CURVATURE RECONSTRUCTION PERFORMANCE SLAC ILC Simulation Meeting September 15 2009 Alex Bogert (Undergraduate student) Bruce Schumm Question: ILD Higgs.

Slides:



Advertisements
Similar presentations
Weighted Least Squares Regression Dose-Response Study for Rosuvastin in Japanese Patients with High Cholesterol "Randomized Dose-Response Study of Rosuvastin.
Advertisements

Background effect to Vertex Detector and Impact parameter resolution T. Fujikawa(Tohoku Univ.) Feb LC Detector Meeting.
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.
1 Vertex fitting Zeus student seminar May 9, 2003 Erik Maddox NIKHEF/UvA.
March 6th, 2006CALICE meeting, UCL1 Position and angular resolution studies with ECAL TB prototype Introduction Linear fit method Results with 1, 2, 3,
SCIPP R&D on the International Linear Collider Detector SCIPP Review May 18, 2006 Presenter: Bruce Schumm.
SCIPP R&D on the International Linear Collider Detector SCIPP Review November 29, 2005 Presenter: Bruce Schumm.
Search for B     with SemiExclusive reconstruction C.Cartaro, G. De Nardo, F. Fabozzi, L. Lista Università & INFN - Sezione di Napoli.
Tracking Efficiency and Momentum Resolution Analysis Chris Meyer UCSC ILC Simulation Reconstruction Meeting March 13, 2007.
Search for LFV  decays involving     ’ at Belle Y. Enari, Belle collaboration Nagoya University.
SIMULATION RESULTS FROM THE SANTA CRUZ LINEAR COLLIDER GROUP Bruce Schumm University of California at Santa Cruz 4 th SiLC Meeting, Barcelona December.
Tracking Simulation Studies at UC Santa Cruz Bruce Schumm UCSC/SCIPP LCWS07 DESY May 30-Jun Tracking Validation Studies Non-prompt tracks with SiD.
1 Physics Impact of Detector Performance Tim Barklow SLAC March 18, 2005.
Impact of ILC Tracker Design on e  e   H 0 Z 0       X Analysis Hai-Jun Yang & Keith Riles University of Michigan, Ann Arbor SiD Benchmarking.
Tracker Performance Benchmarks for High-pT Tracks ALCPG Winter SLAC January 7, 2004 Richard Partridge Brown University.
G. Cowan RHUL Physics Bayesian Higgs combination page 1 Bayesian Higgs combination using shapes ATLAS Statistics Meeting CERN, 19 December, 2007 Glen Cowan.
PPR meeting - January 23, 2003 Andrea Dainese 1 TPC tracking parameterization: a useful tool for simulation studies with large statistics Motivation Implementation.
880.P20 Winter 2006 Richard Kass Propagation of Errors Suppose we measure the branching fraction BR(Higgs  +  - ) using the number of produced Higgs.
Pion test beam from KEK: momentum studies Data provided by Toho group: 2512 beam tracks D. Duchesneau April 27 th 2011 Track  x Track  y Base track positions.
Analysis Meeting vol Shun University.
E. Devetak - LCWS t-tbar analysis at SiD Erik Devetak Oxford University LCWS /11/2008 Flavour tagging for ttbar Hadronic ttbar events ID.
1 ZH Analysis Yambazi Banda, Tomas Lastovicka Oxford SiD Collaboration Meeting
1 Simulation study of e + e -  W H + W H - Introduction Observable to be measured Analysis framework Event selection Results Rei Sasaki (Tohoku University)
ILC Tracking R&D at SCIPP SiD Workshop Thursday, June Bruce Schumm Santa Cruz Institute for Particle Physics.
Mark Thomson University of Cambridge  LoI loose ends  New physics studies?  What next... Future Plans… This talk:
Search for Invisible Higgs Decays at the ILC Akimasa Ishikawa (Tohoku University)
Thomas Knotts. Engineers often: Regress data  Analysis  Fit to theory  Data reduction Use the regression of others  Antoine Equation  DIPPR.
Impact parameter resolution study for ILC detector Tomoaki Fujikawa (Tohoku university) ACFA Workshop in Taipei Nov
Highlights From ILC R&D at SCIPP LCWS 2010 Friendship Hotel, Beijing, PRC March Bruce Schumm Santa Cruz Institute for Particle Physics.
ILC DBD Common simulation and software tools Akiya Miyamoto KEK ILC PAC 14 December 2012 at KEK.
The Santa Cruz Linear Collider Group Simulation Effort SiLC Workshop Prague, Czech Republic April 26, 2007 Bruce Schumm.
Possibility of tan  measurement with in CMS Majid Hashemi CERN, CMS IPM,Tehran,Iran QCD and Hadronic Interactions, March 2005, La Thuile, Italy.
SiD performance for the DBD Jan Strube CERN. Overview Software Preparation (CERN, SLAC) Machine Environment (CERN, SLAC) Tracking Performance (C. Grefe)
LCWS 06 Bangalore, India, March Track fitting using weight matrix Nick Sinev, University of Oregon.
Measurement of the branching ratios for Standard Model Higgs decays into muon pairs and into Z boson pairs at 1.4 TeV CLIC Gordana Milutinovic-Dumbelovic,
