1 META PDFs as a framework for PDF4LHC combinations Jun Gao, Joey Huston, Pavel Nadolsky (presenter) arXiv:1401.0013, Parton.

Slides:



Advertisements
Similar presentations
Lara De Nardo BNL October 8, 2007 QCD fits to the g 1 world data and uncertainties THE HERMES EXPERIENCE QCD fits to the g 1 world data and uncertainties.
Advertisements

High Energy neutrino cross-sections HERA-LHC working week Oct 2007 A M Cooper-Sarkar, Oxford Updated predictions of high energy ν and ν CC cross-sections.
Low-x and PDF studies at LHC Sept 2008 A M Cooper-Sarkar, Oxford At the LHC high precision (SM and BSM) cross section predictions require precision Parton.
Structure of the Proton CTEQ Parton Distribution Functions CTEQ6.6 P. M. Nadolsky, H.-L. Lai, Q.-H. Cao, J. Huston, J. Pumplin, D. Stump, W.-K. Tung, C.-P.
Kriging.
PDF’s: Current status and issues PDF’s with uncertainties (Tuesday, 15:00 -17:00, TH-Auditorium) PDF’s with uncertainties (Tuesday, 15:00 -17:00, TH-Auditorium)
1 CT10, CT14 parton distributions and beyond Parton distributions for the LHC, Benasque, Pavel Nadolsky Southern Methodist University On behalf.
Data preprocessing before classification In Kennedy et al.: “Solving data mining problems”
Sept 2003PHYSTAT61 Uncertainties of Parton Distributions (II) Results.
October 2004CTEQ Meeting1 Parton distribution uncertainty and W and Z production at hadron colliders Dan Stump Department of Physics and Astronomy Michigan.
Sept 2003PHYSTAT41 Uncertainty Analysis (I) Methods.
May 2005CTEQ Summer School25 4/ Examples of PDF Uncertainty.
Road to CTEQ7 J. Huston CTEQ meeting. Roadmap CTEQ6 was published in 2002, followed by CTEQ6.1 in 2003 Pavel has given you a review of CTEQ6.6 which will.
May 2005CTEQ Summer School1 Uncertainties of Parton Distribution Functions Dan Stump Michigan State University.
H1/ZEUS fitters meeting Jan 15 th 2010 Am Cooper-Sarkar Mostly about fitting the combined F2c data New work on an FFN fit PLUS Comparing HERAPDF to Tevatron.
Top properties workshop 11/11/05 Some theoretical issues regarding Method 2 J. Huston Michigan State University.
Sept 2003PHYSTAT1 Uncertainties of Parton Distribution Functions Daniel Stump Michigan State University & CTEQ.
Sept 2003PHYSTAT41 Uncertainty Analysis (I) Methods.
G. Cowan Lectures on Statistical Data Analysis Lecture 10 page 1 Statistical Data Analysis: Lecture 10 1Probability, Bayes’ theorem 2Random variables and.
Radial Basis Function Networks
Preliminary results in collaboration with Pavel Nadolsky Les Houches /6/5.
1 Combination of PDF uncertainties for LHC observables Pavel Nadolsky (SMU) in collaboration with Jun Gao (Argonne), Joey Huston (MSU) Based on discussions.
PDF’s for the LHC: LHC cross section benchmarking and error prescriptions J. Huston Michigan State University MCTP Spring Symposium on Higgs Boson Physics.
880.P20 Winter 2006 Richard Kass 1 Confidence Intervals and Upper Limits Confidence intervals (CI) are related to confidence limits (CL). To calculate.
W/Z PRODUCTION AND PROPERTIES Anton Kapliy (University of Chicago) on behalf of the ATLAS collaboration PHENO-2012.
A Neural Network MonteCarlo approach to nucleon Form Factors parametrization Paris, ° CLAS12 Europen Workshop In collaboration with: A. Bacchetta.
Update on fits for 25/3/08 AM Cooper-Sarkar Central fit: choice of parametrization Central fit: choice of error treatment Quality of fit to data PDFs plus.
NNPDF Partons: Issues NNPDF2.1 Users Guide Reweighting RDB, Valerio Bertone, Francesco Cerutti, Luigi Del Debbio, Stefano Forte, Alberto Guffanti, Jose.
Research Seminars in IT in Education (MIT6003) Quantitative Educational Research Design 2 Dr Jacky Pow.
Possibility of tan  measurement with in CMS Majid Hashemi CERN, CMS IPM,Tehran,Iran QCD and Hadronic Interactions, March 2005, La Thuile, Italy.
Ronan McNulty EWWG A general methodology for updating PDF sets with LHC data Francesco de Lorenzi*, Ronan McNulty (University College Dublin)
Moving on to BSM physics Example of how PDF uncertainties matter for BSM physics– Tevatron jet data were originally taken as evidence for new physics--
