1 Data taking & ONLINE analysis at MCR Hiromi Okada June, 2008.

Slides:



Advertisements
Similar presentations
Beam direction and flux measured by MUMON K. Matsuoka (Kyoto) for the MUMON group Contents: 1.Beam stability (direction/flux) 2.Absolute  beam flux.
Advertisements

VETO Analysis Update Michael Wood University of Massachusetts, Amherst Outline Introduction and basics Reconstruction packages Efficiencies Simulation.
PHENIX local RUN9 RHIC meeting Manabu Togawa for the PHENIX 1.
Jin Huang & Vincent Sulkosky Massachusetts Institute of Technology Boson 2010 Workshop Sept 20, JLab.
1 PID Detectors & Emittance Resolution Chris Rogers Rutherford Appleton Laboratory MICE CM17.
Y. Karadzhov MICE Video Conference Thu April 9 Slide 1 Absolute Time Calibration Method General description of the TOF DAQ setup For the TOF Data Acquisition.
The polarized hydrogen jet target measurements at RHIC Andrei Poblaguev Brookhaven National Laboratory The RHIC/AGS Polarimetry Group: I. Alekseev, E.
SMRD April 2007 Status of the atmospheric muon studies Piotr Mijakowski OUTLINE: Primary muon spectrum at the sea level Primary muon.
DIS 2006 TSUKUBA April 21, 2006 Alessandro Bravar Spin Dependence in Polarized Elastic Scattering in the CNI Region A. Bravar, I. Alekseev, G. Bunce, S.
Polarimetry of Proton Beams at RHIC A.Bazilevsky Summer Students Lectures June 17, 2010.
DIS 2006 Tsukuba, April 21, 2006 Alessandro Bravar Proton Polarimetry at RHIC Alekseev, A. Bravar, G. Bunce, S. Dhawan, R. Gill, W. Haeberli, H. Huang,
Status of W analysis in PHENIX Central Arm Kensuke Okada (RBRC) For the PHENIX collaboration RHIC Spin Collaboration meeting November 21, /21/20091K.Okada.
1 Introduction to Dijet Resonance Search Exercise John Paul Chou, Eva Halkiadakis, Robert Harris, Kalanand Mishra and Jason St. John CMS Data Analysis.
14/02/2007 Paolo Walter Cattaneo 1 1.Trigger analysis 2.Muon rate 3.Q distribution 4.Baseline 5.Pulse shape 6.Z measurement 7.Att measurement OUTLINE.
Jin Huang M.I.T. For Transversity Collaboration Meeting Sept 24, JLab.
Observation of W decay in 500GeV p+p collisions at RHIC Kensuke Okada for the PHENIX collaboration Lake Louise Winter Institute February 20, /20/20101.
Status of TPC experiment ---- Online & Offline M. Niiyama H. Fujimura D.S. Ahn W.C. Chang.
7/30/99Douglas E. Fields for the E950 Collaboration 1 A CNI Polarimeter for RHIC Spin Results from IUCF CE75 & AGS E950 M. Bai, G. Bunce*, H. Huang, Y.
Absolute polarimetry at RHIC Hiromi Okada (BNL) I. Alekseev, A. Bravar, G. Bunce, S. Dhawan, O. Eyser, R. Gill, W. Haeberli, O. Jinnouchi, A. Khodinov,
V.L. Kashevarov. Crystal Collaboration Meeting, Mainz, September 2008 Photoproduction of    on protons ► Introduction ► Data analysis.
Systematic Errors Studies in the RHIC/AGS Proton-Carbon CNI Polarimeters Andrei Poblaguev Brookhaven National Laboratory The RHIC/AGS Polarimetry Group:
