Preliminary Results on Conversions Non-pointing Photon Meeting January 28 2009 Bruce Schumm, UCSC/SCIPP.

Slides:



Advertisements
Similar presentations
First look at mass constraint [How simple can it be?] Two decays: i) pi 0 -> g g ii) K 0 -> pi+ pi- - Mother particle momenta: P = 1, 2, 4, 8, 16 GeV -
Advertisements

Alain Romeyer - January Light higgs decay in SUSY cascade - Status report Introduction Trigger efficiency B tagging Jet calibration Invariant mass.
Effects of Tracking Limitations On Jet Mass Resolution Chris Meyer UCSC ILC Simulation Reconstruction Meeting July 3, 2007.
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.
Using  0 mass constraint to improve particle flow ? Graham W. Wilson, Univ. of Kansas, July 27 th 2005 Study prompted by looking at event displays like.
From GMSB to Photons plus Missing E t : Some Thoughts on Model Independence SUSY/E t Miss “Kickoff” Meeting February 5, 2010 Bruce Schumm, UCSC/SCIPP.
Non-Pointing Photon Work at UC Santa Cruz / SCIPP ATLAS RPV/Long-lived Physics Group November Bruce Schumm, UCSC/SCIPP.
GMSB Trigger Efficiency and Data Stream Issues Non-pointing Photon Meeting September Bruce Schumm, UCSC/SCIPP.
Intended Contributions from the SCIPP (UC Santa Cruz) Group ATLAS e  Workshop June Bruce Schumm, UCSC/SCIPP, for Alan Litke, Jason Nielsen (faculty)
First Look at Conversions for Non-Pointing Photons US ATLAS Egamma Meeting March Bruce Schumm, UCSC/SCIPP.
Reconstruction of neutrino interactions in PEANUT in general scanning (unbiased) mode Giovanni De Lellis on behalf of Andrea Russo Naples University.
GMSB2 Trigger Efficiency vs. Decay Radius for Some 3- Jet Triggers Non-pointing Photon Meeting August Bruce Schumm, UCSC/SCIPP.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 33.
I.1 ii.2 iii.3 iv.4 1+1=. i.1 ii.2 iii.3 iv.4 1+1=
Horng-Chyi HorngStatistics II_Five43 Inference on the Variances of Two Normal Population &5-5 (&9-5)
Tracking Efficiency and Momentum Resolution Analysis Chris Meyer UCSC ILC Simulation Reconstruction Meeting March 13, 2007.
Update from the Photons + MET Group Bruce Schumm UC Santa Cruz / SCIPP 26 August 2010 SUSY/MET Meeting.
First Look at Conversions for Non-Pointing Photons US ATLAS Egamma Meeting March Bruce Schumm, UCSC/SCIPP.
Update on Conversions SCIPP ATLAS Meeting February Bruce Schumm, UCSC/SCIPP.
Neutrino Event Reconstruction Andy Blake Cambridge University September 2003.
I.1 ii.2 iii.3 iv.4 1+1=. i.1 ii.2 iii.3 iv.4 1+1=
Further Update on Conversions ATLAS Informal Two Photon Meeting February Bruce Schumm, UCSC/SCIPP.
1 Physics Impact of Detector Performance Tim Barklow SLAC March 18, 2005.
Analysis work by: Marina Artuso Sheldon Stone Jianchun Wang CBX note available: /homes/cleo/sls/dompi.ps Study of B  D   Jianchun Wang 05/12/00.
Some Thoughts and Pleas from the SCIPP (UC Santa Cruz) Group US ATLAS e  Forum Meeting June Bruce Schumm, UCSC/SCIPP, for Alan Litke, Jason Nielsen.
Tracker Performance Benchmarks for High-pT Tracks ALCPG Winter SLAC January 7, 2004 Richard Partridge Brown University.
ISSUES AND SYSTEMATICS ASSOCIATED WITH FIDING LOW-ENERGY PHOTONS WHEN RECONSTRUCTING  0 s Luke Winstrom Al Eisner Bruce Schumm.
Reconstruction of neutrino interactions in PEANUT G.D.L., Andrea Russo, Luca Scotto Lavina Naples University.
Atmospheric Neutrino Oscillations in Soudan 2
Current Status of Hadron Analysis Introduction Hadron PID by PHENIX-TOF  Current status of charged hadron PID  CGL and track projection point on TOF.
Irakli Chakaberia Final Examination April 28, 2014.
Miscellaneous examples 1. Given that a = log 10 2 and b = log 10 5, find expressions in terms of a and b for: (i) log (ii) log (iii) log 10.
Response of AMANDA-II to Cosmic Ray Muons and study of Systematics Newt,Paolo and Teresa.
Simulation of the energy response of  rays in CsI crystal arrays Thomas ZERGUERRAS EXL-R3B Collaboration Meeting, Orsay (France), 02/02/ /03/2006.
Angular resolution study of GLD Calorimeter 2006/Dec/21 ILC-sousei Annual Meeting M1 ICEPP, Tokyo Hitoshi HANO.
Measurement of b-tagging Fake rates in Atlas Data M. Saleem * In collaboration with Alexandre Khanov** F. Raztidinova**, P.Skubic * *University of Oklahoma,
