Difference between revisions of "PREX2AuxiliaryMeasurements"
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#* use target lock, about 1 uA | #* use target lock, about 1 uA | ||
## <font color="blue">Retake Optics </font> including dp = 0, +-1% (scale all magnets) | ## <font color="blue">Retake Optics </font> including dp = 0, +-1% (scale all magnets) | ||
− | ## <font color="blue">shift beam +/- 4mm in horizontal , retake dp = 0 optics | + | ## <font color="blue">Beam position dependence </font> |
− | ## <font color="blue">use 90 degree Carbon target | + | ##* shift beam +/- 4mm in horizontal , retake dp = 0 optics |
+ | ## <font color="blue">Target Z comparison</font> | ||
+ | ##* use 90 degree Carbon target, Compare y-targ reconstruction to 45 degree carbon target | ||
# <font color="blue">Cavity vs Striplines</font> | # <font color="blue">Cavity vs Striplines</font> | ||
#* measure carbon hole location with 50nA cavity lock and spot++ | #* measure carbon hole location with 50nA cavity lock and spot++ |
Revision as of 15:55, 17 August 2019
Optics and Q2
- Energy Measurement (Bob, talk to Doug)
- look for 1e-3 accuracy. Non invasive?
- VDC/GEM Rate study
- Do this first! Wednesday?
- 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
- 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
- Optics Data
- Sieve in, VDC data. thin Carbon
- about 500k per run
- use target lock, about 1 uA
- Retake Optics including dp = 0, +-1% (scale all magnets)
- Beam position dependence
- shift beam +/- 4mm in horizontal , retake dp = 0 optics
- Target Z comparison
- use 90 degree Carbon target, Compare y-targ reconstruction to 45 degree carbon target
- Cavity vs Striplines
- 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
- Dynamic Thermal-Induced Density Rearrangement
- 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 each case
Backgrounds
- Thin Lead Target to check for inelastics at high-resolution
- Previously done with different kinematics. could be repeated.
- Thin C12 to measure diamond background spectrum?
- Thick C12 to measure diamond background fraction?
- A_T detectors (Bob)
- Significant asymmetries found in A_T detectors, requires investigation
- Pole tip re-scattering
- 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
- Blank PMT (Dustin)
- Integrating measurement
- only if stubby quartz shows something
- Rescattering measurement
- repeat of previous measurements. Roughly 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)
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