Analysis of aCORN Data J. E. Adelman*, M. S. Dewey†, F. Wietfeldt‡, G. Darius‡, G.L. Jones*, B. Collett*, and R. Kosar* August 2012 * Hamilton College,

Slides:



Advertisements
Similar presentations
1 The and -Z Exchange Corrections to Parity Violating Elastic Scattering 周海清 / 东南大学物理系 based on PRL99,262001(2007) in collaboration with C.W.Kao, S.N.Yang.
Advertisements

The best collimator configuration (material, number of collimators, collimator shape) is determined by minimizing the ratio R, where N ae is the number.
5/3/2015J-PARC1 Transverse Matching Using Transverse Profiles and Longitudinal Beam arrival Times.
IKON7, Instrument clip session, September 2014, ESS Headquarters and Medicon Village, Lund, Sweden A cold neutron beamline for Particle
Analysis of instrumental effects in HIBP equilibrium potential profile measurements on the MST-RFP Xiaolin Zhang Plasma Dynamics Lab, Rensselaer Polytechnic.
Statistics for Managers Using Microsoft® Excel 5th Edition
F.Sanchez (UAB/IFAE)ISS Meeting, Detector Parallel Meeting. Jan 2006 Low Energy Neutrino Interactions & Near Detectors F.Sánchez Universitat Autònoma de.
Ionization. Measuring Ions A beam of charged particles will ionize gas. –Particle energy E –Chamber area A An applied field will cause ions and electrons.
I.1 ii.2 iii.3 iv.4 1+1=. i.1 ii.2 iii.3 iv.4 1+1=
Commissioning of a Nebraska-type Retarding Potential Mott Polarimeter J. McCarter, M. L. Stutzman, T. J. Gay, K. Trantham, P. Adderley, J. Brittian, J.
Using GEMINI to study multiplicity distributions of Light Particles Adil Bahalim Davidson College Summer REU 2005 – TAMU Cyclotron Institute.
Introduction to Hadronic Final State Reconstruction in Collider Experiments Introduction to Hadronic Final State Reconstruction in Collider Experiments.
Adil Bahalim Davidson College Dr. Joseph Natowitz (Advisor), Dr. Seweryn Kowalski (Mentor) Summer REU 2005 – TAMU Cyclotron Institute Reconstruction Main.
Neutron background measurement at LNGS: present status Measurement carried out in collaboration between LNGS ILIAS-JRA1 and ICARUS groups.
I.1 ii.2 iii.3 iv.4 1+1=. i.1 ii.2 iii.3 iv.4 1+1=
Previous Work. Gauss fit with pion, proton, electron.
Study of two pion channel from photoproduction on the deuteron Lewis Graham Proposal Phys 745 Class May 6, 2009.
Superheavy Element Studies Sub-task members: Paul GreenleesJyväskylä Rodi Herzberg, Peter Butler, RDPLiverpool Christophe TheisenCEA Saclay Fritz HessbergerGSI.
Forward Detectors and Measurement of Proton-Antiproton Collision Rates by Zachary Einzig, Mentor Michele Gallinaro INTRODUCTION THE DETECTORS EXPERIMENTAL.
Parity Violation in Electron Scattering Emlyn Hughes SLAC DOE Review June 2, 2004 *SLAC E122 *SLAC E158 *FUTURE.
ALLEGRO G Z LSC, Livingston 23 March, Calibration for the ALLEGRO resonant detector -- S2 and S4 Martin McHugh, Loyola University New Orleans.
Oct 15, 2003 Video Conference Energy Deposition Steve Kahn Page 1 Energy Deposition in MICE Absorbers and Coils Steve Kahn November 2, 2003.
Trying to Give Business Students What They Need for Their Future Bob Andrews Virginia Commonwealth University.
Handling Data and Figures of Merit Data comes in different formats time Histograms Lists But…. Can contain the same information about quality What is meant.
Diana Parno – July 22, 2008 January PREx Test Run: Compton Photon Analysis Diana Parno Carnegie Mellon University HAPPEX Collaboration Meeting.
Irakli Chakaberia Final Examination April 28, 2014.
Edwin Chng. Contents Decay Solenoid Electron Peak Muon Peak Slab Hits Appendix Slide 2.
Results from Step I of MICE D Adey 2013 International Workshop on Neutrino Factories, Super-beams and Beta- beams Working Group 3 – Accelerator Topics.
COMPTON POLARIMETRY Collected data Cavity power Status on counting methods Systematic errors and hardware issues.
Observation of W decay in 500GeV p+p collisions at RHIC Kensuke Okada for the PHENIX collaboration Lake Louise Winter Institute February 20, /20/20101.
Status of E391a Search for K L    decay G.Y.Lim IPNS, 32nd ICHEP 19 th August 2004 Beijing.
