Preliminary T2K beam simulation using the G4 2km detector

Slides:



Advertisements
Similar presentations
CC Background Systematic 3 Philip Rodrigues Oxford Group Meeting 30/10/07.
Advertisements

Oscillation formalism
HARP Anselmo Cervera Villanueva University of Geneva (Switzerland) K2K Neutrino CH Meeting Neuchâtel, June 21-22, 2004.
Expected Sensitivity of the NO A  Disappearance Analysis Kirk Bays (Caltech) for the NO A Collaboration April 14, 2013 APS DPF Denver Kirk Bays, APS DPF.
Super-Kamiokande Introduction Contained events and upward muons Updated results Oscillation analysis with a 3D flux Multi-ring events  0 /  ratio 3 decay.
T2K neutrino experiment at JPARC Approved since 2003, first beam in April Priorities : 1. search for, and measurement of,   e appearance  sin.
M.Mevius Open and hidden beauty production in 920 GeV proton –nucleus collisions at HERA-B M.Mevius DESY.
Off-axis Simulations Peter Litchfield, Minnesota  What has been simulated?  Will the experiment work?  Can we choose a technology based on simulations?
Performance of a Water Cherenkov Detector for e Appearance Shoei NAKAYAMA (ICRR, University of Tokyo) November 18-19, 2005 International Workshop on a.
1 Measurement of f D + via D +   + Sheldon Stone, Syracuse University  D o D o, D o  K -  + K-K- K+K+ ++  K-K- K+K+ “I charm you, by my once-commended.
Status of  b Scan Jianchun Wang Syracuse University Representing L b scanners CLEO Meeting 05/11/02.
Background Understanding and Suppression in Very Long Baseline Neutrino Oscillation Experiments with Water Cherenkov Detector Chiaki Yanagisawa Stony Brook.
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.
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.
10/24/2005Zelimir Djurcic-PANIC05-Santa Fe Zelimir Djurcic Physics Department Columbia University Backgrounds in Backgrounds in neutrino appearance signal.
New results from K2K Makoto Yoshida (IPNS, KEK) for the K2K collaboration NuFACT02, July 4, 2002 London, UK.
Expected Sensitivity of the NO A  Disappearance Analysis Kirk Bays (Caltech) for the NO A Collaboration April 14, 2013 APS DPF Denver Kirk Bays, APS DPF.
Preliminary Study of CC-Inclusive Events in the P0D using Global Reconstruction Rajarshi Das (w/ Walter Toki) Nu-Mu Prelim. Meeting Dec 2010 CSU.
Apr. 4, KEK JHF-SK neutrino workshop 1 e appearance search Yoshihisa OBAYASHI (KEK - IPNS)
Dec. 13, 2001Yoshihisa OBAYASHI, Neutrino and Anti-Neutrino Cross Sections and CP Phase Measurement Yoshihisa OBAYASHI (KEK-IPNS) NuInt01,
Yoshihisa OBAYASHI, Oct. Neutrino Oscillation Experiment between JHF – Super-Kamiokande Yoshihisa OBAYASHI (Kamioka Observatory, ICRR)
Feb. 7, 2007First GLAST symposium1 Measuring the PSF and the energy resolution with the GLAST-LAT Calibration Unit Ph. Bruel on behalf of the beam test.
Search for Electron Neutrino Appearance in MINOS Mhair Orchanian California Institute of Technology On behalf of the MINOS Collaboration DPF 2011 Meeting.
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.
April 26, McGrew 1 Goals of the Near Detector Complex at T2K Clark McGrew Stony Brook University Road Map The Requirements The Technique.
1 Performance of a Magnetised Scintillating Detector for a Neutrino Factory Scoping Study Meeting U.C. Irvine Monday 21 st August 2006 M. Ellis & A. Bross.
1 A study to clarify important systematic errors A.K.Ichikawa, Kyoto univ. We have just started not to be in a time blind with construction works. Activity.
Search for active neutrino disappearance using neutral-current interactions in the MINOS long-baseline experiment 2008/07/31 Tomonori Kusano Tohoku University.
Measuring Oscillation Parameters Four different Hadron Production models  Four predicted Far  CC spectrum.
September 10, 2002M. Fechner1 Energy reconstruction in quasi elastic events unfolding physics and detector effects M. Fechner, Ecole Normale Supérieure.
PAC questions and Simulations Peter Litchfield, August 27 th Extent to which MIPP/MINER A can help estimate far detector backgrounds by extrapolation.
MIND Systematic Errors EuroNu Meeting, RAL 18 January 2010 Paul Soler.
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.
Mark Dorman UCL/RAL MINOS WITW June 05 An Update on Using QE Events to Estimate the Neutrino Flux and Some Preliminary Data/MC Comparisons for a QE Enriched.
A Measurement of the Ultra-High Energy Cosmic Ray Spectrum with the HiRes FADC Detector (HiRes-2) Andreas Zech (for the HiRes Collaboration) Rutgers University.
T2K Oscillation Strategies Kevin McFarland (University of Rochester) on behalf of the T2K Collaboration Neutrino Factories 2010 October 24 th 2010.
NNN 2011: The d Experiment Joshua Albert Duke University For the T2K Collaboration November 8, 2011.
The XXII International Conference on Neutrino Physics and Astrophysics in Santa Fe, New Mexico, June 13-19, 2006 The T2K 2KM Water Cherenkov Detector M.
R. Tayloe, Indiana U. DNP06 1 A Search for  → e oscillations with MiniBooNE MiniBooNE does not yet have a result for the  → e oscillation search. The.
Systematics Sanghoon Jeon.
Neutral Current Interactions in MINOS Alexandre Sousa, University of Oxford for the MINOS Collaboration Neutrino Events in MINOS Neutrino interactions.
T2K : New physics results
Neutrino factory near detector simulation
J. Musser for the MINOS Collatoration 2002 FNAL Users Meeting
P0D reconstruction/analysis update
Tracking(1) Kp2 decay-in-flight BG simulation
Wrong sign muons detection in a
L/E analysis of the atmospheric neutrino data from Super-Kamiokande
Status of the OPERA experiment
Update of the Fiducial calibration study in 2km WC detector
Background study : muons from the upstream rock
Neutrino Oscillation Physics with a Neutrino Factory
 Results from KTeV Introduction The KTeV Detector
Yoshihisa OBAYASHI (KEK - IPNS)
Prospects of J-PARC Neutrino Program
Jaewon Park University of Rochester
T2KK sensitivity as a function of L and Dm2
Claudio Bogazzi * - NIKHEF Amsterdam ICRC 2011 – Beijing 13/08/2011
Naotoshi Okamura (YITP) NuFact05
Neutrino interaction measurements in K2K SciBar
Toward realistic evaluation of the T2KK physics potential
Impact of neutrino interaction uncertainties in T2K
J/Y Simulations for Trigger
Conventional Neutrino Beam Experiment : JHF – Super-Kamiokande
L/E analysis of the atmospheric neutrino data from Super-Kamiokande
Presentation transcript:

Preliminary T2K beam simulation using the G4 2km detector Maximilien Fechner In collaboration with C. Walter Status of the 2km simulator Performance of the 2km 8inch simulation + reconstruction Preliminary background estimation @ SK

Status of the GEANT4 simulator 1KT MODE Charge scale tuning with through-going muon K2K-1KT data Energy scale : comparison with K2K-1KT data Using k2k02a ( not 03b) in order to be consistent with the data

Event reconstruction 1KT MODE Vertex resolution : s = 24cm Direction resolution = 2.7°

Energy scale Without any tuning of the pe->MeV tables (ptasmo…) G4 : 141.5 ± 1.5 MeV/c² Data (2000-2001) : 148.1 ± 0.5 MeV/c² Without any tuning of the pe->MeV tables (ptasmo…)

Known problems See previous talks… PID : shifted towards negative values for µ events Can probably be explained because of the excess of indirect light also present in the thrumu simulation data

PID for 2 ring events First ring Second ring The efficiencies are different for the first ring  Differences in the reconstructed pi0 mass

T2K beam event simulation 2km det with 8 inch tubes, ‘old’ setting : length = 16m, 6160 tubes) NEUT 4.5.1 vectors, 2.5° off-axis, 40 GeV protons ( ‘04b’) Processed with k2k02a-special8inch : Geometrical changes only (RPMT=10.0, etc.) No tuning of the pe->MeV tables No optimization of the ring counting & PID cuts e/p0 separation using polfit5 : expected light library not tuned to the 8’’ configuration

Statistics ~45000 nm ~45000 ne With |R| < 300m, -400<Z<600m (‘FV +1m’)

Vertex reconstruction NUE EVENTS NUMU EVENTS Long tail for multi-ring events

Direction reconstruction NUMU : error = 1.9° NUE : error = 3.6°

Energy scale NUMU : energy = 170 MeV/c² NUE : 166 MeV/c²

Ring counting NUMU nue Need tuning ?

PID NUMU NUE Conclusion : k2k02a-8inch needs to be tuned to the MC output

Nue appearance analysis Standard cuts : polfit5 pi0 cuts : fully contained in FV (100.5t), visible energy > 100 MeV Single-ring E- PID 0.35 < rec. En < 0.85 GeV Differences with SK : decay e- are not tagged  less efficient Cosqne < 0.9 Pi0mass < 100 MeV && likelihood difference < 150.0

PI0 plots Numu, nue

Efficiencies (1year) nm CC nm NC Beam ne FC,FV,evis>100 200224 29866 3159 1R 162993 17764 2168 e-like 18219 10605 1971 0.35 < Enrec<0.85 (GeV) 2787 3648 393 pi0 cuts (polfit5) 1536.8 (0.7%) 271.2 (0.9%) 266 (8.4%) At SK (polfit2) : 0.03% 1% 7%

Nue BG @ 2km (1year) Reconstructed nue energy (MeV) nue, numu, total

Prediction @ SK Using flat F/N ratio Using MC true info : oscillate the CC nm, not the NC nm nor the beam ne Taking into account the efficiency differences between SK & 2km Sin²2q13 = 1.0, Dm² = 2.5 eV² From the SK study : 23 BG expected for 5years

Expectation @ SK Total : ~30 events with 0.4 < E < 0.9 GeV Comparable with SK MC expectation

Conclusion simulation of T2K events @ 2km  ne BG rough estimation @ SK (using MC true) : ~30 BG events (sin²2q13=0.1,Dm²=2.5eV²) Todo list for the 2km nue study : Change the geometry (shorter tank) Tune the reconstruction software to G4 Decay e- cut in the G4 simulator Improve the expected light pattern tuning for polfit5 Apply polfit5 to monoenergetic & JPARC MC @ SK (in progress)

Extra slides

BLUE = nue, BLACK = numu