1 CC analysis update Status of the cross-section reweighting package Status of the Physics Analysis Ntuple (PAN) D. A. Petyt Nov 3 rd 2004.

Slides:



Advertisements
Similar presentations
Update on Data / MC Comparisons for Low Hadronic Energy CC-like Events Reminder of problem Fiducial studies with more MC statistics Effect of offset in.
Advertisements

1 Cross-section systematics Broad aims of this study: –Evaluate the effect of cross-section uncertainties on the all-event CC analysis (selection efficiencies,
N. Saoulidou Fermilab 1 Update on track reconstruction in the Near Detector N. Saoulidou, Fermilab
MINERvA Overview MINERvA is studying neutrino interactions in unprecedented detail on a variety of different nuclei Low Energy (LE) Beam Goals: – Study.
Elisabeth Falk Harris University of Sussex On behalf of the MINOS Collaboration SNOW 2006, Stockholm, 2-6 May 2006 First MINOS Results from the NuMI Beam.
Emily Thompson May 5 – UMass HEP Exp Group Meeting 1 Tag-probe method: Fitting Z → μ + μ - mass peaks Motivation: 1. Want to use long p T tail of muon.
Off-axis Simulations Peter Litchfield, Minnesota  What has been simulated?  Will the experiment work?  Can we choose a technology based on simulations?
1 N. Davidson E/p single hadron energy scale check with minimum bias events Jet Note 8 Meeting 15 th May 2007.
CC analysis progress This talk: –A first attempt at calculating CC energy sensitivity using the Far Mock data MC files with full reconstruction. –Quite.
MINOS Feb Antineutrino running Pedro Ochoa Caltech.
Top Turns Ten March 2 nd, Measurement of the Top Quark Mass The Low Bias Template Method using Lepton + jets events Kevin Black, Meenakshi Narain.
Update on NC/CC separation At the previous phone meeting I presented a method to separate NC/CC using simple cuts on reconstructed quantities available.
F.Sanchez (UAB/IFAE)ISS Meeting, Detector Parallel Meeting. Jan 2006 Low Energy Neutrino Interactions & Near Detectors F.Sánchez Universitat Autònoma de.
1 First look at new MC files First look at reconstruction output from the newly- generated “mock-data” MC files. –These contain the following improvements:
1 CC Update Status of the PAN –Integration of “standard” all-event analysis with Mad Analysis update –Resolving parameter degeneracies in the ND –To do.
2015/6/23 1 How to Extrapolate a Neutrino Spectrum to a Far Detector Alfons Weber (Oxford/RAL) NF International Scoping Study, RAL 27 th April 2006.
Event Reweighting Tools Contents: ● Goals ● Reweighting Packages ● Usage & Reweight Friendly Packages ● Validation ● Caveats.
1 CC update –  momentum resolution Software news: –Converted code to read Sue’s ntuples. Allows use of Chris’s analysis framework (including event display)
CC/NC SEPARATION STUDY Andy Blake Cambridge University Friday February 23 rd 2007.
1 CC analysis update New analysis of SK atm. data –Somewhat lower best-fit value of  m 2 –Implications for CC analysis – 5 year plan plots revisited Effect.
FD event selection and data/MC comparisons Motivation of this study –Look at FD events (with blinding scheme imposed) to determine Whether we observe neutrino.
1 MDC post-mortem Now that we know most (if not all) of the input MDC parameters, I thought it would be useful to conduct a post- mortem of the CC MDC.
Neutrino Event Reconstruction Andy Blake Cambridge University September 2003.
1 MDC status Overall concept: –The FarDet Mock data challenge ‘dataset’ has been generated with unknown values of  m 2 and sin 2 2  which are to be determined.
1 CC analysis update Repeat of CC analysis with R1.9 ntuples –What is the effect of improved tracking efficiency? Alternative PID methods: likelihood vs.
Far Detector Fiducial Volume Study Andy Blake Cambridge University Thursday December 7 th 2006.
1/16 MDC post-mortem redux Status as of last CC meeting: –True values of cross-section and oscillation parameters were used to reweight the ND and FD MC.
Identification of neutrino oscillations in the MINOS detector Daniel Cole
CC ANALYSIS STUDIES Andy Blake Cambridge University Fermilab, September 2006.
Status of the OPERA experiment Yoshiaki Nonoyama Nagoya Univ.
T-CHANNEL MODELING UNCERTAINTIES AND FURTHER QUESTIONS TO TH AND NEW FIDUCIAL MEASUREMENTS Julien Donini, Jose E. Garcia, Dominic Hirschbuehl, Luca Lista,
Atmospheric Neutrino Oscillations in Soudan 2
P. Vahle, Fermilab Oct An Alternate Approach to the CC Measurement— Predicting the FD Spectrum Patricia Vahle University College London Fermilab.
1 ZH Analysis Yambazi Banda, Tomas Lastovicka Oxford SiD Collaboration Meeting
Monte Carlo Comparison of RPCs and Liquid Scintillator R. Ray 5/14/04  RPCs with 1-dimensional readout (generated by RR) and liquid scintillator with.