Preliminary analysis of p-Pb data update n. 6 Lorenzo Bonechi LHCf Catania meeting – 19 December 2013.
Yury Gurchin June 2011 MEASUREMENT OF THE CROSS-SECTION IN DP-ELASTIC SCATTERING AT THE ENERGIES OF 500 AND 880 MEV AT NUCLOTRON.
1 The results of the study of dp-elastic scattering at the energies from 500 to 1000 MeV/nucleon A.A Terekhin et al. Joint Institute for Nuclear Research,
October 14, 2004 Single Spin Asymmetries 1 Single Spin Asymmetries for charged pions. Overview  One physics slide  What is measured, kinematic variables.
K.O. Eyser --- Absolute Polarization Measurement at RHIC in the Coulomb Nuclear Interference Region -1- Absolute Polarization Measurement at RHIC in the.
Polarization Measurements of RHIC-pp RUN05 Using CNI pC-Polarimeter Itaru Nakagawa (RIKEN/RBRC) On behalf of CNI Polarimeter Group I.G.Alekseev A A.Bravar.
Polarization Measurement of 100GeV Proton Beams at RHIC with CNI pC Polarimeter Itaru Nakagawa (RIKEN/RBRC) On behalf of CNI Polarimeter Group I.G.Alekseev.
1 Calorimeter in G4MICE Berkeley 10 Feb 2005 Rikard Sandström Geneva University.
M. Dugger, February Triplet polarimeter study Michael Dugger* Arizona State University *Work at ASU is supported by the U.S. National Science Foundation.
» Absolute Polarimetry of Proton Beams at RHIC« Oleg Eyser for the RHIC Polarimetry Group International Workshop on Polarized Sources, Targets and Polarimetry.
Mitglied der Helmholtz-Gemeinschaft Calibration of the COSY-TOF STT & pp Elastic Analysis Sedigheh Jowzaee IKP Group Talk 11 July 2013.
Mass production (Super-K) Setup of jnubeam – 3 horn 250 kA – 30-GeV proton beam of Gaussian distribution (  x,y = cm) – On center, parallel beam.
PRESORT OF THE DATA OF THE COLOGNE TEST EXPERIMENT ● Quality and integrity of data ● Detector numbering and positions ● Calibrations and gain stability.
1 A first look at the KEK tracker data with G4MICE Malcolm Ellis 2 nd December 2005.
» RHIC Polarimetry « Oleg Eyser for the RHIC Polarimetry Group 2014 RHIC Retreat, August 14.
Proton Polarimetry at RHIC K. Oleg Eyser for the CNI polarimeter group Newport News, VA, October 25, 2013.
A. Zelenski a, G. Atoian a *, A. Bogdanov b, D.Raparia a, M.Runtso b, D. Steski a, V. Zajic a a Brookhaven National Laboratory, Upton, NY, 11973, USA b.
H-Jet polarimeter status report Yousef Makdisi RSC 07/28/06.
00 Cooler CSB Direct or Extra Photons in d+d  0 Andrew Bacher for the CSB Cooler Collaboration ECT Trento, June 2005.
Run6 CNI Analysis: Concluding Remarks and Summary of Systematic Uncertainties A.Bazilevsky For RHIC CNI group RHIC Spin Collaboration Meeting November.
POLARIZATION MEASUREMENTS AND ABSOLUTE POLARIZATION VALUES EVOLUTION DURING PROTON BEAM ACCELERATION IN THE RHIC ACCELERATOR COMPLEX A.Zelenski, T.Roser,
