Difference between revisions of "Spectrometer Optics First pass 48p8d"
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+ | '''If you have questions call Vince Sulkosky or Kalyan Allada, Numbers are on white board'''<br> | ||
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+ | ==== Integration with LHRS plan ==== | ||
+ | |||
+ | <table border="1" cellpadding="2" cellspacing="1" width:90%'> | ||
+ | <tr> | ||
+ | <td> LHRS step </td> | ||
+ | <td> RHRS step </td> | ||
+ | <td> Approximate beam time</td> | ||
+ | <td> Goals</td> | ||
+ | <td> Status</td> | ||
+ | </tr> | ||
+ | <tr> | ||
+ | <td>L1 (sieve)</td> | ||
+ | <td>R1 (sieve)</td> | ||
+ | <td> 14h </td> | ||
+ | <td> 20 uA DIS with sieve slit on optics foils, single carbon and LH2</td> | ||
+ | <td><b>Completed</b></td> | ||
+ | </tr> | ||
+ | <tr> | ||
+ | <td> L2 (sieve)</td> | ||
+ | <td> </td> | ||
+ | <td> 3h </td> | ||
+ | <td> Delta Elastic on LH2, 1 uA</td> | ||
+ | <td><b>Completed</b></td> | ||
+ | </tr> | ||
+ | <tr> | ||
+ | <td> L3 (no sieve)</td> | ||
+ | <td> (no sieve) </td> | ||
+ | <td> 3h </td> | ||
+ | <td> Elastic on carbon (Needs A. Camsonne as sieve operator)</td> | ||
+ | <td> In Progress </td> | ||
+ | </tr> | ||
+ | <tr> | ||
+ | <td> </td> | ||
+ | <td> R2 (no sieve)</td> | ||
+ | <td> 4-5h </td> | ||
+ | <td> Delta Elastic on LH2, 20 uA</td> | ||
+ | <td> </td> | ||
+ | </tr> | ||
+ | <tr> | ||
+ | <td> </td> | ||
+ | <td> R3 (no sieve)</td> | ||
+ | <td> 1h </td> | ||
+ | <td> Elastic dummy </td> | ||
+ | <td> </td> | ||
+ | </tr> | ||
+ | <tr> | ||
+ | <td>L1 (sieve)</td> | ||
+ | <td>R1 (sieve)</td> | ||
+ | <td> 4h </td> | ||
+ | <td> 20 uA DIS with sieve slit on 4 cm dummy (Needs A. Camsonne as sieve operator)</td> | ||
+ | <td> </td> | ||
+ | </tr> | ||
+ | <tr> | ||
+ | <td> </td> | ||
+ | <td> R4 (no sieve)</td> | ||
+ | <td> 1h </td> | ||
+ | <td> DIS on dummy and optics </td> | ||
+ | <td>Dropped </td> | ||
+ | </tr> | ||
+ | <tr> | ||
+ | <td> L4 (sieve) </td> | ||
+ | <td> R5 (no sieve)</td> | ||
+ | <td> 1h </td> | ||
+ | <td> Tungsten wire <br> | ||
+ | (Needs D. Mekins as wire operator)<br> | ||
+ | (Needs A. Camsonne as sieve operator)</td> | ||
+ | <td>Dropped</td> | ||
+ | </tr> | ||
+ | </table> | ||
+ | <br> | ||
+ | See [https://hallaweb.jlab.org/wiki/index.php/Winter_2016_optic_plans <b>Left HRS Optics Run Plan</b> ] | ||
+ | <br><br> | ||
+ | |||
==== Step R1: Procedure with Sieve-slit ==== | ==== Step R1: Procedure with Sieve-slit ==== | ||
* Time estimate: 12 hours | * Time estimate: 12 hours | ||
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<td>1.18</td> | <td>1.18</td> | ||
<td>1.617</td> | <td>1.617</td> | ||
− | <td>5 | + | <td>2.5</td> |
− | <td> | + | <td>10</td> |
<td>100k events</td> | <td>100k events</td> | ||
</tr> | </tr> | ||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
− | |||
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<tr> | <tr> | ||
<td>Carbon single foil</td> | <td>Carbon single foil</td> | ||
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<td>1.3</td> | <td>1.3</td> | ||
<td>96k events</td> | <td>96k events</td> | ||
+ | </tr> | ||
+ | <tr> | ||
+ | <td>4 cm Dummy</td> | ||
+ | <td>2.301</td> | ||
+ | <td>0.75</td> | ||
+ | <td>1x1 mm<sup>2</sup></td> | ||
+ | <td>48.74</td> | ||
+ | <td>1.18</td> | ||
+ | <td>1.617</td> | ||
+ | <td>1.8</td> | ||
+ | <td>4</td> | ||
+ | <td>25k events</td> | ||
</tr> | </tr> | ||
</table> | </table> | ||
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==== Step R2: Delta Scan with Proton Elastic (without sieve slit)==== | ==== Step R2: Delta Scan with Proton Elastic (without sieve slit)==== | ||
− | * Time estimate: 3 hours | + | * 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. | * Trained personnel will be required to remove the 1-inch tungsten sieve-slit collimator from the front face of the HRS. | ||
