5 May 2009MICE Analysis - MR1 The December Shifts: Beam Characterization by the Time of Flight System Mark Rayner.

Slides:



Advertisements
Similar presentations
Space-Charge Instabilities in Linacs. What limits the beam current in ion linacs? This is a very important topics for anyone designing linacs. For example,
Advertisements

HLAB MEETING -- Paper -- T.Gogami 30Apr2013. Experiments with magnets (e,eK + ) reaction.
1 MICE Beamline: Plans for initial commissioning. Kevin Tilley, 16 th November. - 75days until commissioning Target, detectors, particle production Upstream.
M. LindroosNUFACT06 School Accelerator Physics Transverse motion Mats Lindroos.
1 EMCal & PID Rikard Sandström Universite de Geneve MICE collaboration meeting 26/6-05.
TOF0 calibration The resolution in a given pixel can be measured before the absolute time calibration (see the plot) The expected total resolution of the.
1 PID, emittance and cooling measurement Rikard Sandström University of Geneva MICE Analysis phone conference.
M. Bonesini - VC TOF status M. Bonesini Sezione INFN Milano Bicocca.
Emittance–momentum matrix1 Demonstrating the emittance-momentum matrix Mark Rayner, MICE Video Conference, 21 January Initial 4D.
SLIDE Beam measurements using the MICE TOF counters Analysis meeting, 23 September 2008 Mark Rayner.
1 Downstream PID update Rikard Sandström PID phone conference
TJR Sept 22, 2004MICE Beamline Analysis -- SEPT041 MICE Beamline Analysis – SEPT04 Tom Roberts Muons, Inc. September 22, 2004.
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.
1 PID status MICE Analysis phone conference Rikard Sandström.
CM23 Harbin January 2009TOF Reconstruction1 TOF reconstruction Mark Rayner CM23 Harbin.
Beam line characterization with the TOFs1 Demonstrating the emittance-momentum matrix Mark Rayner, CM26 California, 24 March Initial.
Simulated real beam into simulated MICE1 Mark Rayner CM26.
Wilson Lab Tour Guide Orientation 11 December 2006 CLASSE 1 Focusing and Bending Wilson Lab Tour Guide Orientation M. Forster Mike Forster 11 December.
Y. Karadzhov MICE Video Conference Thu April 9 Slide 1 Absolute Time Calibration Method General description of the TOF DAQ setup For the TOF Data Acquisition.
Analysis Meeting 27 Jan 09Beam Characterization with TOFs1 Beam Characterization with the TOFs Mark Rayner.
Analysis mtng. 29 th April 2008Measuring pz using the KEKSlide 1 TOF momentum reconstruction for the KEK data Analysis meeting, 15 April 2005 Mark.
1 G4MICE Analysis of KEK Test Beam Aron Fish Malcolm Ellis CM15 10th June 2006.
CM23 Harbin January 2009TOF Emittance Measurement1 Beam Characterization with the TOFs Mark Rayner CM23 Harbin.
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.
Lattice calculations: Lattices Tune Calculations Dispersion Momentum Compaction Chromaticity Sextupoles Rende Steerenberg (BE/OP) 17 January 2012 Rende.
1 EMCal design MICE collaboration meeting Fermilab Rikard Sandström.
Critical Issues for MICE Chris Rogers MICE CM 15.
1 M. Bonesini - CM 25 RAL 5/11/09 PID status report M. Bonesini Sezione INFN Milano Bicocca.
Zhihong Ye Hampton University Feb. 16 th 2010, APS Meeting, Washington DC Data Analysis Strategy to Obtain High Precision Missing Mass Spectra For E
What’s the object(ive) of tracking? some things: – hits, wires, clusters, track segments, tracks, trajectories, outer detector matching hits, ….. some.
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.
Quadrupole Transverse Beam Optics Chris Rogers 2 June 05.
Yichao Jing 11/11/2010. Outline Introduction Linear lattice design and basic parameters Combined function magnets study and feasibility Nonlinear dynamics.
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.
Results from Step I of MICE D Adey 2013 International Workshop on Neutrino Factories, Super-beams and Beta- beams Working Group 3 – Accelerator Topics.
DE/dx measurement with Phobos Si-pad detectors - very first impressions (H.P Oct )
Jin Huang M.I.T. Hall A Analysis Workshop Dec 14, JLab.
MICE Step 1: First Emittance Results with Particle Physics Detectors Linda R. Coney EuCARD Meeting – 10 May 2011.
Simulation of direct space charge in Booster by using MAD program Y.Alexahin, A.Drozhdin, N.Kazarinov.
BigCal Reconstruction and Elastic Event Selection for GEp-III Andrew Puckett, MIT on behalf of the GEp-III Collaboration.
Mark Rayner 14/8/08Analysis Meeting: Emittance measurement using the TOFs 1 Emittance measurement using the TOFs The question: can we use position measurements.
11 Nov 2008PC Analysis PC Schedule 2008 Tuesdays fortnightly 9 September  23 September  2 October  CM22  11 November  25 November 9 December.
Alexander Molodozhentsev KEK for MR-commissioning group September 20, 2005 for RCS-MR commissioning group September 27, 2005 Sextupole effect for MR -
Frank L. H. WolfsDepartment of Physics and Astronomy, University of Rochester Status of the TOF February 22, 2001 Straight-line tracking What have we learned?
PID simulations Rikard Sandström University of Geneva MICE collaboration meeting RAL.
HES HKS collaboration meeting 3/11/2010 T.Gogami.
Tuesday, 02 September 2008FFAG08, Manchester Stephan I. Tzenov1 Modeling the EMMA Lattice Stephan I. Tzenov and Bruno D. Muratori STFC Daresbury Laboratory,
Timing measurements at the MICE experiment – 1 The analysis of timing measurements at the Muon Ionization Cooling Experiment Mark Rayner The University.
By Verena Kain CERN BE-OP. In the next three lectures we will have a look at the different components of a synchrotron. Today: Controlling particle trajectories.
Lecture 4 - E. Wilson - 23 Oct 2014 –- Slide 1 Lecture 4 - Transverse Optics II ACCELERATOR PHYSICS MT 2014 E. J. N. Wilson.
Analysis meeting: Beam momentum measurements using TOFs Tuesday, 22 January 2008 Slide 1 of 10 Beam momentum measurement using.
18 th March 2008Measuring momentum using the TOFsSlide 1 Measuring momentum using TOF0 and TOF1 Progress report Mark Rayner (Oxford/RAL) Analysis Meeting,
TOF Emittance Pion Emittance Measurement with the TOFs? