Difference between revisions of "Fall 2016 LHRS optic plans"
From Hall A Wiki
(→Step L3: Dummy Target Runs) |
(→Step L4: Procedure without Sieve-slit) |
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<br> | <br> | ||
+ | * <b>4th Pass (E<SUB>beam</SUB> = 8.5 GeV)</b> Time estimate: 19 days @ 15 μA | ||
<table border="1" style="width:80%"> | <table border="1" style="width:80%"> | ||
<tr> | <tr> | ||
<td>Target</td> | <td>Target</td> | ||
+ | <td>Raster</td> | ||
<td>E<SUB>beam</SUB> [GeV]</td> | <td>E<SUB>beam</SUB> [GeV]</td> | ||
<td>P<sub>0</sub> [GeV/c]</td> | <td>P<sub>0</sub> [GeV/c]</td> | ||
− | |||
<td>θ<SUB>e</SUB> [deg]</td> | <td>θ<SUB>e</SUB> [deg]</td> | ||
<td>Q<SUP>2</SUP> [GeV<SUP>2</SUP>]</td> | <td>Q<SUP>2</SUP> [GeV<SUP>2</SUP>]</td> | ||
− | <td> | + | <td> Electron Rate [Hz] at 15 μA</td> |
− | <td> | + | <td><b>PAC days</b> at 15 μA</td> |
− | <td> | + | </tr> |
− | <td> | + | <tr> |
+ | <td>15 cm LH2</td> | ||
+ | <td>2 x 2 mm<sup>2</sup></td> | ||
+ | <td>8.517</td> | ||
+ | <td>2.081</td> | ||
+ | <td>48.75</td> | ||
+ | <td>12.08</td> | ||
+ | <td>0.018</td> | ||
+ | <td>19 (for 29k events)</td> | ||
</tr> | </tr> | ||
<tr> | <tr> | ||
<td>Optics</td> | <td>Optics</td> | ||
− | <td> | + | <td>Off</td> |
− | <td> | + | <td>8.517</td> |
− | <td> | + | <td>0.85</td> |
− | <td> | + | <td>48.75</td> |
− | <td> | + | <td>4.93</td> |
− | <td> | + | <td>6.9</td> |
− | <td> | + | <td>1 hour (for 24k events)</td> |
− | + | ||
− | + | ||
</tr> | </tr> | ||
<tr> | <tr> | ||
− | <td> | + | <td>15 cm Dummy</td> |
− | + | <td>2 x 2 mm<sup>2</sup></td> | |
− | + | <td>8.517</td> | |
− | <td> | + | <td>2.081</td> |
− | <td> | + | <td>48.75</td> |
− | <td> | + | <td>12.08</td> |
− | <td> | + | <td>----</td> |
− | <td> | + | <td>1 hour</td> |
− | <td> | + | |
− | + | ||
</tr> | </tr> | ||
</table> | </table> | ||
<br> | <br> |
Revision as of 18:45, 8 October 2016
Contents
Step L1: Procedure with Sieve-slit
- Time estimate: 1 hour
* 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. * Adjust the prescale factors to keep the DAQ deadtime below 10%. * 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 | minutes at 60 μA | Good Electrons |
Optics | 2.217 | 1.0 | Off | 17.5 | 0.20 | 1.72 | 540 | 32 | 1M events |
15 cm LH2 | 2.217 | 1.0 | 3x3 mm2 | 17.5 | 0.20 | 1.72 | 4600 | 10.0 | 2.7M events |
Step L2: Delta Scan with Proton Elastic (with sieve slit)
- Time estimate: 1.5 hours
* Keep the 1-inch tungsten sieve-slit collimator on the front face of the left HRS. * Take runs with the 15 cm liquid hydrogen target for the elastic kinematics in the table. * Wait until the left 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. * Adjust the prescale factors to keep the DAQ deadtime below 10%. * The Q2 for these settings is 0.41 GeV2.
Ebeam (GeV) | k' (GeV) | Raster | θe (deg) | ΔP (%) | Rate [Hz] at 10 μA | minutes at 10 μA | Good Electrons |
2.217 | 2.078 | 3x3 mm2 | 17.5 | -4 | 10,000 (2500 Hz with ps = 4) | 10 | 1M events |
2.217 | 2.038 | 3x3 mm2 | 17.5 | -2 | 10,000 (2500 Hz with ps = 4) | 10 | 1M events |
2.217 | 1.998 | 3x3 mm2 | 17.5 | 0 | 10,000 (2500 Hz with ps = 4) | 10 | 1M events |
2.217 | 1.958 | 3x3 mm2 | 17.5 | +2 | 10,000 (2500 Hz with ps = 4) | 10 | 1M events |
2.217 | 1.918 | 3x3 mm2 | 17.5 | +4 | 10,000 (2500 Hz with ps = 4) | 10 | 1M events |
Step L3: Dummy Target Runs
- Go back to the ΔP = 0% elastic setting. Make sure the L-HRS P0 = 1.998 GeV.
- Move the target to "15 cm Dummy"
- Take L-HRS run with same setting as previous step.
- Take data with this setting for 10 minutes
Ebeam (GeV) | k' (GeV) | Raster | θe (deg) | ΔP (%) | Rate [Hz] at 10 μA | minutes at 10 μA | Good Electrons |
2.217 | 1.998 | 3x3 mm2 | 17.5 | 0 | 460 | 10 | 270k 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.
- 4th Pass (Ebeam = 8.5 GeV) Time estimate: 19 days @ 15 μA
Target | Raster | Ebeam [GeV] | P0 [GeV/c] | θe [deg] | Q2 [GeV2] | Electron Rate [Hz] at 15 μA | PAC days at 15 μA |
15 cm LH2 | 2 x 2 mm2 | 8.517 | 2.081 | 48.75 | 12.08 | 0.018 | 19 (for 29k events) |
Optics | Off | 8.517 | 0.85 | 48.75 | 4.93 | 6.9 | 1 hour (for 24k events) |
15 cm Dummy | 2 x 2 mm2 | 8.517 | 2.081 | 48.75 | 12.08 | ---- | 1 hour |