Photon Polarization Analysis Bill Bugg Data selection: 1)PCALE Max cut 2)Visual Inspection. For every cycle of every run we plot and examine a series of.

Slides:



Advertisements
Similar presentations
POLARIMETRY of MeV Photons and Positrons Overview Beam Characterization – undulator photons – positrons Basics of the Transmission Method – for photon.
Advertisements

2010 PREx Run – Dithering & Compton Polarimetry Chun-Min Jen on behalf of the Hall-A JLab. Institution: Syracuse University, NY, 13244,
Lumi Analysis for HAPPEx III / PREX Presented by: Luis Mercado UMass - Amherst 5/18/2007.
5 MeV Mott Measurement for CEBAF Operations group Joe Grames, Marcy Stutzman February 14 th, 2007 Sir Nevill F. Mott at the ceremony with his Nobel Prize.
Image reconstruction and analysis for X-ray computed microtomography Lucia Mancini 1, Francesco Montanari 2, Diego Dreossi 3 1 Elettra - Trieste 2 A.R.P.A.
Copyright © 2010, 2007, 2004 Pearson Education, Inc. All Rights Reserved. Lecture Slides Elementary Statistics Eleventh Edition and the Triola.
09/30/'06SPIN2006, T. Horaguchi1 Measurement of the direct photon production in polarized proton-proton collisions at  s= 200GeV with PHENIX CNS, University.
S6 - 1© 2011 Pearson Education, Inc. publishing as Prentice Hall S6 Statistical Process Control PowerPoint presentation to accompany Heizer and Render.
Positron Asymmetry and Polarization from the E166 September 2005 run Gideon Alexander, Erez Reinherz-Aronis.
Error Propagation. Uncertainty Uncertainty reflects the knowledge that a measured value is related to the mean. Probable error is the range from the mean.
K.T. McDonald DoE Review Aug. 10, E-166 Experiment E-166 is a demonstration of undulator-based polarized positron production for linear colliders.
E166 “Polarized Positrons for Future Linear Colliders” John C. Sheppard E166 Co-spokesman SLAC: August 31, 2004.
K.T. McDonald DoE Review July 29, E-166 Experiment E-166 is a demonstration of undulator-based polarized positron production for linear colliders.
Left: The polarization of the undulator radiation as a function of energy. Right: Calculated positron longitudinal polarization as a function of energy.
R. Dollan, Princeton 22/05/06 Analysis of the September data H. Kolanoski, K. Laihem, S. Riemann, A. Schälicke, DESY R. Dollan,T. Lohse, HU - Berlin.
K. LaihemE166 collaboration LCWS06 Bangalore March 12th 2006 The E166 experiment Development of a polarized positron source for the ILC. Karim Laihem on.
Asymmetry Analysis A. Schälicke, 23 May 2006 Status: independent analyses give similar asymmetries but (significant) different errors.
EMLAB 1 Power Flow and PML Placement in FDTD. EMLAB 2 Lecture Outline Review Total Power by Integrating the Poynting Vector Total Power by Plane Wave.
M. Woods (SLAC) Beam Diagnostics for test facilities of i)  ii) polarized e+ source January 9 –11, 2002.
Handling Data and Figures of Merit Data comes in different formats time Histograms Lists But…. Can contain the same information about quality What is meant.
The PEPPo e - & e + polarization measurements E. Fanchini On behalf of the PEPPo collaboration POSIPOL 2012 Zeuthen 4-6 September E. Fanchini -Posipol.
Understanding ADC Specifications September Definition of Terms 000 Analogue Input Voltage Digital Output Code FS1/2.
Correlation.
Chapter 4 Statistics. 4.1 – What is Statistics? Definition Data are observed values of random variables. The field of statistics is a collection.
Beijing, Feb 3 rd, 2007 LEPOL 1 Low Energy Positron Polarimetry for the ILC Sabine Riemann (DESY) On behalf of the LEPOL Collaboration.
Polarimetry of Proton Beams at RHIC A.Bazilevsky Summer Students Lectures June 17, 2010.
Diana Parno – July 22, 2008 January PREx Test Run: Compton Photon Analysis Diana Parno Carnegie Mellon University HAPPEX Collaboration Meeting.
A study of systematic uncertainties of Compton e-detector at JLab, Hall C and its cross calibration against Moller polarimeter APS April Meeting 2014 Amrendra.
COMPTON POLARIMETRY Collected data Cavity power Status on counting methods Systematic errors and hardware issues.
LMS Stability, Data Correction and the Radiation Accident within the PrimEx Experiment by LaRay J. Benton M.S. Nuclear Physics May 2006 Graduate North.
Chapter 10 Quality Control.
Examination of Corrupted Data in the Tile Calorimeter Stephanie Hamilton Michigan State University The ATLAS Experiment Supervisor: Irene Vichou (U of.
Seven Quality Tools The Seven Tools –Histograms, Pareto Charts, Cause and Effect Diagrams, Run Charts, Scatter Diagrams, Flow Charts, Control Charts.
1 Problem 6.15: A manufacturer wishes to maintain a process average of 0.5% nonconforming product or less less. 1,500 units are produced per day, and 2.
Quality Assurance How do you know your results are correct? How confident are you?
Sampling Error SAMPLING ERROR-SINGLE MEAN The difference between a value (a statistic) computed from a sample and the corresponding value (a parameter)
Photon Polarization Analysis Bill Bugg Data selection: 1)PCALE Max cut
Objectives Determine Detector offsets in hall B reference frame and thus absolute beam position at Hycal Examine Flux calculation and see if beam trips.
© Copyright McGraw-Hill 2000
Statistical Quality Control
Photon Flux Control Liping Gan UNCW. Outline PrimEx-  experiment requirement Tagged photon Procedure to obtain the number of tagged photons Relative.
Chapter 20 Classification and Estimation Classification – Feature selection Good feature have four characteristics: –Discrimination. Features.
Preliminary results for the BR(K S  M. Martini and S. Miscetti.
1 Marek Szczekowski, Artur Ukleja Warsaw Group 3 June 2015 Model-independent search for CPV in three-bodies charm baryon decays Outline Selections for.
1 Warsaw Group May 2015 Search for CPV in three-bodies charm baryon decays Outline Selections Mass distributions and reconstructed numbers of candidates.
1 Occupancy, Rate Effects & Combinatorial Background By Rusty Towell January 8, 2009.
RHIC CNI Polarimeter status RHIC CNI Group February 26, 2008.
 0 life time analysis updates, preliminary results from Primex experiment 08/13/2007 I.Larin, Hall-B meeting.
06/2006I.Larin PrimEx Collaboration meeting  0 analysis.
Electron Spectrometer: Status July 14 Simon Jolly, Lawrence Deacon 1 st July 2014.
Absolute Polarization Measurement at RHIC in the Coulomb Nuclear Interference Region September 30, 2006 RHIC Spin Collaboration Meeting RIKEN, Wako, Japan.
1 HBD Update Itzhak Tserruya DC meeting, May 7, 2008 May7, 2008.
ArgonneResult_ ppt1 Comparison of data and simulation of Argonne Beam Test July 10, 2004 Tsunefumi Mizuno
Analysis of    production ► Data taking ► Reaction identification ► Results for double polarization observable F ► Summary Based on data taken in the.
RHIC pC Polarimeter status A.Bazilevsky For RHIC CNI Group February 26, 2008.
CsI(Tl) Calorimeter and status of the E166 experiment E166 experiment CsI ( Tl) calorimeter construction. Test beam results vs. Geant4 simulation Schedules.
Monitoring Energy Gains Using the Double and Single Arm Compton Processes Yelena Prok PrimEx Collaboration Meeting March 18, 2006.
Chapter 7 Process Control.
5 MeV Mott Measurement for CEBAF Operations group
° status report analysis details: overview; “where we are”; plans: before finalizing result.. I.Larin 02/13/2009.
Problem 6.15: A manufacturer wishes to maintain a process average of 0.5% nonconforming product or less less. 1,500 units are produced per day, and 2 days’
E166 - LEPOL - Low Energy Positron Polarimetry for the ILC
HyCal Energy Calibration using dedicated Compton runs
Volume 34, Issue 5, Pages (May 2002)
Volume 34, Issue 5, Pages (May 2002)
西村美紀(東大) 他 MEGIIコラボレーション 日本物理学会 第73回年次大会(2018年) 東京理科大学(野田キャンパス)
p0 ALL analysis in PHENIX
Colin J. Akerman, Darragh Smyth, Ian D. Thompson  Neuron 
° status report analysis details: overview; “where we are”; plans: before finalizing result.. I.Larin 02/13/2009.
Statistical Quality Control
Presentation transcript:

