Difference between revisions of "PREX2AuxiliaryMeasurements"
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== Optics and Q2 == | == Optics and Q2 == | ||
− | + | # <font color="blue">Energy Measurement </font> (Doug) | |
− | # <font color="blue"> | + | #* <font color="red"> Priority High </font> |
− | #* <font color="red"> | + | #* Can be performed Day shift Monday or Tuesday? |
− | #* | + | #* look for 1e-3 accuracy. Non invasive. |
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− | #* | ||
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# <font color="blue">Optics Data</font> (Cip) | # <font color="blue">Optics Data</font> (Cip) | ||
#* requires access to prepare, about 8-10 hrs data, access to backout | #* requires access to prepare, about 8-10 hrs data, access to backout | ||
Line 27: | Line 14: | ||
#* use target lock, about 1 uA | #* use target lock, about 1 uA | ||
#* no raster | #* no raster | ||
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## <font color="blue">Beam position dependence </font> (2 hrs) | ## <font color="blue">Beam position dependence </font> (2 hrs) | ||
+ | ##* <font color="red"> Priority High - this data has not been taken during PREX </font> | ||
##* shift beam +/- 4mm in horizontal , retake dp = 0 optics | ##* shift beam +/- 4mm in horizontal , retake dp = 0 optics | ||
## <font color="blue">Target Z comparison</font> (2 hrs) | ## <font color="blue">Target Z comparison</font> (2 hrs) | ||
+ | ##* <font color="red"> Priority High - this data has not been taken during PREX </font> | ||
##* use 90 degree Carbon target, Compare y-targ reconstruction to 45 degree carbon target | ##* use 90 degree Carbon target, Compare y-targ reconstruction to 45 degree carbon target | ||
− | # <font color="blue"> | + | ## <font color="blue">Retake Optics Data</font> (Cip) (6 hours) |
− | #* | + | ##* <font color="red"> High Priority (unless Q2 results shown to be stable over run, then reconsider) </font> |
− | + | ##* including dp = 0, +-1% (scale all magnets) | |
− | # | ||
− | #* | ||
− | |||
# <font color="blue">Dynamic Thermal-Induced Density Rearrangement </font> (Bob, Chandon, Siyu, Cip) (4 hours) | # <font color="blue">Dynamic Thermal-Induced Density Rearrangement </font> (Bob, Chandon, Siyu, Cip) (4 hours) | ||
+ | #* <font color="red"> High Priority (unless we can measure significant density variation at low current) </font> | ||
#* requires access to prepare, 3 hrs data + analysis, access to backout | #* requires access to prepare, 3 hrs data + analysis, access to backout | ||
#* Sieve in. S0 on, GEMs on, VDC Off. Production raster. | #* Sieve in. S0 on, GEMs on, VDC Off. Production raster. | ||
Line 48: | Line 33: | ||
#* Repeat measurement of scattering density over target x vs y | #* Repeat measurement of scattering density over target x vs y | ||
#* If different, do the same on a pristine target | #* If different, do the same on a pristine target | ||
− | #* Evaluate Q2 for each case | + | #* Evaluate Q2 (for specific sieve holes?) in each case |
+ | # <font color="blue">Cavity vs Striplines </font> (Cip) (~1.5 hrs) | ||
+ | #* <font color="red"> High Priority </font> | ||
+ | #* measure carbon hole location with 50nA cavity lock and spot++ | ||
+ | #* measure carbon hole with 0.5uA tgt lock and spot++ | ||
+ | #* show these are the same, within a 1mm or so | ||
+ | # <font color="maroon">VDC/GEM Rate study</font> (Bob, Chandon, Siyu) | ||
+ | #* <font color="maroon"> Completed (awaiting results)</font> | ||
+ | #* Requires access, 3 hrs data, access to back out | ||
+ | #* Detector counting mode. | ||
+ | #* S0 trigger | ||
+ | #* Lead target | ||
+ | #* production raster and beam position | ||
+ | #* Use cavity lock, low current | ||
+ | #* start at low S0 rate (50kHz?) and go up in rate to 500 kHz, in several steps (50, 100, 200, 500 kHz) | ||
+ | #* turn off VDC, continue up to 2MHz rates in GEMs (1MHz, 2MHz) | ||
+ | #* Compare Q2 measurements at each rate from GEMS and VDC to look for rate dependence | ||
+ | # <font color="maroon">Q2 from damaged target</font> (Bob) | ||
+ | #* <font color="maroon"> Completed (awaiting results)</font> | ||
+ | #* measure Q2 from most damaged target (Pb10?) | ||
+ | #* compare to Q2 from pristine target | ||
+ | #* If these are different - we need a plan to correct for damage or measure all used targets | ||
+ | #* can be combined with previous study, add 1 hr for target move and measurement | ||
== Backgrounds == | == Backgrounds == |
Revision as of 10:52, 25 August 2019
Optics and Q2
- Energy Measurement (Doug)
- Priority High
- Can be performed Day shift Monday or Tuesday?
