Tracker Reconstruction Stuff Timothy Carlisle Oxford.

Slides:



Advertisements
Similar presentations
1 Progress report on Calorimeter design comparison simulations MICE detector phone conference Rikard Sandström.
Advertisements

Emittance definition and MICE staging U. Bravar Univ. of Oxford 1 Apr Topics: a) Figure of merit for MICE b) Performance of MICE stages.
“Amplitude Cooling” in Step III & IV Timothy Carlisle.
1 Tracker Resolution Malcolm Ellis MICE Analysis Forum Meeting 15 th September 2005.
Cooling channel issues U. Bravar Univ. of Oxford 31-Mar-2004.
1 PID, emittance and cooling measurement Rikard Sandström University of Geneva MICE Analysis phone conference.
SLIDE Beam measurements using the MICE TOF counters Analysis meeting, 23 September 2008 Mark Rayner.
KEK Analysis Report Makoto Yoshida Osaka Univ. 2006/06/10 MICE CM15.
1 September 09Mark Rayner – Emittance measurement by The TOFs1 Emittance measurement by the TOFs Via trace space reconstruction of individual muons. Complementary.
Analysis Meeting – – Slide 1 Beam momentum measurement using TOFs: progress report Analysis Meeting, February 2008 Mark Rayner.
OPTICS UPDATE Ulisse Bravar University of Oxford 3 August 2004.
1 Downstream scraping and detector sizes Rikard Sandström University of Geneva MICE collaboration meeting CERN.
MICE analysis meeting - (6/4/2006) 1 Update on MICE – step III M. Apollonio – University of Oxford.
MICE analysis meeting - (21/09/2006) 1 Transmittance, scraping and maximum radii for MICE STEPVI M. Apollonio – University of Oxford.
1 Statistics Toy Monte Carlo David Forrest University of Glasgow.
1 Losses in the Cooling Channel Malcolm Ellis PID Meeting 1 st March 2005.
Simulated real beam into simulated MICE1 Mark Rayner CM26.
1 KEK Beam Test Analysis Hideyuki Sakamoto 15 th MICE Collaboration Meeting 10 st June,2006.
Beamline-to-MICE Matching Ulisse Bravar University of Oxford 2 August 2004 MICE performance with ideal Gaussian beam JUNE04 beam from ISIS beamline (Kevin.
30 June 2004MICE VC1 MICE  functions Since last VC report: –New Mike Green configurations for decreased spacing between focus and matching coils of 400mm,
Beam Parameter Study - preliminary findings Tim Carlisle.
1 G4MICE Analysis of KEK Test Beam Aron Fish Malcolm Ellis CM15 10th June 2006.
MICE Collaboration Meeting 8th Octorber KEK Beam Test Analysis Hideyuki Sakamoto 16 th MICE Collaboration Meeting 8 th October 2006.
Mark Rayner, Analysis workshop 4 September ‘08: Use of TOFs for Beam measurement & RF phasing, slide 1 Use of TOFs for Beam measurement & RF phasing Analysis.
04/01/2006MICE Analysis Meeting1 MICE phase III M. Apollonio, J. Cobb (Univ. of Oxford)
18 August 09Mark Rayner – Momentum measurement by The TOFs1 Momentum measurement by the TOFs A correction to an O(4 MeV/c) bias on the current muon momentum.
Stats update Was asked to provide comparison between toy mc and g4mice at two points along z (middle of first and third absorbers) 10,000 events, step.
Timothy Carlisle, Oxford CM 28. Step 3 Matching Step 3  Step 3 rematched for 830 mm spool piece  Calc. B(z) & BetaFn with the following:  Minimize.
Emittance measurement: ID muons with time-of-flight Measure x,y and t at TOF0, TOF1 Use momentum-dependent transfer matrices iteratively to determine trace.
24/11/2014MAUS Status, A. Dobbs, MPB Talk2 24/11/2014MAUS Status, A. Dobbs, MPB Talk3 CKOV – Threshold Cherenkov detectors (aerogel) TOF – Three Time.
Emittance measurement: ID muons with time-of-flight Measure x,y and t at TOF0, TOF1 Use momentum-dependent transfer matrices to map  path Assume straight.
Tracking Studies of Phase Rotation Using a Scaling FFAG Ajit Kurup FFAG07 12 th – 17 th April 2007.
Takashi Matsushita Imperial College T. Matsushita 1 Tracker performance Vacuum/helium/air.
Introduction Miha Zgubič, summer student Scintillating fibre tracker software Analysis of performance of momentum reconstruction 1.
Results from Step I of MICE D Adey 2013 International Workshop on Neutrino Factories, Super-beams and Beta- beams Working Group 3 – Accelerator Topics.
