic plans"

From Hall A Wiki
Jump to: navigation, search
(Step L1: Procedure with Sieve-slit)
(Step L1: Procedure with Sieve-slit)
Line 21: Line 21:
 
     <td> Good Electrons</td>
 
     <td> Good Electrons</td>
 
   </tr>
 
   </tr>
   <tr>
+
   <tr>/
 
     <td>Optics</td>
 
     <td>Optics</td>
 
     <td>2.217</td>
 
     <td>2.217</td>
 
     <td>1.0</td>
 
     <td>1.0</td>
 
     <td><b>Off</b></td>
 
     <td><b>Off</b></td>
     <td>48.75</td>
+
     <td>17.5</td>
 
     <td>1.51</td>
 
     <td>1.51</td>
 
     <td>1.287</td>
 
     <td>1.287</td>
Line 38: Line 38:
 
     <td>1.0</td>
 
     <td>1.0</td>
 
     <td>3x3 mm<sup>2</sup></td>
 
     <td>3x3 mm<sup>2</sup></td>
     <td>48.75</td>
+
     <td>17.5</td>
 
     <td>1.51</td>
 
     <td>1.51</td>
 
     <td>1.287</td>
 
     <td>1.287</td>

Revision as of 15:29, 8 October 2016

Step L1: Procedure with Sieve-slit

  • Time estimate: 6 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 9 carbon foils, only 37 out of 155 sieve holes per foil have events (~ 0.41 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 60 μA hours at 60 μA Good Electrons
Optics 2.217 1.0 Off 17.5 1.51 1.287 14 2 100k events
15 cm LH2 2.217 1.0 3x3 mm2 17.5 1.51 1.287 40.0 1.0 144k events


Step L2: Delta Scan with Proton Elastic (without sieve slit)

  • Time estimate: 3-4 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 1.86 GeV2.
Ebeam (GeV) k' (GeV) Raster θe (deg) ΔP (%) Rate [Hz] at 60 μA minutes at 60 μA Good Electrons
2.217 1.277 3x3 mm2 48.75 -4 650 10 390k events
2.217 1.253 3x3 mm2 48.75 -2 650 10 390k events
2.217 1.228 3x3 mm2 48.75 0 650 20 780k events
2.217 1.204 3x3 mm2 48.75 +2 650 10 390k events
2.217 1.179 3x3 mm2 48.75 +4 650 10 390k events


Step L3: Dummy Target Runs

  • Go back to the ΔP = 0% elastic setting. Make sure the L-HRS P0 = 1.228 GeV.
  • Move the target to "15 cm Dummy"
  • Take R-HRS run with same setting as previous step.
  • Take data with this setting for 1 hour


Ebeam (GeV) k' (GeV) Raster θe (deg) ΔP (%) Rate [Hz] at 40 μA hours at 40 μA Good Electrons
2.217 1.228 3x3 mm2 48.75 0 19.5 1 70k events


Step L4: 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 9 carbon foils or 1 single carbon foil, 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 60 μA minutes at 60 μA Good Electrons
Optics 2.217 1.0 173.808 48.75 1.51 1.287 250 15 220k events
Single Carbon 2.217 1.0 173.808 48.75 1.51 1.287 56 15 50k events