Status report from T2K-SK group Task list of this group discussion about NEUT Kaneyuki, Walter, Konaka We have just started the discussion.
1 CC analysis – systematic errors At the last collaboration meeting it was recognised that we needed to develop tools to enable us to properly assess the.
Detector Monte-Carlo ● Goal: Develop software tools to: – Model detector performance – Study background issues – Calculate event rates – Determine feasibility.
Search for Electron Neutrino Appearance in MINOS Mhair Orchanian California Institute of Technology On behalf of the MINOS Collaboration DPF 2011 Meeting.
1 Mike Kordosky – NuFact 06 - Aug 27, 2006 Neutrino Interactions in the MINOS Near Detector Mike Kordosky University College London on behalf of the MINOS.
1 Physics Requirements on Reconstruction and Simulation Software Jorge G. Morfín - Fermilab.
First Look at Data and MC Comparisons for Cedar and Birch ● Comparisons of physics quantities for CC events with permutations of Cedar, Birch, Data and.
N. Saoulidou, Fermilab, MINOS Collaboration Meeting N. Saoulidou, Fermilab, ND/CC Parallel Session, MINOS Collaboration Meeting R1.18.
Cedar and pre-Daikon Validation ● CC PID parameter based CC sample selections with Birch, Cedar, Carrot and pre-Daikon. ● Cedar validation for use with.
P. Vahle, Oxford Jan F/N Ratio and the Effect of Systematics on the 1e20 POT CC Analysis J. Thomas, P. Vahle University College London Feburary.
Beam Extrapolation Fit Peter Litchfield  An update on the method I described at the September meeting  Objective;  To fit all data, nc and cc combined,
A bin-free Extended Maximum Likelihood Fit + Feldman-Cousins error analysis Peter Litchfield  A bin free Extended Maximum Likelihood method of fitting.
Mark Dorman UCL/RAL MINOS Collaboration Meeting Fermilab, Oct. 05 Data/MC Comparisons and Estimating the ND Flux with QE Events ● Update on QE event selection.
Study of the ND Data/MC for the CC analysis October 14, 2005 MINOS collaboration meeting M.Ishitsuka Indiana University.
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.
April 26, McGrew 1 Goals of the Near Detector Complex at T2K Clark McGrew Stony Brook University Road Map The Requirements The Technique.
Progress Report on GEANT Study of Containerized Detectors R. Ray 7/11/03 What’s New Since Last Time?  More detailed container description in GEANT o Slightly.
A different cc/nc oscillation analysis Peter Litchfield  The Idea:  Translate near detector events to the far detector event-by-event, incorporating.
Update on my oscillation analysis Reconstructed Near detector data event Reconstructed Near detector MC event Truth Near detector MC event Truth Far detector.
MINOS Coll Meet. Oxford, Jan CC/NC Data Cross Checks Thomas Osiecki University of Texas at Austin.
Search for active neutrino disappearance using neutral-current interactions in the MINOS long-baseline experiment 2008/07/31 Tomonori Kusano Tohoku University.
NUMI NUMI/MINOS Status J. Musser for the MINOS Collatoration 2002 FNAL Users Meeting.
Status of QEL Analysis ● QEL-like Event Selection and Sample ● ND Flux Extraction ● Fitting for MINOS Collaboration Meeting FNAL, 7 th -10 th December.
Measuring Oscillation Parameters Four different Hadron Production models  Four predicted Far  CC spectrum.
PAC questions and Simulations Peter Litchfield, August 27 th Extent to which MIPP/MINER A can help estimate far detector backgrounds by extrapolation.
Extrapolation Techniques  Four different techniques have been used to extrapolate near detector data to the far detector to predict the neutrino energy.
MIND Systematic Errors EuroNu Meeting, RAL 18 January 2010 Paul Soler.
Neutrino Oscillation Results from MINOS Alexandre Sousa Oxford University (for the MINOS Collaboration) 30 th International Cosmic Ray Conference - ICRC.
Observation Gamma rays from neutral current quasi-elastic in the T2K experiment Huang Kunxian for half of T2K collaboration Mar. 24, Univ.
 CC QE results from the NOvA prototype detector Jarek Nowak and Minerba Betancourt.
MINERνA Overview  MINERνA is studying neutrino interactions in unprecedented detail on a variety of different nuclei  Low Energy (LE) Beam Goals: t Study.
Measuring Nuclear Effects with MINERnA APS April Meeting 2011 G. Arturo Fiorentini Centro Brasileiro de Pesquisas Físicas On behalf of the MINERnA collaboration.
Neutral Current Interactions in MINOS Alexandre Sousa, University of Oxford for the MINOS Collaboration Neutrino Events in MINOS Neutrino interactions.
A PID based approach for antineutrino selection
Impact of neutrino interaction uncertainties in T2K
Presentation transcript:

1 CC analysis update Status of the cross-section reweighting package Status of the Physics Analysis Ntuple (PAN) D. A. Petyt Nov 3 rd 2004

2 Cross-section reweighting package A working version of this package now exists (thanks to Chris Smith and Hugh Gallagher) –The package provides an interface to NEUGEN and allows the user to calculate a weight for a particular GMINOS event given a tweaked set of NEUGEN input parameters. –The parameters are: M A for quasi-elastic scattering M A for resonance production DIS/Resonance scaling factors (8 parameters – 2 multiplicities, 4 initial states) Parton distribution functions (from PDFLIB) –This package will enable us to assess the effect of cross-section uncertainties on the CC analysis It is also required for the completion of the Mock Data Challenge –The code is still under development, but should be available for general use soon. The source code currently lives in the Contrib area of the minossoft CVS repository under Contrib/cbs/NeugenInterface

3 Cross-section reweighting function The weighting function has the following form: Double_t reweight( Float_t E_nu, Kinematic_variable_t::kv1, Float_t val1, Kinematic_variable_t::kv2, Float_t val2, Interaction I, process_t::proc neugen_config newconfig neugen_config oldconfig ) Neutrino energy Kinematic variables (x,y,q 2 or W) relevant to this interaction and their values Includes: flavour, nucleus (A,Z), CC or NC, initial state ( p, n, N …) QEL, RES, DIS, COH  These objects hold the values of the neugen config parameters (m A etc). The event weight is calculated based on these two sets of quantities

4 The Physics Analysis Ntuple (PAN) A simple ROOT ntuple that contains “all relevant quantities” for the CC analysis. –Truth information for MC events, including sufficient information to permit event reweighting (i.e. need at minimum E_nu, x, y, q 2, W, E_mu, limited STDHEP information). Can be extended to accommodate other reweighting functions as required. –Reconstructed information necessary to perform oscillation fit –Quantities specific to the CC analysis, such as PID parameters and fiducial cuts, that enable CC-like events to be selected –Association of tracks/showers/slices in the Near Detector. Identical format for ND and FD events An initial version of the PAN now exists with the quantities necessary for cross-section reweighting. A sample PAN for the far detector can be downloaded from the following website: – Ed Lartey has provided code to produce a PAN object from within the Mad analysis framework

5 PAN variables - 1 Variable Description true_enutrue neutrino energy (GeV) true_pmu true muon momentum (GeV/c) true_ehad true hadron energy (GeV) true_mudircos true muon z-direction cosine cc_nc cc/nc flag: 1-cc 2-nc flavour true flavour: 1-e 2-mu 3-tau process process: 1001-QEL 1002-RES 1003-DIS 1004-COH true_x true x true_ytrue y true_q2true q^2 true_wtrue w initial_state initial state: 1-vp 2-vn 3-vbarp 4-vbarn... nucleus target nucleus: 274-C 284-O 372-Fe run_num run number snarl snarl number evt_index event index within snarl mc_index mc index for this event numevt number of events/snarl numtrk number of tracks numshw number of showers evtvtx event vertex x-coord (m) Required for cross-section reweighting

6 PAN variables - 2 evtvty event vertex y-coord (m) evtvtz event vertex z-coord (m) is_fid vertex fiducial volume flag: 0-fail 1-pass is_cev containment flag: 1-CEV 2-PCE trkpass track quality flag: 0-fail 1-pass evlength event length (planes) trklength track length (planes) trkrange track momentum range (GeV/c) trkqp track momentum q/p trkeqp error on fitted q/p trkdircos track z-direction cosine shwph summed shower pulse height (shw.ph.gev) reco_pmu reconstructed muon momentum (GeV/c) (range or q/p) reco_eshw reconstructed shower energy (shw.ph.gev/1.23) reco_enu reconstructed neutrino energy (GeV) phfrac track pulse height fraction (uses sigcor) phplane track pulse height per plane ( " " ) pid1 pid parameter - Super-K definition pid2 pid parameter (probmu/(probmu+probnc)) neural neural network output is_cc cc-like flag: 0-nc-like 1-cc-like The only cut required to select cc-like events

7 Reweighting FarDet events – a simple example QEL: change ma_qel from 1.01 to 1.1 GeV RES: change ma_res from 0.95 to 1.05 GeV DIS: multiply DIS/RES matching scale factors by 0.75

8 PID variable by process All events QEL NC DIS RES is_cc=1 cut applied

9 Effect of weighting Pid parameter unweighted weighted

10 Near/far comparison – change m A by  10% nominal m A -10% m A +10%

11 Far/near ratio Effect largely cancels out in far/near ratio