1 Unfolding Study 07/11/12. 2 RooUnfold Using the RooUnfold 1.1.1 In this study we make response.

Slides:



Advertisements
Similar presentations
1 Data Analysis II Beate Heinemann UC Berkeley and Lawrence Berkeley National Laboratory Hadron Collider Physics Summer School, Fermilab, August 2008.
Advertisements

Interjet Energy Flow. Patrick Ryan, Univ. of Wisconsin Collaboration Meeting, June 6, Patrick Ryan University of Wisconsin Claire Gwenlan Oxford.
RooUnfold unfolding framework and algorithms
Selection: i) Used “basic cuts” described in my NuBarPID talk (slide 3). 74.4% of CC events pass this cut. ii) Used David’s PID cut at -0.2 to remove NC.
Statistical Image Modelling and Particle Physics Comments on talk by D.M. Titterington Glen Cowan RHUL Physics PHYSTAT05 Glen Cowan Royal Holloway, University.
1 Beam e ’s from antineutrinos using the pME and LE beams David Jaffe, Pedro Ochoa December 8 th 2006  Part 1: Reminder and update  Part 2: Change in.
10. Unfolding ctd… K. Desch – Statistical methods of data analysis SS10.
Interjet Energy Flow at ZEUS. Patrick Ryan. Univ. of Wisconsin DPF, Aug. 27, Patrick Ryan University of Wisconsin Aug. 27, 2004 Interjet Energy.
November 1999Rick Field - Run 2 Workshop1 We are working on this! “Min-Bias” Physics: Jet Evolution & Event Shapes  Study the CDF “min-bias” data with.
Sung-Won Lee 1 Study of Jets Production Association with a Z boson in pp Collision at 7 and 8 TeV with the CMS Detector Kittikul Kovitanggoon Ph. D. Thesis.
Unfolding algorithms and tests using RooUnfold
Quark Compositeness Study and Progress Satyaki Bhattacharya, Sushil S. Chauhan, Brajesh C. Choudhary & Debajyoti Choudhury Department of Physics & Astrophysics.
CDF Joint Physics Group June 27, 2003 Rick FieldPage 1 PYTHIA Tune A versus Run 2 Data  Compare PYTHIA Tune A with Run 2 data on the “underlying event”.
1 2vtx tagged diBjets mass cross section measurement Univeristy of Notre Dame Hong Luo Mar 3 th 2005.
Unfolding jet multiplicity and leading jet p T spectra in jet production in association with W and Z Bosons Christos Lazaridis University of Wisconsin-Madison.
A measurement of the Ratio of Tree over Two Jet Cross Sections with CMS at 7TeV P.Kokkas, I.Papadopoulos, C.Fountas, I.Evangelou, N.Manthos University.
Progress on H/Abb -> 4b’s channel for the FTK physics case ~ 4jets Trigger w/ and w/o FTK ~ Kohei Yorita Young-Kee Kim University of the FTK.
Central Limit Theorem Example: (NOTE THAT THE ANSWER IS CORRECTED COMPARED TO NOTES5.PPT) –5 chemists independently synthesize a compound 1 time each.
RooUnfold unfolding framework and algorithms Tim Adye Rutherford Appleton Laboratory ATLAS RAL Physics Meeting 20 th May 2008.
Ratio of Three over Two Jet Cross Sections: Update 36 pb -1 P.Kokkas, I.Papadopoulos, C.Fountas University of Ioannina, Greece QCD High p T Meeting 17.
RooUnfold unfolding framework and algorithms Tim Adye Rutherford Appleton Laboratory Oxford ATLAS Group Meeting 13 th May 2008.
Run 2 Monte-Carlo Workshop April 20, 2001 Rick Field - Florida/CDFPage 1 The Underlying Event in Hard Scattering Processes  The underlying event in a.
Descriptive Statistics-IV (Measures of Variation)
Hadronic Event Shapes at 7 TeV with CMS Detector S,Banerjee, G. Majumdar, MG + ETH, Zurich CMS PAS QCD M. Guchait DAE-BRNS XIX High Energy Physics.
PHENO 2008 April 29th Tom Schwarz University of California Davis Measurement of the Forward-Backward Asymmetry In Top Production with 1.9 fb -1.
Sung-Won Lee 1 Study of Jets Production Association with a Z boson in pp Collision at 7 and 8 TeV with the CMS Detector Kittikul Kovitanggoon Ph. D. Thesis.
Unfolding in ALICE Jan Fiete Grosse-Oetringhaus, CERN for the ALICE collaboration PHYSTAT 2011 CERN, January 2011.
Update : Ratio of Three over Two Jet Cross Sections P.Kokkas, I.Papadopoulos, C.Fountas, I.Evangelou, N.Manthos University of Ioannina, Greece Senior Editor.
DIJET (and inclusive-jet) CROSS SECTIONS IN DIS AT HERA T. Schörner-Sadenius (for the ZEUS collaboration) Hamburg University DIS 06, April 2006 Tsukuba,
8th December 2004Tim Adye1 Proposal for a general-purpose unfolding framework in ROOT Tim Adye Rutherford Appleton Laboratory BaBar Statistics Working.
1 NCC Task Force Richard Seto NCC Task Force Meeting Jan 8, 2007 BNL.
22 January 2009 David1 Look at dead material and fake MET in Jx samples mc08 10 TeV simulations, release J0 to J6 are tag s479_r586, ‘ideal geometry’
G. Cowan CERN Academic Training 2012 / Statistics for HEP / Lecture 41 Statistics for HEP Lecture 4: Unfolding Academic Training Lectures CERN, 2–5 April,
QCD Background Estimation From Data Rob Duxfield, Dan Tovey University of Sheffield.
Charged Particle Multiplicity, Michele Rosin U. WisconsinQCD Meeting May 13, M. Rosin, D. Kçira, and A. Savin University of Wisconsin L. Shcheglova.
Measurement of the 3-jet to 2-jet Cross Sections Ratio in pp Collisions at 7TeV Update : Pythia8 tune 2C P.Kokkas, I.Papadopoulos, C.Fountas University.
1 The comparisons between with and without JES uncertainty. jet with pt > 30 GeV, |eta| 40. Jet Y is calculated by 0.5*log[(E+pz)/(E-pz)] CMS Data.
Update on Diffractive Dijets Hardeep Bansil University of Birmingham 12/07/2013.
A measurement of the Ratio of Three over Two Jet Cross Sections with CMS at 7TeV 70 nb -1 P.Kokkas, I.Papadopoulos, C.Fountas, I.Evangelou, N.Manthos University.
网上报账系统包括以下业务: 日常报销 差旅费报销 借款业务 1. 填写报销内容 2. 选择支付方式 (或冲销借款) 3. 提交预约单 4. 打印预约单并同分类粘 贴好的发票一起送至财务 处 预约报销步骤: 网上报账系统 薪酬发放管理系统 财务查询系统 1.
I'm concerned that the OS requirement for the signal is inefficient as the charge of the TeV scale leptons can be easily mis-assigned. As a result we do.
1 RA1 Analysis Exclusive n-jet + MET search Overview and Status Report Tanja Rommerskirchen on behalf of the RA1 group Universitaet Zuerich SUSY Workshop;
IC40 Spectrum Unfolding 7/1/2016Warren Huelsnitz1 SVD Method described in A. Höcker and V. Kartvelishvili, NIM A 372 (1996) 469NIM A 372 (1996) 469 Implemented.
1 Unfolding Study Closure test on SHERPA 08/16/12.
1 Unfolding Study Closure test on SHERPA 08/10/12.
Solving Linear Equations in Two VariablesProjector Resources Solving Linear Equations in Two Variables Projector Resources.
Update on Diffractive Dijets Analysis Hardeep Bansil University of Birmingham Soft QCD / Diffraction WG Meeting 27/01/2014.
Klaus Rabbertz Hamburg, Germany, Terascale Workshop Klaus Rabbertz, KIT 6. Physics at the Terascale Workshop, Hamburg, 2012 Determination.
Update on A FB Myfanwy Liles μ-μ- μ+μ+ q q θ*θ*. A FB Reminder  Forward-Backward Asymmetry  Due to parity violation of the weak interaction  Interference.
Linear Algebra Review.
Report Jet-veto SF and Uncertainties Jet smearing
Effect of t42 algorithm on jets
light jet energy scale from Wjj
CDS comments on supporting note
Measurement of the γ,W,Z with ATLAS for the ATLAS Collaboration
Tips Need to Consider When Organizing a College Event
Observation of Diffractively Produced W- and Z-Bosons
ماجستير إدارة المعارض من بريطانيا
The Big 6 Research Model Step 3: Location and Access
Rick Field – Florida/CDF/CMS
Observation of Diffractively Produced W- and Z-Bosons
½ of 6 = 3.
Booster prograss Code in Mathematica: from thin to thick. SVD and response matrix. Code for orbit correct is in progress.
C.2.10 Sample Questions.
W polarization and ttbar spin correlation study
C.2.8 Sample Questions.
Booster prograss Code in Mathematica: from thin to thick. SVD and response matrix. Code for orbit correct is in progress.
C.2.8 Sample Questions.
Types of Errors And Error Analysis.
A brief update on b-tagging of High P jets
Presentation transcript:

1 Unfolding Study 07/11/12

2 RooUnfold Using the RooUnfold In this study we make response matrix from MADGRAPH MC and use it to unfold the Pythia6 sample Plots we are interested are rapidity of Z and jet in Z+1jet events i.e. Yz, Yjet, different of Yz and Yjet, and sum of Yz and Yjet The unfolding methods are  Bayes with number of iteration = 4  Svd with ktern =15 (total number of bins) i.e. just inverts matrix  Bin by Bin

3 Response Matrix MADGRAPH

4 |Y of Z| BayesSvdBin by Bin The corrections for all 3 methods are small. The corrections are almost the same for all 3 methods.

5 |Y of jet| BayesSvdBin by Bin The corrections are small. The corrections are almost the same for all 3 methods.

6 0.5|Y z +Y jet | BayesSvdBin by Bin Y sum again shows the small and consistent corrections for all methods (except the last bin).

7 0.5|Y z -Y jet | BayesSvdBin by Bin Y diff shows the small corrections but not the last three bins. There big corrections in last two bin might be from low statistic (big errors).

8 Keng's Comments 1. By using MADGRAPH response matrix, the corrections for PYTHIA are small and consistent. 2. The correction also look the same for all methods. 3. The last three bins of Ydiif show big corrections. This may be from small statistic.