Search for High-Mass Resonances in e + e - Jia Liu Madelyne Greene, Lana Muniz, Jane Nachtman Goal for the summer Searching for new particle Z’ --- a massive.
04/06/07I.Larin pi0 systematic error 1  0 error budget Completed items (review) Updated and new items (not reported yet) Items to be completed.
RHIC CNI Polarimeter status RHIC CNI Group February 26, 2008.
Thomas Roser Snowmass 2001 June 30 - July 21, 2001 Proton Polarimetry Proton polarimeter reactions RHIC polarimeters.
06/2006I.Larin PrimEx Collaboration meeting  0 analysis.
1 EMCAL Reconstruction in Pass pp 900 GeV 29/03/2010 Gustavo Conesa Balbastre.
Info Read SEGY Wavelet estimation New Project Correlate near offset far offset Display Well Tie Elog Strata Geoview Hampson-Russell References Create New.
Absolute Polarization Measurement at RHIC in the Coulomb Nuclear Interference Region September 30, 2006 RHIC Spin Collaboration Meeting RIKEN, Wako, Japan.
27/02/04 ATLAS weekTileCal Athena tutorial, part 21 TileCal Athena tutorial Part 2: Reading GEANT hits from ZEBRA and POOL Reading HLT and testbeam ByteStream.
RHIC Polarimetery A.Bazilevsky for RHIC Polarimetry group RHIC Spin Collaboration Metting April 10 (Friday), 2009.
RHIC pC polarimeter what has been achieved and what needs to be done Osamu Jinnouchi RBRC 2/10/05 RSC meeting.
RHIC pC Polarimeters in Run9: Performance and Issues A.Bazilevsky for the RHIC CNI Group Polarimetry Worshop BNL, July 31, 2009.
Jin Huang Brookhaven National Lab ● Optics General ● Test Run Calibration ● Comment on Full Runs Trying to collect materials from three years ago. May.
Matteo Volpi, Luca Fiorini Timing study with Muons at 90º from first beam PRELIMINARY STUDY (Barcelona) 1 Tile Timing Group meeting 17 September 2008.
TOF detector in PHENIX experiment PHENIX time-of-flight counter The PHENIX time-of-flight (TOF) counter serves as a particle identification device for.
H-jet Run at Injection A. Dion, H. Huang, A. Poblaguev, A. Zelenski, and YM.
20 April 2007MICE Tracker Phone Meeting1 Analysis of cosmic/self-triggerd data of station 5 Hideyuki Sakamoto MICE Tracker Phone Meeting 20 th April 2007.
EZDC spectra reconstruction and calibration
Introduction Goal: Can we reconstruct the energy depositions of the proton in the brain if we are able to reconstruct the photons produced during this.
° status report analysis details: overview; “where we are”; plans: before finalizing result.. I.Larin 02/13/2009.
Status report Minjung Kim
Yuxi Pan University of California, Los Angeles
Photoproduction of poh pairs on the proton
Today’s topics; New AN and ANN results at s = 6.9 GeV
NKS2 Meeting with Bydzovsky NKS2 Experiment / Analysis Status
Run5 Analysis of RHIC-pC Polarimeter
p0 ALL analysis in PHENIX
° status report analysis details: overview; “where we are”; plans: before finalizing result.. I.Larin 02/13/2009.
Presentation transcript:

1 Data taking & ONLINE analysis at MCR Hiromi Okada June, 2008

2 Contents Memos. How to start data taking. Preparation for Physics data taking. What I did during RUN8 period.

3 Memos: Login to pc2pc.rhic.bnl.gov machine as user e950: >ssh pc2pc.rhic.bnl.gov –l e950 –X (pass: ) RUN8 raw data: >cd /usr/local/polarim/bin/jet name of data: xDDMM.5AB.data DD is day, MM is month and AB is from 01~ Ex. The first data on Feb. 26 th is “x dat”. RUN-log for RUN8: (Ron and Yousef know how to look) >cd /usr/local/polarim/bin >oocalc JETRUNLOG08.sxc &

4 How to start data taking: To start GUI on Yousef’s document page2: >cd /usr/local/polarim/bin >./jetrun.pl & To start data taking: follow the instruction of Yousef’s document page 1-2. This GUI is a set of “data-taking+online analysis” To find output ROOT files (ntuple): >cd /usr/local/polarim/bin/root name of output root file: xDDMM.5AB.root DD is day, MM is month and AB is from 01~ Ex. Online analysis for “x dat” is “x root”. To re-do online analysis only: >./jetana.pl &

5 Ntuple structure: typedef struct { int rev; // revolution number int bunch; // bunch number int bpol; // bunch polarization (-1, 0, +1) int jpol; // jet polarization (-1, 0, +1) float time; // reconstructed time float ampl; // reconstructed amplitude float quality; // event quality float ekin; // recoil kinetic energy, keV float tof; // time of flight, ns float rmass; // recoil mass, GeV float angle; // pi/2 -, radians float mmass2; // missing mass squared, GeV // int wave[192]; } EventStruct;

6 Preparation for Physics data taking 1. Energy calibration. 2. Banana hunting. 3. Acceptance check (by moving vertical position of the RHIC- beam). 4. time0 check. 5. ROUGH HJET profile measurement by fixing the RHIC beam position, by moving HJET base position (  To find a good HJET base position). 6. Spin and bunch pattern check. 7. Channel selection for every energy-bin 8. Repeat items 2~ 6 for the another RHIC beam!

7 1. Energy calibration How to take  calibration data?  Retract calibration shutter.  ask Yousef, Anatoli or Ron.  Just run GUI on slide 4. You do not need the RHIC beam nor the HJET! How to analyze calibration data?  See page 8. How to update energy/ADC coefficients?  See page 12. How often you need to repeat this?  RUN8 case, every 3 days or more.  (If you have the RHIC beam, HJET, or both, you can take calibration data!) Calibration  : 5.486MeV (Am), MeV (Gd) Use Am source data for ONLINE.

8 How to analyze calibration data? 1.You can copy a tool from “/home/okadah/JET2008/Online_tools/AmPeak.C” to your directory (here directory name is “tmp”. 2.And then create “Calib” directory below your “tmp” directory. 3.How to use: Start root session >root –l Run a tool >.x AmPeak.C(DDMM,5AB) Output file “Calib/calib_xDDMM.5AB.txt” Contents : 1st column is channel#, 2 nd column is energy coefficient [KeV/ADC]

9 AmPeak.C picks peak position of ADC spectra for every channel

10 1, , , , , , , , , , , ,50.33 ……… 88, , , , , , , , ,49.87 Example of output file: /home/okadah/HJET2008/Onl ine_tools/Calib/x txt 1st column: channel#, 2nd column: energy coefficient [KeV/ADC] Coeffcient = 5486[keV]/peak[ADC]

11 Energy coefficienttime0 Use only 1(time0) and 2 (energy coefficient) columns. Do not use shaded area

12 How to update energy/ADC coefficients txt? Copy old config file to new config file at: /usr/local/polarim/config >cp calib_1602.dat calib_XXXX.dat XXXX is arbitrary 4 digit (DDMM is recommended). Then you have to modify “jetanal.sh”.  Open /usr/local/polarim/bin/jetanal.sh  Comment out old line starts from “export..”  Add new line export HJET_CALIB="../config/calib_${2:-XXXX}.dat“ See next page!

13 #!/bin/bash # Analize(reanalize) jet run RUN=$1 export HJET_ROOTFILE="root/"$RUN".root" export HJET_DATAFILE="jet/"$RUN".data" #export HJET_CALIB="../config/calib_${2:-3003}.dat" Hiromi changed t0=t0+4nsec #export HJET_CALIB="../config/calib_${2:-1602}.dat" #export HJET_CALIB="../config/calib_${2:-1802}.dat" export HJET_CALIB="../config/calib_${2:-XXXX}.dat" export HJET_DAQ="" if [ "x"$1 == "x" ] ; then echo "Usage:./jetanal.sh [ ]" else root -b jetrun.C fi “#” means “comment out”. New file “calib_XXXX.dat” (XXXX is arbitrary) /usr/local/polarim/bin/jetanal.sh

14 x y jet (-10, -10) mm 2. Banana hunting Ch#1 Ch# (0, -4) mm Collision point – detector: 80cm Cover kinetic energy: 0.5 < T R < 5 MeV (But we use 1.0<T R < 4 MeV.) Each detector has 16 readout channels. Experimental setup