- look for 1e-3 accuracy. Non invasive.
- Optics Data (Cip)
- requires access to prepare, about 8-10 hrs data, access to backout
- Sieve in, VDC data. thin Carbon
- about 500k per run
- use target lock, about 1 uA
- no raster
- Beam position dependence (2 hrs)
- Priority High - this data has not been taken during PREX
- shift beam +/- 4mm in horizontal , retake dp = 0 optics
- Target Z comparison (2 hrs)
- Priority High - this data has not been taken during PREX
- use 90 degree Carbon target, Compare y-targ reconstruction to 45 degree carbon target
- Retake Optics Data (Cip) (6 hours)
- High Priority (unless Q2 results shown to be stable over run, then reconsider)
- including dp = 0, +-1% (scale all magnets)
- Dynamic Thermal-Induced Density Rearrangement (Bob, Chandon, Siyu, Cip) (4 hours)
- High Priority (unless we can measure significant density variation at low current)
- requires access to prepare, 3 hrs data + analysis, access to backout
- Sieve in. S0 on, GEMs on, VDC Off. Production raster.
- 1uA
- Pb10
- Measure scattering density over target x vs y
- 70uA
- Repeat measurement of scattering density over target x vs y
- If different, do the same on a pristine target
- Evaluate Q2 (for specific sieve holes?) in each case
- Cavity vs Striplines (Cip) (~1.5 hrs)
- High Priority
- measure carbon hole location with 50nA cavity lock and spot++
- measure carbon hole with 0.5uA tgt lock and spot++
- show these are the same, within a 1mm or so
- VDC/GEM Rate study (Bob, Chandon, Siyu)
- Completed (awaiting results)
- Requires access, 3 hrs data, access to back out
- Detector counting mode.
- S0 trigger
- Lead target
- production raster and beam position
- Use cavity lock, low current
- start at low S0 rate (50kHz?) and go up in rate to 500 kHz, in several steps (50, 100, 200, 500 kHz)
- turn off VDC, continue up to 2MHz rates in GEMs (1MHz, 2MHz)
- Compare Q2 measurements at each rate from GEMS and VDC to look for rate dependence
- Q2 from damaged target (Bob)
- Completed (awaiting results)
- measure Q2 from most damaged target (Pb10?)
- compare to Q2 from pristine target
- If these are different - we need a plan to correct for damage or measure all used targets
- can be combined with previous study, add 1 hr for target move and measurement
Backgrounds
- Thin Lead Target to check for inelastics at high-resolution (Bob)
- Previously done with different kinematics. could be repeated.
- valuable illustration for presentation/publication
- Thin C12 to measure diamond background spectrum? (Bob)
- I'm unclear on the value of this, since the carbon is presumably a very small fraction. But might it be easier to see than the lead inelastic?
- Thick C12 to measure diamond background fraction?
- I'm unclear on the value of this, since we are not set up terribly well for yields at very different rates, the radiation is so different, and I don't know how accurately the targets are known.
- A_T detectors (Bob)
- Significant asymmetries found in A_T detectors, requires investigation
- Pole tip re-scattering (Bob, Cip?)
- Q2 or septum mis-tune, to increase interception on pole tip and improve poletip rescattering estimate
- Stubby Quartz (Dustin)
- Replace detector quartz with superelastic stub
- Integrating measurement
- High priority
- Blank PMT (Dustin)
- Integrating measurement
- Low priority, needed only if stubby quartz shows something
- Rescattering measurement (Bob, Cip?)
- repeat of previous measurements. (Lower priority?)
- requires about 1 shift
- Detune spectrometer up in momentum, to dump elastic peak into spectrometer wall.
- Measure (integrating mode) signal in main detectors. Requires HV boot leg to get higher gain (is 10x possible?)
- should scale all spectrometer magnets _except_ Q3.
Detectors
- Linearity Studies (PITA + current scans) (Caryn)
- Linearity Studies (LED) (Dustin)
Other
- Sign check
- run Moller, Compton, and parity DAQ for quick PITA scan
Moller polarimetry
- Repeat measurements
- need enough granularity to track changing polarization.
- at least 2x/week = 6 measurements
- Target uniformity
Compton polarimetry
- No-target runs
- Laser polarization optimization
- Laser polarization flip
- linearity studies