Beam position reconstruction Pengjia Zhu 1 Analysis Overview ● ● ● BCM Calibration (finished) BPM Calibration (finished) Asymmetry correction for different acceptance(on going) Hardware Overview ● Hardware overview ● Low beam current 50-100nA ● polarization of NH3 target sensitive with temperature and radicals ● Super harp installed to work in high current pulsed mode beam ● New BPM receiver with digital processing system ● Two raster systems ● Fast raster, 2mmx2mm rectangle ● Slow raster, 2cm diameter circle ● 2.5/5 T Transverse target magnet field ● Two chicane dipole magnet installed ● Limited space between second chicane magnet and target ● Antenna BPM chamber installed Harp data analysis ● ● BPM: non-invasive device, relative readout, need to be calibrated before use Harp: invasive device, read absolute beam position by using three wires, used for calibrating BPM Harp data analysis Offline data: ● Index – sample index for harp, related to the number of steps the fork moved ● Position – value of the wire position for each index Position information implete during online data recording, use index information to extend: pos=a*index+b ● Signal Harp data analysis Absolute beam position gotten from peaks of three wires: (based on the survey information of three wires) Harp data analysis harp1 chicane chicane BPMA harp2 BPMB Absolute beam position at BPM location got from harp: Based on survey information Straight through setting needed Harp data analysis BPMA harp2 BPMB If no straight through calibration: One BPM should be well calibrated from straight through setting Use one calibrated BPM and one harp to calibrate another BPM Antenna BPM Chamber Signal fo r antenna : each 2 2 r −ρ ϕ=ϕ0 I 2 2 r +ρ −2r ρcos(θ−θ 0) θ= π 4 3π 4 − 3π 4 −π 4 angle for 4 antennas I: Beam current r: BPM vacuum chamber radius (17.3 mm) ρ: radial position o f beam θ0 : angle position o f beam Assume: Infinite chamber Antenna small enough 9 BPM calibration : calibration constant 1. raw signal received in antenna VS recorded ADC data(linear region): 2. diff/sum value(temp value): 3. nonlinearity correction for diff/sum(temp value): 4. Calibrate with harp data Position from harp, already transfered to BPM local coordinate(use survey data) Constants b: got from linear fit for current VS recorded ADC data ● Some bpm calibrations did the calibration for several currents ● Each harp scan position(one point) corresponding to several runs with different current(100nA,75nA,50nA) ● Assumption: those runs with different current have same beam position ● Influence: key parameter to eliminate the current effection, let calculated position immuse to fluctuating current(50~100nA), especially for the difference of b+ - b- Pedestal – ADC value when no beam Pedestal changes, use the most closed run's value. Pedestals calculated from pedestal run or ADC value during beam trip Pedestal change during experiment for left arm with 6 settings BPM signal connected to DAQ system Have redundancy in case a system would fail Happex have better bit resolution and integrate longer time, more accurate 2Hz Software filter used for offline data analysis Fixed trigger rate for Happex DAQ, could be treated as a sampling ADC 2Hz filter used for getting average beam position, to get better resolution Position and angle at target (center beam position) ● Straight through – linear transport from BPMs to target ● With target field Transport functions from BPMs to target Functions fitted from BdL simulation from existed target field map Position and angle at target (center beam position) BPM A: 95.5cm upstream the target BPM B: 69cm upstream the target Only 26.5cm between them 0.2/0.27mm uncertainty at BPM A/B → 1.1mm at target Position event by event at target Average beam position info from BPM position dispersed from fast raster, info from fast raster's magnet current, recorded in ADC position dispersed from slow raster, info from slow raster's magnet current, recorded in ADC Slow raster size: calibrated from carbon hole Fast raster size: calibrated from BPM, them transport to target Optional slow raster information handling – slow raster phase reconstruction For slow raster: ● Known frequency ● Known function ● ● ● Can easily reconstruct the phase from data Improve accuracy caused by ADC resolution Can extract fast clock frequency from fit Blue dot:data red curve: fitted Uncertainty Center position Uncertainty source : ● ● ● ● ● Pedestal ~ 0.7mm,0.7mrad BPM resolution ~ 0.5mm,0.5mrad Survey ~ 0.5mm Target magnet field 0.3~0.9mrad for theta, depends on field setting Calibration constant ~ 0.7mm,0.7mrad ● Harp/BPM Survey for calibration runs ● BPM resolution for calibration runs Total uncertainty for center position for best situation: 1mm for pos, 1.1mrad for angle thesis defense time in USTC: March May <--------- my plan(2015) November lowest requirement: ● two papers ● BPM NIM paper, done for draft, publish soon ● ??? ● preliminary physics result ● Earliest physics result --- asymmetry ? Post graduate plan(short term): Looking for a job: company/postdoc
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