A NALYSIS OVERVIEW & “T HE M ISSING P HYSICS ” V. Blackmore CM38 23rd February /14.
ICHEP 2012 Melbourne, 7 July 2012 Paul Soler on behalf of the MICE Collaboration The MICE Beam Line Instrumentation (Trackers and PID) for precise Emittance.
MICE input beam weighting Dr Chris Rogers Analysis PC 05/09/2007.
Marco apollonio/J.CobbMICE coll. meeting 16- RAL - (10/10/2006) 1 Transmittance, scraping and maximum radii for MICE STEPVI M. Apollonio – University of.
1 Performance of a Magnetised Scintillating Detector for a Neutrino Factory Scoping Study Meeting Rutherford Appleton Lab Tuesday 25 th April 2006 M. Ellis.
Timing measurements at the MICE experiment – 1 The analysis of timing measurements at the Muon Ionization Cooling Experiment Mark Rayner The University.
Progress in the construction of the MICE cooling channel and first measurements Adam Dobbs, EPS-HEP, 23 rd July 2011.
Step IV Studies Timothy Carlisle Oxford. Intro. CM28 – Step III vs Step IV Cooling formula & G4MICE disagree on – Also observed in ICOOL (note #199 –
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.
Analysis meeting: Beam momentum measurements using TOFs Tuesday, 22 January 2008 Slide 1 of 10 Beam momentum measurement using.
Calorimeter design & simulations for Stage I Rikard Sandström University of Geneva MICE PID phone conference
18 th March 2008Measuring momentum using the TOFsSlide 1 Measuring momentum using TOF0 and TOF1 Progress report Mark Rayner (Oxford/RAL) Analysis Meeting,
Mark Rayner – Analysis SessionCM25, 4 November Beam characterization by the TOFs Mark Rayner The University of Oxford MICE CM25.
Measuring Multiple Scattering in Step IV Timothy Carlisle Oxford See MICE Note 374 for updated results.
Mark Rayner 26/8/08Analysis Meeting: Emittance measurement using the TOFs 1 Measuring emittance with the TOFs Data: –G4MICE has been used to obtain transfer.
M. Ellis - MICE Collaboration Meeting - Wednesday 27th October Sci-Fi Tracker Performance Software Status –RF background simulation –Beam simulation.
Monte Carlo simulation of the particle identification (PID) system of the Muon Ionization Cooling Experiment (MICE) Mice is mainly an accelerator physics.
MICE Step IV Lattice Design Based on Genetic Algorithm Optimizations Ao Liu on behalf of the MICE collaboration Fermilab Ao Liu on behalf of the MICE collaboration.
MEASUREMENT OF EMITTANCE AND OTHER OPTICS QUANTITIES V. Blackmore 01/19.
Mark Rayner – Analysis SessionCM25, 4 November The TOF detectors: Beyond particle identification Mark Rayner The University of Oxford MICE CM25.
(one of the) Request from MPB
MICE S TEP IV P HYSICS ‘D ELIVERABLES ’ V. Blackmore MAP 2014 Spring Meeting 30 th May, /15 AKA “What will we learn from Step IV?”
CM Nov 2009 DOES MICE NEED STEP III ? Somewhat hard to understand MICE Schedule… –If the gods are (un)kind it’s possible that SS1, SS2 & FC1 are.
MEASUREMENT OF EMITTANCE AND OTHER OPTICS QUANTITIES V. Blackmore MICE Optics Review 14 th January, /22.
C. Rogers, ASTeC Intense Beams Group Rutherford Appleton Laboratory
Step IV Physics Paper Readiness
Beam Energy-Loss measurement
MICE Step IV Lattice Design Based on Genetic Algorithm Optimizations
C. Rogers, ASTeC Intense Beams Group Rutherford Appleton Laboratory
Field-on measurement of multiple scattering
Step 1 Analysis: Progress Towards the Emittance Paper
MICE: First Beam Emittance Results w/Particle Detectors
DT Local Reconstruction on CRAFT data
Real Life I BUBBLES! ICECREAM theory.
The Detector System of the MICE Experiment
Presentation transcript:

Tracker Reconstruction Stuff Timothy Carlisle Oxford

Track Finding... Upstream TrackerDownstream Tracker 10,000 muons 6mm beam Two Trackers, no material Step IV fields

Resolution – middle Station X resolution Px resolution Pz resolution (Equivalent for y & Py)

Step IV Empty Black – mc [Virtual Planes], 99.5% Transmitted Green - mc Blue – reconstructed Emittance 4d [mm] Av. Pz [MeV/c] Condition: Abs(mc – rec) < 50 for x, y, px, py to avoid daft emittances..

Step IV with 63mm LiH Black – mc [Virtual Planes] Green - mc Blue – reconstructed Emittance 4d [mm] Av. Pz [MeV/c]