  (tau neutrino magnetic moment) Reinhard Schwienhorst University of Minnesota Donut analysis Talk at Nagoya University, 6/9/99.

Slides:



Advertisements
Similar presentations
Monte Carlo Simulation of DY signal using standard Compass software: very preliminary results M. Chiosso Drell –Yan meeting, Dubna, 14/12/2006.
Advertisements

Monte Carlo simulation of the background for the Drell-Yan COMPASS Marialaura Colantoni Laboratory of Nuclear Problems Dubna Marialaura.
New results from the CHORUS Neutrino Oscillation Experiment Pasquale Migliozzi CERN XXIX International Conference on High Energy Physics UBC, Vancouver,
1 Deep Sea Neutrino Telescope Detection Principle.
1 N. Davidson E/p single hadron energy scale check with minimum bias events Jet Note 8 Meeting 15 th May 2007.
Radiative B Decays (an Experimental Overview) E.H. Thorndike University of Rochester CLEO Collaboration FPCP May 18, 2002.
The Matrix Method Data-driven method of estimating the W→lv and QCD multijet contributions to sample S’.
M. Kowalski Search for Neutrino-Induced Cascades in AMANDA II Marek Kowalski DESY-Zeuthen Workshop on Ultra High Energy Neutrino Telescopes Chiba,
A. Dabrowski, October Ratio(ke3/pipi0); Ratio(kmu3/pipi0) 1 Comments Γ(Ke3) / Γ(pipi0) Γ(Kmu3) / Γ(pipi0) Γ(Kmu3) / Γ(ke3) Anne Dabrowski Northwestern.
Reconstruction of neutrino interactions in PEANUT in general scanning (unbiased) mode Giovanni De Lellis on behalf of Andrea Russo Naples University.
1 Analysis code for KEK Test-Beam M. Ellis Daresbury Tracker Meeting 30 th August 2005.
Atmospheric Neutrino Event Reconstruction Andy Blake Cambridge University September 2003.
MUON FLUX MEASUREMENTS AT THE LSC JRA1-N2 Meeting, Zaragoza, Nov 23 rd 2007 Héctor Gómez Maluenda, University of Zaragoza.
Neutrino Event Reconstruction Andy Blake Cambridge University September 2003.
Interaction point analysis Judgment  /  March 10, 2009 Yoshiaki Nonoyama Nagoya Univ.
1 Monte Carlo methods Mike Sinclair. 2 Overview Monte Carlo –Based on roulette wheel probabilities –Used to describe large-scale interactions in biology.
1 The momentum measurement of 2ry particle emitted from neutrino interaction DONUT DEC 10 th -11 th B.D.Park, S.Takahashi and T.Furukawa.
1 Momentum measurements of 2ry particles emitted from neutrino interactions in DONuT experiment B. D. Park Nagoya univ. Emulsion Dec.
Measurement of the Branching fraction B( B  D* l ) C. Borean, G. Della Ricca G. De Nardo, D. Monorchio M. Rotondo Riunione Gruppo I – Napoli 19 Dicembre.
Statistical Analysis of Systematic Errors and Small Signals Reinhard Schwienhorst University of Minnesota 10/26/99.
DONUT Reinhard Schwienhorst DOE review 7/28/1999.
A long baseline neutrino oscillation search - MINOS Reinhard Schwienhorst School of Physics and Astronomy University of Minnesota.
14 July 2004University of Hawaii Physics Seminar New Nu’s from the DONUT Experiment Emily Maher University of Minnesota.
Probabilistic Mechanism Analysis. Outline Uncertainty in mechanisms Why consider uncertainty Basics of uncertainty Probabilistic mechanism analysis Examples.
IEEE 64 th ECTC – Orlando, FL, USA May 27–30, 2014 Add Company Logo Here.
EPECUR – Investigation of narrow baryon resonances Konovalova Elena St. Petersburg Nuclear Physics Institute (PNPI) with collaboration Institute of Theoretical.
N. Saoulidou & G. Tzanakos1 Event Location N. Saoulidou and G. Tzanakos University of Athens, Department of Physics, Div. Of Nuclear & Particle Physics.
Par: Grace McNamara MONTE CARLO, MONACO.
Z boson mass reconstruction Caroline Steiblin Prof. Al Goshaw Dr. Andrea Bocci Duke University 1.
National Taiwan University PEAKASO: Peak-Temperature Aware Scan- Vector Optimization Minsik Cho and David Z. Pan Dept. of ECE The University of Texas at.