8.1.4 Can it still be factored? Factoring Completely I can factor out a common factor.
Neutron Beam Intensity for the Spallation Neutron Source Beamline 13: The NPDGamma Experiment Analysis and Results Jeremy Stewart University of Tennessee.
Ian Ross Rose-Hulman Institute of Technology Mentor: Dr. Richard Teuscher University of Toronto ATLAS Group ATLAS Calorimetery: Cosmic Ray Commissioning.
Mass spectrometry (Test) Mass spectrometry (MS) is an analytical technique that measures masses of particles and for determining the elemental composition.
Preliminary Results from the MINER A Experiment Deborah Harris Fermilab on behalf of the MINERvA Collaboration.
Electron Collimator Design for the Little “a” Measurement Travis Clark, Aung Kyaw Sint, Dr. Alex Komives Project Objective & Purpose: Beta Decay Explained.
BigCal Calibration E04-108& Wei Luo Lanzhou University, China January 2008 Hall C Users Meeting.
Introduction to Basic Statistical Tools for Research OCED 5443 Interpreting Research in OCED Dr. Ausburn OCED 5443 Interpreting Research in OCED Dr. Ausburn.
The aSPECT collaboration: Institut für Physik, Universität Mainz, Germany: F. Ayala Guardia, M. Borg, F. Glück, W. Heil, G. Konrad, N. Luquero Llopis,
Hycal Energy Resolution, Timing, &Trigger Efficiency, A cumulative study. Chris Mauney.
Top mass error predictions with variable JES for projected luminosities Joshua Qualls Centre College Mentor: Michael Wang.
Emily Nurse W production and properties at CDF0. Emily Nurse W production and properties at CDF1 The electron and muon channels are used to measure W.
APPLICATION OF A WAVELET-BASED RECEIVER FOR THE COHERENT DETECTION OF FSK SIGNALS Dr. Robert Barsanti, Charles Lehman SSST March 2008, University of New.
How does a smoke detector work? Theme: Stability and Change A review of what we’ve learned about the nucleus so far!
SANE Collaboration ( E07-003) Anusha Liyanage Hampton University January 12, 2010 Measurement Of the Proton Form Factor Ratio at High Q 2 by Using The.
Elliptic flow of electrons from heavy flavor decays
The cosmic connection There is a very close connection between particle physics and astrophysics. I’m going to show two examples: Type II supernovas Dark.
Highest Q 2 Polarized Measurement of the Electric Form Factor of the Neutron – E Presented by Jonathan Miller For the Hall A E Collaboration.
Moriond QCD March 24, 2003Eric Kajfasz, CPPM/D01 b-production cross-section at the TeVatron Eric Kajfasz, CPPM/D0 for the CDF and D0 collaborations.
NUMI NUMI/MINOS Status J. Musser for the MINOS Collatoration 2002 FNAL Users Meeting.
Measuring Oscillation Parameters Four different Hadron Production models  Four predicted Far  CC spectrum.
Background Shape Study for the ttH, H  bb Channel Catrin Bernius First year talk 15th June 2007 Background Shape Study for the ttH 0, H 0  bb Channel.
G0 Backward Angle Request: Q 2 = 0.23, 0.48 GeV 2 Main points G0 goal is to measure G E s, G M s and G A e over range of momentum transfers with best possible.
ArgonneResult_ ppt1 Comparison of data and simulation of Argonne Beam Test July 10, 2004 Tsunefumi Mizuno
ArgonneResult_ ppt1 Results of PoGO Argonne Beam Test PoGO Collaboration meeting at SLAC, February 7, 2004 Tsunefumi Mizuno
(one of the) Request from MPB
Static electricity The atomRules for charges + and + -and – -+ and - Relative charge Releative mass Proton Neutron Electron Electrostatic paint spraying.
OD Tuning: SK-IV Roger Wendell TMC Meeting
Neutron Imaging and Tomography with MCPs
Activities on straw tube simulation
Detection of muons at 150 GeV/c with a CMS Preshower Prototype
Analyzing Redistribution Matrix with Wavelet
Status of the TOF Detector
Investigation on Part of Work Done by Electroweak Group
G0 Beam Polarization T. Horn, D. Gaskell Jefferson Lab
Status of Instrumental Beam Studies and Technical Description of Detectors and DAQ February 24, 2017.
The np -> d p0 reaction measured with g11 data
Picture 1 10 protons 10 neutrons = an electron.
Measurement of Parity-Violation in the N→△ Transition During Qweak
Presentation transcript:

Analysis of aCORN Data J. E. Adelman*, M. S. Dewey†, F. Wietfeldt‡, G. Darius‡, G.L. Jones*, B. Collett*, and R. Kosar* August 2012 * Hamilton College, Clinton NY † The National Institute of Standards and Technology, Gaithersburg, MD ‡ Tulane University, New Orleans, LA.

Background: Neutron Decays Free neutrons undergo beta decay Standard Model: Two constants characterize this decay – g A : axial coupling – g V : vector coupling

Neutron decay has several correlation coefficients – Know any two, get g V, g A. – Know any three – test standard model a is the electron-antineutrino correlation coefficient – Current value: ± 0.004

veve Background II: The aCORN Project To get a, measure antineutrino and electron momentum – Proton used to infer ν ē Experiment designed to give two groups – “Fast” and “Slow” protons p+ veve e- p+ Electron Detector Proton Detector Group 1 “Fast” Group 2 “Slow”

Group Separation depends on electron energy – Result: “Wishbone” data shape “Slow” Group “Fast” Group

The aCORN Apparatus Analysis focused on four apparatus parameters 1. Electrostatic mirror voltage 2. Electron detector trim coil current 3. Proton detector size and focusing grid 4. Electron detector gain

Current State of aCORN Apparatus assembled on NCNR’s NG-6 beamline January – March 2011: Data collection – Raw data distilled and reduced prior to analysis Another round with the beam – February 2012

Goals: 1.Introduce a new calibration paradigm 2.Perform series by series analysis on outstanding data 3.Note the effects of parameter changes on calculated asymmetries 4.Offer suggestions for next round of data collection

Part I: Calibration Bi and Sn sources Points of Analysis: – Resolutions – Are three Gaussians better than one? – Effect of apparatus parameters on resolutions Channel Number Counts

Results Resolutions still below expectations – Need ~ 20% Three Gaussian: – 1% better on Sn – 2% better on Bi 975 Curve correlated to run parameters New Bi source shows promise of improved

Part II: Series Analysis Goal: extract values for “pseudo-a”, wishbone rate, and background rate for all outstanding data.

Part III: Analysis Original Goal: Algebraic isolation of individual effects by pairwise examination – Problem: Splitting series in half gives values beyond the calculated error bars Fallback: Single-factor Analysis of Variance (ANOVA) – f-test to find correlations – Difficult to discern contributions from multiple effects

ANOVA Results Algebraic analysis indicated effects on the order of pseudo a Evidence is consistent with a problem detecting protons

Series Summary

Part IV: Unanswered Questions Missing Rate Shape to Rate vs. Time Graph

Acknowledgement I would like to thank NIST, the SURF advisors, my mentor Scott Dewey, the members of the aCORN consortium, PML’s Neutron Research group, and everyone else who helped foster an enjoyable and productive summer