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* Once beam is centered on the cross-wire target, have MCC turn off the raster. Make sure the spectrometers still have rates above cosmics by checking <br>the scaler rates. | * Once beam is centered on the cross-wire target, have MCC turn off the raster. Make sure the spectrometers still have rates above cosmics by checking <br>the scaler rates. | ||
* Take a run with the with <b>raster off</b> for both LHRS and RHRS. | * Take a run with the with <b>raster off</b> for both LHRS and RHRS. | ||
− | * 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. | + | * Electron rates assume 200 μm of tungsten. For LHRS, the rate is only for the central hole of the sieve slit (~ 0.023 mSr acceptance), and 8% delta acceptance. |
* <b>A GMp expert will determine when enough good electron events have been collected.</b> | * <b>A GMp expert will determine when enough good electron events have been collected.</b> | ||
Latest revision as of 00:11, 26 February 2016
If you have questions call Vince Sulkosky or Kalyan Allada, Numbers are on white board
Contents
Integration with LHRS plan
LHRS step | RHRS step | Approximate beam time | Goals | Status |
L1 (sieve) | R1 (sieve) | 14h | 20 uA DIS with sieve slit on optics foils, single carbon and LH2 | Completed |
L2 (sieve) | 3h | Delta Elastic on LH2, 1 uA | Completed | |
L3 (no sieve) | (no sieve) | 3h | Elastic on carbon (Needs A. Camsonne as sieve operator) | In Progress |
R2 (no sieve) | 4-5h | Delta Elastic on LH2, 20 uA | ||
R3 (no sieve) | 1h | Elastic dummy | ||
L1 (sieve) | R1 (sieve) | 4h | 20 uA DIS with sieve slit on 4 cm dummy (Needs A. Camsonne as sieve operator) | |
R4 (no sieve) | 1h | DIS on dummy and optics | Dropped | |
L4 (sieve) | R5 (no sieve) | 1h | Tungsten wire (Needs D. Mekins as wire operator) |
Dropped |
Step R1: Procedure with Sieve-slit
- Time estimate: 12 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 | 2.5 | 10 | 100k 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 |
4 cm Dummy | 2.301 | 0.75 | 1x1 mm2 | 48.74 | 1.18 | 1.617 | 1.8 | 4 | 25k events |
Step R2: 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 1.96 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 |
Step R3: 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 |
Step R4: 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 |
Step R5: Cross-wire Target Run
- Time estimate: 5 hours (includes access to install wire target and left HRS Sieve-slit)
* After the above runs are completed, ask for the target group (call Dave Meekins) to insert the cross-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 * At the same time have the Techs or A. Camsonne install the left HRS sieve-slit. The right HRS sieve-slit remains off. * Take a run with the cross-wire target with 2x2 mm2 rastered beam, and verify that the beam is centered on the cross-wire target using spot++. * If the beam in not centered, then ask MCC to move the beam until the rastered beam spot is centered on the wires. * Once beam is centered on the cross-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 with raster off for both LHRS and RHRS. * Electron rates assume 200 μm of tungsten. For LHRS, 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.
Spectrometer | Target | Sieve Slit | Raster | Ebeam [GeV] | P0 [GeV/c] | θe [deg] | Q2 [GeV2] | W [GeV] | Rate [Hz] at 1 μA | minutes at 1 μA | Good Electrons |
Right HRS | 200 μm tungsten wire | OUT | Off | 2.301 | 0.75 | 48.74 | 1.18 | 1.617 | 3.28 | 30 | 5.9k events |
Left HRS | 200 μm tungsten wire | IN | Off | 2.301 | 1.0 | 16.63 | 0.19 | 1.769 | 1.3 | 30 | 2.3k events |
- 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.