15 Ch#1 Ch#4 Ch#5 Ch#8 Ch#16 ADC TDC ADC and TDC correlations from one of the detector Use /home/okadah/JET2008/Online_tools/LookBanana.C

16 Useful tools for BANANA hunting: To make a plot in slide 15 and 17:  ADC vs. TDC 2-D plot for every channel.  /home/okadah/JET2008/Online_tools/LookBanana.C >root –l >.x LookBanana.C >Enter run name: xDDMM.5AB >Enter mode:  1 You can modify easily change TDC  ToF, ADC  Energy in these source codes (After you get correct energy coefficients and time0). Blue mode -1, yellow mode 1

17 3. Acceptance check Si1 Si2 Si3 Si4 Si5 Si6 x y Si2 Si3 Si1 Si5 Si4 Si6 In case the RHIC beam is too high (low), Si#3 and Si#4 (Si#1 and Si#6) may be shadowed by collimator. collimator HJET Use /home/okadah/JET 2008/Online_tools/ LookBanana.C Collimator shadowed !

18 x y (x,y)=(0, 0) =(0,-1) =(0,-2) =(0,-4) Try wider range! Please try the RHIC beam vertical scan!! Fix horizontal (x-position) and scan vertical (along y-axis)

19 4. time0 check: What is time0?  We measure signal arrival time start from the RHIC clock.  Arrival time = “ToF” + “signal process & travel time”  Time0 = “signal process & travel time” How to estimate time0? Look at BANANA plot and estimate time0 by eyes.  for example, see next page. /home/okadah/JET2008/Online_tools/LookBanana3.C (You might set a same values for all 96 channels for ONLINE: see page 11 the first column.)

20 TOF TRTR 20 nsec Si#3 Si#1 Si#4 Si#6 Si#5 Si#2 TOF TRTR Recoil particle identification How to look at BANANA plot to estimate time0 by eyes? Confirm BANANA locus is between two solid lines. ToFcal+10 [nsec] ToFcal  10 [nsec] Use /home/okadah/JET 2008/Online_tools/ LookBanana3.C

21 5. ROUGH HJET profile measurement Fix the RHIC beam position (one is at the center, the other is at far away). Move HJET base for every 1.5mm step (gage=6000). Take short time data (5 minutes is enough, but make sure always same minutes). Calculate event counts for every gage point. Use /home/okadah/JET2008/Online_toosl/LookProfile.C  BOX shape event cut (1.2<T R <2.5 MeV, 25<ToF<55 nsec). Look at source code for details. Make a plot (gage position vs. event counts).

22 Sample HJET profile Each event count is 5 minutes data and is calculated by LookProfile.C You can find a good HJET base position!

23 6. Spin and bunch pattern check. You need to check bunch pattern and spin pattern for every fill. Use /home/okadah/JET2008/Online_tools/LookBunch.C >root –l >.x LookBunch.C >Enter run name: xDDMM.5AB If you run with blue (yellow) mode, you need to check blue (yellow) side spin and bunch pattern. If aboard gap is wrong position, you need to modify ONLINE analysis program source (/usr/local/polarim/bin/HJET.h).  Open HJET.h source file and find “#define BUNCHCORR 40”.  In RUN8, we used yellow-clock only. And I guess the same for RUN9~. You might need to shift bunch0 for BLUE.  (I set BUNCHCORR = 40 for RUN8,  ask Igor if you do not know.)

24 Output sample plots of LookBunch.C Sample data x (BLUE mode). Filled color corresponds spin sign: pink , green . This sample is BLUE mode, then you need to look at “blue side” data (left.) You need to confirm aboard gap sit proper position.