Photon Polarization Analysis Bill Bugg Data selection: 1)PCALE Max cut 2)Visual Inspection. For every cycle of every run we plot and examine a series of histograms and scatter plots of signals from individual counters. PCALE,D,C,B Ag1Sic Ag2Sic Ag1 Ag2 GCAL CsI (channel 9) Toroid Possi TL,TR,BL,BR X,Y, etc. We look for changes in toroid current, or beam position, saturated channels, missed undulator pulses during the cycle and eliminate runs on this basis.

3)Adjacent runs with opposite field are treated in pairs and averaged to obtain the global asymmetry. 4)To more closely monitor the results I divide the data into segments of approximately pairs(60 run cycles) which are examined separately and then combined. 5)For now I chose not to remove ‘flyers’(results outside 3 sigma) unless study of data for the cycles involved identifies a problem missed earlier.

ANALYSIS In routine analysis background is subtracted and counter data normalized to AG1SiC signal. (Ag1 works about as well) Signal ratios and the difference/sum value evaluated for each pair. For each segment the average value and standard deviation is recorded and a plot of diff/sum vs run pair number made.This is done for the transmitted photon signal measured by Ag2SiC, Ag2 and GCAL For target in data we evaluate asymmetries for CsI channel 9 (crystal 5) and two signals Possisum and AG1which should show no asymmetry. The weighted mean and error of the segment results are then calculated for the entire sample. A few selection examples follow.

Run 2542 target in Good

Run 2590 cycle 1 Target out (Bad)

Run 1571 saturation of Ag2Sic(bad)

For target out data analysis has been completed for the selected runs from the June and September runs(about 200 runs). In addition target in results are obtained for superrun data(lens=340, spectrometer=140,about 450 runs) taken with 0.25X0 target. (Runs ), A small amount of June data is also included. Measurement of the transmitted photon asymmetry is made by 3 separate counters, Ag2Sic, AG2, and GCAL. Ag1Sic counts all photons with approximately equal sensitivity, Ag2 threshold is about 4.5MeV and GCAL signal is proportional to transmitted energy. For target in data we also report the CsI (channel 9) asymmetry and in addition test for asymmetry in the AG1 and PossiSum signal both of which should be small. The latter is a test for asymmetry due to possible effect of analyzing magnet fringe field on the positrons striking the reconversion target.

Example data from June runs

This was the result that made us wonder if fringe field of Analyzing magnet was affecting CsI asymmetry. Possold had a definite asymmetry which was of opposite sign to CsI asymmetry.

September data tuns

Possisum asymmetry is consistent with zero

Target Out data by segment

Target in data by segment