Physics Colloquium-28 November 2001 “The Neutrino Oscillation Industry”Maury Goodman, Argonne National Lab Outline  Neutrino History   Oscillations.
DONUT - Observation of  Interactions Reinhard Schwienhorst University of Minnesota The DONUT collaboration: Aichi University, Kobe University, Nagoya.
Machine Design Under Uncertainty. Outline Uncertainty in mechanical components Why consider uncertainty Basics of uncertainty Uncertainty analysis for.
Measuring the Spin Structure of 3 He and the Neutron at Low Q 2 Timothy Holmstrom College of William and Mary For the Jefferson Lab Hall A Collaboration.
Elastic Electron Scattering off He and He at Large Momentum Transfers Elena Khrosinkova Kent State University Hall A Collaboration Meeting Jefferson Lab.
JPS 2003 in Sendai Measurement of spectral function in the decay 1. Motivation ~ Muon Anomalous Magnetic Moment ~ 2. Event selection 3. mass.
The DONuT Experiment Observations of the Tau Neutrino Presentation by Suzanne Nichols.
Susan Burke DØ/University of Arizona DPF 2006 Measurement of the top pair production cross section at DØ using dilepton and lepton + track events Susan.
Search for diffuse cosmic neutrino fluxes with the ANTARES detector Vladimir Kulikovskiy The ANTARES Collaboration 3-9 August 2014ANTARES diffuse flux.
Single-spin asymmetry in interference fragmentation on a transversely polarized hydrogen target at HERMES Tomohiro Kobayashi Tokyo Institute of Technology.
The development of the story
PREWRITE: STEP 1: Graphic Organizer Describes who the person is Personality Characteristics.
14 July 2004University of Hawaii Physics Seminar New Nu’s from the DONUT Experiment Emily Maher University of Minnesota.
The Personal Narrative Writing about a small moment in your life.
Aug _5071 Top stop by charm channel analysis using D0 runI data OUTLINE physics process of top to stop Monte Carlo simulation for signal data.
A New Upper Limit for the Tau-Neutrino Magnetic Moment Reinhard Schwienhorst      ee ee
1 Reinhard Schwienhorst, MSU Top Group Meeting W' Search in the single top quark channel Reinhard Schwienhorst Michigan State University Top Group Meeting,
Proposal Preparation. Documents for June PAC  Full Proposal  Starting point is LOI + updates in EOI  Project Definition Report  Cost estimate  Excel-based.
Comparison of reconstruction strategies in IceCube Lake Geneva, April 2007.
Pythia simulations of multijet events in proton-proton collisions at 7 TeV centre-of-mass energy. Angelika Fertig University of Cambridge Supervisor: Klaus.
Introduction Intro Problem Materials Hypothesis Procedure Results
Gamma Ray Constraints on New Physics Interpretations of IceCube Data
γ γ-> hadron Background Events at CLIC
Estimating the SuperB experimental reach on (g-2)t
Tips Need to Consider When Organizing a College Event
Validation Plots from the Mainland ANITA Simulation
مبررات إدخال الحاسوب في رياض الأطفال
NUCLEUS-NUCLEUS COLLISION Centrality Determination For NICA/MPD
ماجستير إدارة المعارض من بريطانيا
Subhayu Basu et al. , DNA8, (2002) MEC Seminar Su Dong Kim
Application of neutron monitor data for assessment of aircrew exposure
21twelveinteractive.com/ twitter.com/21twelveI/ facebook.com/21twelveinteractive/ linkedin.com/company/21twelve-interactive/ pinterest.com/21twelveinteractive/
Event Shape Variables in Deep Inelastic Scattering at HERA
The gluon polarisation ΔG/G at COMPASS
(your title) arXiv:xxxx.xxxx [hep-ex]
NuTel Video Conference 6/13/2003 M.A. Huang
Title Introduction: Discussion & Conclusion: Methods & Results:
(max 5 slides and 5 minutes) (-5 point for each extra slide or minute)
RITESH KUMAR LENKA REGD NO: BRANCH: EIE 7th SEMESTER
Title Firstname Lastname 1, Firstname Lastname 2 and Firstname Lastname 3 1 Affiliations. Dummy text, dummy text, dummy text 2 Affiliations. Dummy text,
Presentation transcript:

  (tau neutrino magnetic moment) Reinhard Schwienhorst University of Minnesota Donut analysis Talk at Nagoya University, 6/9/99

Outline Introduction Physics –magnetic moment interaction –Expected event yield Spectrometer analysis: –Monte Carlo Analysis –Cuts Preliminary Physics result Conclusions All of the numbers in this presentation are preliminary

Introduction Standard Model –  =0 current experimental limit: – e :  <1.8   B –  :  <7.4   B –  :  <5.4   B (all obtained in neutrino-electron scattering experiments)

Magnetic moment interaction      ee ee

Magnetic moment interaction example (MC)

Physics reminder Neutrino-electron scattering –no hadronic activity in the event –small forward angle  magnetic moment interaction –cross section  : neutrino magnetic moment E : neutrino energy T: electron kinetic energy

Electron energy and angle Production angle and energy for the electron in a magnetic moment interaction

Expected event yield If  =5.4   B (the current limit): –with an electron energy cutoff at 5GeV current cat3 neutrino event sample expect  10  magnetic moment interactions (compared to  40  CC interaction) –with an electron energy cutoff at 0.5GeV.nustrip files expect  30  magnetic moment interactions –with an electron energy cutoff at 10MeV emulsion analysis expect  80  magnetic moment interactions we must scan at least 1/3 of the emulsion to improve the sensitivity

Emulsion-only analysis Scan a large volume of the emulsion Search for single electron tracks in the direction of the beam –challenges: identify electrons down to very low energies many straight tracks in the emulsion Advantage: independent of the spectrometer, time, trigger disadvantages: –must scan a large volume –background from pair production

Spectrometer analysis outline Optimize cuts for magnetic moment events –cross-check with  CC events (data and MC) easy to find ® determine efficiency apply to neutrino candidate events –apply first to MC events, determine expected # of events –blind analysis apply to nustrip files – find (almost) all candidate events – not quite a blind analysis at the end, scan emulsion for confirmation –identify hadrons, decays, secondary interactions, nuclear breakup

Monte Carlo analysis So far only periods 3 and 4 Trigger efficiency =65% for  magnetic moment interactions with T>0.5GeV Tune each cut to remove no more than ~5% of the magnetic moment interactions

Cuts Muon ID –remove muons and hadrons –watch out for noise ®require <2 MID hits (sum over all tracks) EMCAL –require E EMCAL <20GeV –require for each track with P>4GeV that E EMCAL <P/2 for blocks within 0.2m of the track –check the rectangle with |x-x vtx |<0.7m and |y-y vtx |<0.2m : require at least 50% of the EMCAL energy to be inside the rectangle require the energy outside the rectangle to be less than 1GeV

Cuts II SF system: –require small # of SF hits (< 12000) –remove events with: hadrons: highly ionizing tracks (large fiber pulseheight) tracks not coming from the emulsion (muons interacting in the shielding) tracks that go straight through a module (electrons are required to shower) –require at least one straight SF line in each view (<0.1rad) put the vertex at the origin of this line –require the vertex to be in the emulsion volume

Cuts III Trigger counters: –remove backward trigger O O O O O O O O T1 O O X X O O O O O T2 O O X O O O O O T3 –require a trigger panel hit on a straight line behind the vertex VDC: –require VDC hits on a straight line behind the vertex

Cut efficiency: electronic analysis Percentage of events removed in periods 3+4

Cuts IV Refit and find the vertex remove events “by hand” if: –a straight muon is in the SF –the event has only a single track with P>0 –there are slow hadrons in the SF apply all of the previous cuts again output: 3 cat3 events, 14 nustrip events –periods 3 and 4 –MC efficiency for these cuts  100%

Cuts V Careful visual inspection of each event –Can it be scanned? –Check E EMCAL /P for each track –Check track straightness (angle <0.1rad in X and Y) –check trigger timing Output: 0 cat3 events, 1 nustrip event –if   current limit: expect 6 cat3 events, 11 nustrip events

Candidate event

Preliminary Physics result Data analysis: –0 events for T>5GeV –1 events for T>0.5GeV –systematic error: not determined yet, assume  0.5events preliminary 90% confidence limit for the magnetic moment:

Conclusions The magnetic moment analysis is still in progress Searching for event candidates in the nustrip files will give the best limit Emulsion information for candidate events is very important An emulsion-only analysis is only useful if we scan a considerable fraction of the emulsion volume