ECE-7000: Nonlinear Dynamical Systems Overfitting and model costs Overfitting  The more free parameters a model has, the better it can be adapted.
An Introduction to Kalman Filtering by Arthur Pece
DIJET (and inclusive-jet) CROSS SECTIONS IN DIS AT HERA T. Schörner-Sadenius (for the ZEUS collaboration) Hamburg University DIS 06, April 2006 Tsukuba,
Precision Cross section measurements at LHC (CMS) Some remarks from the Binn workshop André Holzner IPP ETH Zürich DIS 2004 Štrbské Pleso Štrbské Pleso.
Status of Recent Parton Distribution Analyses Hung-Liang Lai Department of Science Education Taipei Municipal Teachers College Introduction Time evolution.
Discussion of calculation of LHC cross sections and PDF/  s uncertainties J. Huston Michigan State University 1.
Itamar Roth, Ehud Duchovni Group meeting 19/01/15 1.
MACHINE LEARNING 7. Dimensionality Reduction. Dimensionality of input Based on E Alpaydın 2004 Introduction to Machine Learning © The MIT Press (V1.1)
Further investigations on the fits to new data Jan 12 th 2009 A M Cooper-Sarkar Considering ONLY fits with Q 2 0 =1.9 or 2.0 –mostly comparing RTVFN to.
Treatment of correlated systematic errors PDF4LHC August 2009 A M Cooper-Sarkar Systematic differences combining ZEUS and H1 data  In a QCD fit  In a.
11 QCD analysis with determination of α S (M Z ) based on HERA inclusive and jet data: HERAPDF1.6 A M Cooper-Sarkar Low-x meeting June 3 rd 2011 What inclusive.
DIJET (and inclusive-jet) CROSS SECTIONS IN DIS AT HERA T. Schörner-Sadenius (for the ZEUS collaboration) Hamburg University DIS 06, April 2006 Tsukuba,
1 Heavy Flavour Content of the Proton Motivation Experimental Techniques charm and beauty cross sections in DIS for the H1 & ZEUS Collaborations Paul Thompson.
H1 QCD analysis of inclusive cross section data DIS 2004, Štrbské Pleso, Slovakia, April 2004 Benjamin Portheault LAL Orsay On behalf of the H1 Collaboration.
CT14 PDF update J. Huston* PDF4LHC meeting April 13, 2015 *for CTEQ-TEA group: S. Dulat, J. Gao, M. Guzzi, T.-J. Hou, J. Pumplin, C. Schmidt, D. Stump,
G. Cowan Lectures on Statistical Data Analysis Lecture 10 page 1 Statistical Data Analysis: Lecture 10 1Probability, Bayes’ theorem 2Random variables and.
H1 and ZEUS Combined PDF Fit DIS08 A M Cooper Sarkar on behalf of ZEUS and H1 HERA Structure Function Working Group NLO DGLAP PDF fit to the combined HERA.
D Parton Distribution Functions, Part 2. D CT10-NNLO Parton Distribution Functions.
LHC Higgs Cross Section Working Group: Vector Boson Fusion Sinead Farrington University of Oxford Co-contacts: A. Denner, C. Hackstein, D. Rebuzzi, C.
Uncertainty and confidence Although the sample mean,, is a unique number for any particular sample, if you pick a different sample you will probably get.
MSTW update James Stirling (with Alan Martin, Robert Thorne, Graeme Watt)
Drell-Yan Spectrum and PDFs Dimitri Bourilkov University of Florida Di-lepton Meeting, LPC, FNAL, October 2, 2008.
Moriond 2001Jets at the TeVatron1 QCD: Approaching True Precision or, Latest Jet Results from the TeVatron Experimental Details SubJets and Event Quantities.
Physics at the LHC M. Guchait DHEP Annual Meeting 7-8 th April, 2016.
1 Proton Structure Functions and HERA QCD Fit HERA+Experiments F 2 Charged Current+xF 3 HERA QCD Fit for the H1 and ZEUS Collaborations Andrew Mehta (Liverpool.
1 A M Cooper-Sarkar University of Oxford ICHEP 2014, Valencia.
Developments in PDF4LHC Developments in PDF4LHC Albert De Roeck CERN, Geneva, Switzerland Antwerp University Belgium UC-Davis California USA BUE, Cairo,
Parton Distributions and Higgs Production at the LHC and the Tevatron James Stirling Cambridge University introduction: overview and recent developments.
Diphoton+MET: Update on Plans and Progress
J. Huston Michigan State University for CTEQ-TEA PDF fitting group
Michigan State University
Principal Component Analysis (PCA)
HESSIAN vs OFFSET method
Filtering and State Estimation: Basic Concepts
Uncertainties of Parton Distributions
A. DJOUADI (Paris, Montpellier)
ATLAS 2.76 TeV inclusive jet measurement and its PDF impact A M Cooper-Sarkar PDF4LHC Durham Sep 26th 2012 In 2011, 0.20 pb-1 of data were taken at √s.
Heavy Flavour Content of the Proton
Presentation transcript:

