1 Losses in the Cooling Channel Malcolm Ellis PID Meeting 1 st March 2005.

Slides:



Advertisements
Similar presentations
1 MICE Beamline: Plans for initial commissioning. Kevin Tilley, 16 th November. - 75days until commissioning Target, detectors, particle production Upstream.
Advertisements

January 14, 2004 TJR - - UPDATED 1/25/04 1 MICE Beamline Analysis Using g4beamline Including Jan 25 Updates for Kevin’s JAN04 Beamline Design Tom Roberts.
Emittance definition and MICE staging U. Bravar Univ. of Oxford 1 Apr Topics: a) Figure of merit for MICE b) Performance of MICE stages.
FIGURE OF MERIT FOR MUON IONIZATION COOLING Ulisse Bravar University of Oxford 28 July 2004.
1 Angular Momentum from diffuser Beam picks up kinetic angular momentum (L kin ) when it sits in a field –Canonical angular momentum (L can ) is conserved.
Particle by Particle Emittance Measurement to High Precision Chris Rogers Imperial College/RAL 17th March 2005.
Tracker Reconstruction Stuff Timothy Carlisle Oxford.
1 Tracker Resolution Malcolm Ellis MICE Analysis Forum Meeting 15 th September 2005.
1 Emittance Calculation Progress and Plans Chris Rogers MICE CM 24 September 2005.
1 PID, emittance and cooling measurement Rikard Sandström University of Geneva MICE Analysis phone conference.
1 Downstream PID update Rikard Sandström PID phone conference
KEK Analysis Report Makoto Yoshida Osaka Univ. 2006/06/10 MICE CM15.
TJR Sept 22, 2004MICE Beamline Analysis -- SEPT041 MICE Beamline Analysis – SEPT04 Tom Roberts Muons, Inc. September 22, 2004.
MICE analysis meeting - (4/5/2006) 1 some reflections on scraping, PID sizes and Transmittance M. Apollonio – University of Oxford.
1Malcolm Ellis - Video Conference - 7th December 2006 Data Challenge Report  Disclaimer  Data Challenge definition(s)  Software status u G4MICE u GRID.
Analysis Meeting – – Slide 1 Beam momentum measurement using TOFs: progress report Analysis Meeting, February 2008 Mark Rayner.
1 Downstream scraping and detector sizes Rikard Sandström University of Geneva MICE collaboration meeting CERN.
1 PID Detectors & Emittance Resolution Chris Rogers Rutherford Appleton Laboratory MICE CM17.
1 PID status MICE Analysis phone conference Rikard Sandström.
1 G4MICE studies of PID transverse acceptance MICE video conference Rikard Sandström.
Downstream transversal sizes Rikard Sandström University of Geneva MICE detector meeting.
PID Detector Size & Acceptance Chris Rogers Analysis PC
M.apollonioCM17 -CERN- (22/2 - 25/2 2007)1 Single Particle Amplitude 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.
Tracker Misalignment Study David Forrest CM23 HIT, Harbin January 14 th.
Beam line characterization with the TOFs1 Demonstrating the emittance-momentum matrix Mark Rayner, CM26 California, 24 March Initial.
Diffuser in G4MICE Victoria Blackmore 09/03/10 Analysis Meeting 1/8.
1 OPTICS OF STAGE III Ulisse Bravar University of Oxford 6 October 2004.
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.
Beam Parameter Study - preliminary findings Tim Carlisle.
1 Emittance Calculation Progress and Plans Chris Rogers Analysis PC 18 August 2005.
1Malcolm Ellis - Software Meeting - 31st May 2006 Data Challenge Requirements  First list of requirements, based on Yagmur’s document: u
1 G4MICE Analysis of KEK Test Beam Aron Fish Malcolm Ellis CM15 10th June 2006.
Jun 27, 2005S. Kahn -- Ckov1 Simulation 1 Ckov1 Simulation and Performance Steve Kahn June 27, 2005 MICE Collaboration PID Meeting.
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.
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.
M.apollonio/j.cobbMICE UK meeting- RAL - (9/1/2007) 1 Single Particle Amplitude M. Apollonio – University of Oxford.
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.
Diffuser Studies Chris Rogers, IC/RAL MICE VC 09 March 2005.
Analysis of MICE Chris Rogers 1 Imperial College/RAL Thursday 28 October, With thanks to John Cobb.
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.
MICE pencil beam raster scan simulation study Andreas Jansson.
Particle Production in the MICE Beam Line Particle Accelerator Conference, May 2009, Vancouver, Canada Particle Production in the MICE Beam Line Jean-Sebastien.
Results from Step I of MICE D Adey 2013 International Workshop on Neutrino Factories, Super-beams and Beta- beams Working Group 3 – Accelerator Topics.
11 Nov 2008PC Analysis PC Schedule 2008 Tuesdays fortnightly 9 September  23 September  2 October  CM22  11 November  25 November 9 December.
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 Statistics David Forrest University of Glasgow May 5 th 2009.
M. Ellis - MICE Collaboration Meeting - Thursday 28th October Sci-Fi Tracker Performance Software Status –RF background simulation –Beam simulation.
26 Oct 2010PC Physics Requirements of Software from Chris R ~19 Oct. My.
Analysis meeting: Beam momentum measurements using TOFs Tuesday, 22 January 2008 Slide 1 of 10 Beam momentum measurement using.
1 Statistics Update David Forrest University of Glasgow.
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.
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.
CKOV1 design status 1. Generation of muon and pion beam files 2. PID performances with water radiator 3. Does it help with fluorocarbon FC72 ? 4. Conclusion.
MEASUREMENT OF EMITTANCE AND OTHER OPTICS QUANTITIES V. Blackmore 01/19.
August 8, 2007 AAC'07 K. Yonehara 1 Cooling simulations for Muon Collider and 6DMANX Katsuya Yonehara Fermilab APC MCTF.
Muons, Inc. Feb Yonehara-AAC AAC Meeting Design of the MANX experiment Katsuya Yonehara Fermilab APC February 4, 2009.
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
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
Design of the MANX experiment
PANDA Collaboration Meeting
The Detector System of the MICE Experiment
Presentation transcript:

1 Losses in the Cooling Channel Malcolm Ellis PID Meeting 1 st March 2005.

2 Simulation  10 simulations of a matched beam, with very narrow P Z, and transverse emittance from 0.5 – 9.5  mm rad.  Beam is started just upstream of the upstream SciFi tracker and simulated through the experiment to the downstream tracker.  Simulation of the full MICE (stage VI) cooling channel.  Material, field map, etc as described at LBNL meeting.

3 Reference Planes Upstream Tracker Downstream Tracker Cooling Channel  10 reference planes provide Monte Carlo truth information (one for each station).  Distributions of radial position of muon in Station 1 (closest to cooling channel) are compared  In next slides, upstream is red, downstream is blue.

4 0.5 and 1.5  mm rad

5 2.5 and 3.5  mm rad

6 4.5 and 5.5  mm rad

7 6.5 and 7.5  mm rad

8 8.5 and 9.5  mm rad

9 Transmission  Ratio of number of muons in downstream to upstream tracker is compared.  Transmission flat at about 99.3% at low emittance, then drops to 90% at 9.5  mm rad.