25 /usr/local/polarim/bin/HJET.h (part) /* Class definition for online Hjet data analysis I. Alekseev & D. Svirida, */ #ifndef HJET_H #define HJET_H #include #include "rhicpol.h" #include "rpoldata.h" #include "HCut.h" #define MAXWAVEFORMS 100 #define MAXSICHAN 100 #define MAXQUEUE 100 #define LINEPOINTS 6 #define DETECTORS 6 #define BUNCHCORR 40 //RUN6 80, RUN8 40 Hiromi Feb. 25, 2008 #define LARGE_VALUE (1.0E50) typedef struct { int chan; // Channel number int rev; // revolution number int bunch; // bunch number int bpol; // bunch polarization (-1, 0, +1) int jpol; // jet polarization (-1, 0, +1) Change “BUNCHCORR” value as needed.

26 TOF TRTR Ch#1 Ch#4 Ch#5 Ch#8 Ch#9 Ch#16 Use /home/okadah/JET2008/Online_tools/LookBanana.C 7. Channel selection for every energy-bin pp elastic scattering events have 2 correlations: “Energy-ToF” and “Energy-recoil angle (channel#)”.

27 T R and ch# correlation Ch#   R Y B Si#3 Si#1 Si#4 Si#6 Si#5 Si#2 Ch# TRTR Forward scattered particle identification (TOF cut is applied already.) Use /home/okadah/JET2008/ Online_tools/LookEx.C

28 How to select proper channels?  Look at event distribution for energy-bin. Elastic scattering: recoil angle and kinetic energy of recoil proton are highly correlated.  Within a certain energy bin, hit channels are always same!  I picked 3 channels. Si 1 Si2 Si3 Si4 Si5 Si6 BLUE mode Use /home/okadah/JET2008/Onli ne_tools/LookEvent.C You can pink proper channel numbers from this plot by your eyes.

29 Useful tools for Channel selection for every energy-bin : To make a plot in page 24:  Energy vs. ToF 2-D plot for every Si detector.  /home/okadah/JET2008/Online_tools/LookEx.C >root –l >.x LookEx.C >Enter run name: xDDMM.5AB To make an event count distribution plot in page 25:  /home/okadah/JET2008/Online_tools/LookEvent.C >root –l >.x LookEvent.C >Enter run name: xDDMM.5AB >Enter energy bin (1-6): 1 Check every energy-bin! And pick channel numbers from plots

30 How to use selected channel information? This information is needed for a tool:  /home/okadah/online_tools/LookAsymEvent.C To calculate 8 types of event counts (sorted by energy-bin, spin-info., left-right). Please modify source code followed by comments in the source code. >root –l >.x LookAsymEvent.C >Enter run name: xDDMM.5AB >Enter mode (blue mode -1, yellow moew 1): 1 Output txt format file into directort AsymTxt/xDDMM.5AB.txt Plot channel# vs. Energy plot. Selected events are in red color. See next page.

31 Example plot channel# vs. Energy plot. Selected events are in red color. You should confirm your channel selection (page 28) is reasonable. Use /home/okadah/online_tools /LookAsymEvent.C

32 8. Repeat items 2~ 6 for the another RHIC beam!

33 What I did during RUN8 physics data taking period. Signal/Background ratio stability check by eyes at least every fill.  Use /home/okadah/JET2008/Online_tools/LookEvent.C  See next page to find how to check data.  target,  beam and ratio=  beam /  target calculation for every beam swap (every beam mode change).  Use /home/okadah/JET2008/Online_tools/CtoANB.C for blue mode data, and CtoANY.C for yellow mode data.  You need to prepare input file: runB.txt (runY.txt) to run CtoANB.C (CtoANY.C). Please look at the source code for more details.

34 Signal/Background stability check BLUE mode Elastic scattering: recoil angle and kinetic energy of recoil proton are highly correlated.  Within a certain energy bin, hit channels are always same!  I picked 3 channels. Check background level and signal/background ratio. Signal Background (inside cuts accidentally) Use /home/okadah/JET2008/Online_tools/ LookEvent.C

35 ONLINE beam polarization Repeat same thing for every beam-period. Use /home/okadah/JET2008/Online_tools/CtoANB.C for blue mode data, and CtoANY.C for yellow mode data.