1 META PDFs as a framework for PDF4LHC combinations Jun Gao, Joey Huston, Pavel Nadolsky (presenter) arXiv: , Parton distributions for the LHC, Benasque, , 2015

2 A meta-analysis compares and combines LHC predictions based on several PDF ensembles. It serves the same purpose as the PDF4LHC prescription. It combines the PDFs directly in space of PDF parameters. It can significantly reduce the number of error PDF sets needed for computing PDF uncertainties and PDF- induced correlations. Meta PDFs: a fit to PDF fits The number of input PDF ensembles that can be combined is almost unlimited What is the PDF meta-analysis?

PDF4LHC recommendation for combination of PDF uncertainties (M. Botje et al., (2011), arxiv: ; R. Ball et al., arXiv: )

Yes No 2015: A concept for a new PDF4LHC recommendation Is a reduced PDF4LHC PDF ensemble available for this observable? No Yes Choose: This procedure applies both at NLO and NNLO

Combination of the PDFs into the future PDF4LHC ensemble

6 1.Combination based on MC replicas (G. Watt, R. Thorne, ; R. Ball et al., ; S. Forte, G. Watt, ) Many Monte-Carlo PDF replicas are generated for each input ensemble The cross sections are still computed for each of many (>100) replicas and combined based on the probability distribution in the PDF space. The number of replicas grows with the number of input ensembles. Alternative to the 2010 PDF4LHC prescription

7 2. Reduction of MC replicas Starting from step 1, the number of input MC replicas is reduced to a much smaller number while preserving as much input information as possible Two reduction methods are being explored: 1. Meta-parametrizations + MC replicas + Hessian data set diagonalization (J. Gao, J. Huston, P. Nadolsky, , ; update by P.N.) 2. Compression of Monte-Carlo replicas (G. Watt, R. Thorne, ; R. Ball et al., ; S. Forte, G. Watt, ; update by S. Carrazza) The final combination prescription will probably retain the best features of both approaches. Alternative to the 2010 PDF4LHC prescription

8 1.Select the input PDF ensembles (CT, MSTW, NNPDF…) 2.Fit each PDF error set in the input ensembles by a common functional form (“ a meta-parametrization ”) 3.Generate many Monte-Carlo replicas from meta-parametrizations of each set to investigate the probability distribution on the ensemble of all meta- parametrizations (as in Thorne, Watt, ) 4.Construct a final ensemble of 68% c.l. Hessian eigenvector sets to propagate the PDF uncertainty from the combined ensemble of replicated meta- parametrizations into LHC predictions. META1.0 PDFs: A working example of a meta-analysis See arXiv: for details Only in the META set