Difference between Roman Pots and VELO Very forward tracking is typically done using detectors located in Roman pots. They are far away from the interaction.
Λ and Σ photoproduction on the neutron Pawel Nadel-Turonski The George Washington University for the CLAS Collaboration.
Photon reconstruction and matching Prokudin Mikhail.
Status Report particle identification with the RICH detector Claudia Höhne - GSI Darmstadt, Germany general overview focus on ring radius/ Cherenkov angle.
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,
1 Detector Performance and Physics talks at Bern (very selective!) Pete Watkins.
Neutron Detection in JLab’s Hall B Michael Braverman Tel-Aviv University Data Mining Meeting, MIT, August 9th 2014 In Collaboration With : E. Piasetzky.
Mike HildrethEPS/Aachen, July B Physics Results from DØ Mike Hildreth Université de Notre Dame du Lac DØ Collaboration for the DØ Collaboration.
Thomas RufVELO RZ ProjectionFebruary Motivation Find useful projections which help to debug the reconstruction algorithms. Event display useful.
Signatures IV Group Report ALCPG07 FNAL, Oct Bruce Schumm, UCSC/SCIPP Momentum Reconstruction, V0 Finding, and Charged Particle ID Apologies to.
06/2006I.Larin PrimEx Collaboration meeting  0 analysis.
January 13, 2004A. Cherlin1 Preliminary results from the 2000 run of CERES on low-mass e + e - pair production in Pb-Au collisions at 158 A GeV A. Cherlin.
Palaiseau, 13/1/ 2005 P. Colas - Optimising tracking 1 Optimising a Detector from the Tracking Point-of-View P.Colas, CEA Saclay constraints role Optimisation.
The Birthday Problem. The Problem In a group of 50 students, what is the probability that at least two students share the same birthday?
1 HBD Update Itzhak Tserruya DC meeting, May 7, 2008 May7, 2008.
VXDBasedReco TRACK RECONSTRUCTION PERFORMANCE STUDIES Bruce Schumm University of California at Santa Cruz ALCPG Workshop, Snowmass Colorado August 14-28,
Study of Charged Hadrons in Au-Au Collisions at with the PHENIX Time Expansion Chamber Dmitri Kotchetkov for the PHENIX Collaboration Department of Physics,
LNF 12/12/06 1 F.Ambrosino-T. Capussela-F.Perfetto Update on        Dalitz plot slope Where we started from A big surprise Systematic checks.
Photon Selection Algorithm Ming Yang , Mingshui Chen BESIII Meeting
Reconstruction of converted photons E. Tournefier LAPP meeting Feb. 2,2012 Algorithm for the reconstruction of converted photons Performances studies:
F2F Tracking Meeting, Prague 12/12/2013
Converted photons efficiency
Converted photons efficiency
HARPO Analysis.
Detector Configuration for Simulation (i)
Tagging in T(b) (I) Generated 1M events of e + Pb208 collisions at 10  40 GeV/n with 1 < Q2 < 20, 0.3 < y < 0.95, parameter settings tuned by Mark, genShd.
Jaewon Park University of Rochester
Preliminary Comparison of Monte Carlo and 9-string IceCube Data
Angular resolution: Critical for source morphology
Progress in angular acceptance study
Prospects for quarkonium studies at LHCb
Measurement of
road – Hough transform- c2
Problems in π0 Reconstruction
Presentation transcript:

Preliminary Results on Conversions Non-pointing Photon Meeting January Bruce Schumm, UCSC/SCIPP

Initial goal: include conversions in reconstruction Mauro Donega, UPenn Conversion radius resolution may be good enough to provide an independent constraint on GMSB parameters Pointing accuracy of reconstructed conversion may be quite good Reconstructed radius of material-induced conversions

Step I: Reconstruction Reconstruct in , but with two updated tags: TrkParticleCreator and TrkTrackSlimmingTool (confirmed with Thomas Koffas that this should give good conversion performance) Reconstruct 50 events of GMSB2

Step II: Learn to use Conversion Container There are two types of conversions: single-track and two-track. Here’s the distribution of radius for reconstructed conversions: Note that there are 1076 reconstructed conversions in 50 events!

And separately for one- and two-track conversions:

Step III: Truth Matching Define momentum ratio P as P = (p reco – p truth )/p truth and let R be the three-dimensional angle between and with For each reconstructed conversion, loop through true conversions and plot the minimum P and R.

3D Angular Separation ALL One track Two track

Momentum Ratio ALL One track Two track ???