August 26, 2003P. Nilsson, SPD Group Meeting1 Paul Nilsson, SPD Group Meeting, August 26, 2003 Test Beam 2002 Analysis Techniques for Estimating Intrinsic.
Determination of True Attenuation Lengths using SPASE-AMANDA Coincidence Data Tim Miller JHU/APL.
Taikan Suehara, 16 th general meeting of ILC physics (Asia) wg., 2010/07/17 page 1 Model 500 GeV Taikan Suehara ICEPP, The Univ. of Tokyo.
Tracking at the ILC: Why Silicon Tracking is Best, and How it Might Be Optimized Bruce Schumm SCIPP & UC Santa Cruz STD6 “AbeFest” September 11, 2006.
Taikan Suehara et al., Albuquerque, 1 Oct page 1 Tau-pair analysis in the ILD detector Taikan Suehara (ICEPP, The Univ. of Tokyo) T. Tanabe.
1 Top and Tau Measurements Tim Barklow (SLAC) Oct 02, 2009.
This work was performed under the auspices of the U.S. Department of Energy by the University of California, Lawrence Livermore National Laboratory under.
1TeV study for DBD ILD analysis meeting Sep H. Ono (NDU) Sep ILD analysis meeting TeV study 1.
Event Generation of Tim Barklow SLAC October 21, 2010.
QCD Background Estimation From Data Rob Duxfield, Dan Tovey University of Sheffield.
Lucia Bortko | Optimisation Studies for the BeamCal Design | | IFJ PAN Krakow | Page 1/16 Optimisation Studies for the BeamCal Design Lucia.
VXDBasedReco TRACK RECONSTRUCTION PERFORMANCE STUDIES Bruce Schumm University of California at Santa Cruz ALCPG Workshop, Snowmass Colorado August 14-28,
Tau polarization LoI Benchmarking Study Tim Barklow Ron Cassell Subhendu Chakrabarti Ray F. Cowan Cosmin Deaconu Rich Partridge SiD Collaboration Meeting.
December, Calibration of electromagnetic calorimeter of Hall A DVCS experiment Eric FUCHEY Ph.D Laboratoire de Physique Corpusculaire.
Particle identification by energy loss measurement in the NA61 (SHINE) experiment Magdalena Posiadala University of Warsaw.
Shun Watanuki (Tohoku University) 1.  How does the tracker resolution affect the results of the measurement of Higgs recoil mass and cross section? 
Taikan Suehara, 15 th general meeting of ILC physics (Asia) wg., 2010/05/15 page 1 Model 500 GeV Taikan Suehara ICEPP, The Univ. of Tokyo.
Measurement the Higgs mass via the channel: e + e - → Z H → e + e - + X & Analog vs. Digital Energy Reconstruction in the Si-W ECal Youssef KHOULAKI ILCP.
Simulation Plan Discussion What are the priorities? – Higgs Factory? – 3-6 TeV energy frontier machine? What detector variants? – Basic detector would.
Tracking: An Experimental Overview Richard Partridge Brown / SLAC Fermilab ALCPG Meeting.
Physics performance with SB2009 Progress report of a study by QuickSimulator Akiya Miyamoto 15-Jan-2010 KEK SB2009 WG Meeting.
Higgs Recoil Mass Measurement and ZH Cross Section Tim Barklow, Awatif Belymam SLAC Feb 24, 2009.
SiD Benchmarking Status
Measurement of sZH using Zqq mode - preliminary result -
Discrimination of new physics models with ILC
Erik Devetak Oxford University SiD Workshop 24/02/2009
(5) Notes on the Least Squares Estimate
M. Kuhn, P. Hopchev, M. Ferro-Luzzi
Step 1 Analysis: Progress Towards the Emittance Paper
Top and WW final states Harry Weerts For LC working group
ILD Optimisation: towards 2012 University of Cambridge
LCWS10 & ILC10, Beijing, China, March 2010
Width vs. Area for Sample Squares
B  at B-factories Guglielmo De Nardo Universita’ and INFN Napoli
Study of Hb`b, c`c and gg in the `H channel
Presentation transcript:

CURVATURE RECONSTRUCTION PERFORMANCE SLAC ILC Simulation Meeting September Alex Bogert (Undergraduate student) Bruce Schumm Question: ILD Higgs LOI recoil reconstruction appears somewhat better than SiD’s. Could this be due to curvature reconstruction?

CURVATURE RECONSTRUCTION PERFORMANCE 1.Compare width of Gaussian fit to residuals with two different estimates: Error from square root of appropriate diagonal error matrix element Error from Billior calculation (LCDTRK program) 2.Only tracks with all DOF (5 VTX and 5 CT layers) are considered. 3.Only gaussian smearing is used, since this is what is assumed for the two estimators. Use q/qbar at 500 and 1000 GeV, tau samples at 500 GeV, all mixed together (shouldn’t matter)

CURVATURE ERROR vs. CURVATURE LCDTRK calculation includes beam constraint Gaussian fit

Snowmass 2005 Results (RMS residual)

Most HZ tracks have all 10 DOF (but very small statistics!) Tracks from HZ events P t > 5 Gev/c |cos(  )| < 0.8