9 The logic behind the META approach When expressed as the meta –parametrizations, PDF functions can be combined by averaging their meta- parameter values Standard error propagation is more feasible, e.g., to treat the meta-parameters as discrete data in the linear (Gaussian) approximation for small variations The Hessian analysis can be applied to the combination of all input ensembles in order to optimize uncertainties and eliminate “noise” Emphasize simplicity and intuition

10 META PDFs can be provided with asymmetric errors Although only symmetric META errors have been discussed so far, asymmetric Hessian errors can be also determined as in CTEQ analyses

11 Specific realization (META1.0) Take NNLO (or NLO) PDFs Choose a meta-parametrization of PDFs at initial scale of 8 GeV (away from thresholds) for 9 PDF flavors (66 parameters in total) Generate MC replicas for all 3 groups and merge with equal weights, finding meta parameters for each of the replicas by fitting PDFs in x ranges probed at LHC –PDF uncertainties for above three groups are all reasonably consistent with each other (see next slide) –can add other sets, perhaps with non-equal weights to take into account more limited data sets and thus larger uncertainties

12 Merging PDF ensembles Central value on g Standard deviation on g

13 Reduction of the error PDFs

14 General-purpose META PDF ensemble 50 eigenvectors (100 error sets) provide a very good representation of the PDF uncertainties for all of the 3 PDF error families above The META PDFs provide both an average of the chosen central PDFs, as well as a good estimation of the 68% c.l. total PDF uncertainty Can re-diagonalize the Hessian matrix to get 1 orthogonal eigenvector to get the  s uncertainty (H.-L. Lai et al., ) meta-PDF uncertainty band

15 PDFs for sea quarks

16 Reduced META ensemble Already the general-purpose ensemble reduced the number of error PDFs needed to describe the LHC physics; but we can further perform a data set diagonalization to pick out eigenvector directions important for Higgs physics or another class of LHC processes Select global set of Higgs cross sections at 8 and 14 TeV (46 observables in total; more can be easily added if there is motivation)

17 Some parton luminosities Plots are made with APFEL WEB (apfel.mi.infn.it; Carrazza et al., )

18 Data set diagonalization (Pumplin, ) There are 50 eigenvectors, but can rediagonalize the Hessian matrix to pick out directions important for the Higgs observables listed on previous page; with rotation of basis, 50 important eigenvectors become 6 J. Gao, J. Huston P. Nadolsky (in progress)

19 Higgs eigenvector set high y not included in original fit

20

21 Re-diagonalized eigenvectors…

22

23

24

25

26

27

28

29 A Mathematica package MP4LHC Includes all tools for the META analysis Will be public Includes all tools for the META analysis Will be public

30 To summarize, the meta-parametrization and Hessian method facilitate the combination of PDF ensembles even when the MC replicas are introduced at the intermediate stage Benefits of the meta-parametrization The PDF parameter space of all input ensembles is visualized explicitly. Data combination procedures familiar from PDG can be applied to each meta-PDF parameter

31 To summarize, the meta-parametrization and Hessian method facilitate the combination of PDF ensembles even when the MC replicas are introduced at the intermediate stage Benefits of the Hessian method It is very effective in data reduction, as it makes use of diagonalization of a semipositive-definite Hessian matrix in the Gaussian approximation. [The unweighting of MC replicas is both more detailed and nuanced.] Correlations between Higgs signals and backgrounds are reproduced with just 13 META PDFs. Asymmetric Hessian errors can be computed.

32 According to Joey, some of the discussion of META & CMC PDFs spilled into an episode of the Big Bang theory sitcom on January 29: 36D84D053DAC/the-big-bang-theory-the-anxiety-optimization

33

34 Even Leonard accepts some strengths of the Hessian formalism. We have a hope of reaching a consensus on the PDF combination methods soon!

35 Back-up slides 35

36 Meta-parameters of 5 sets and META PDFs 36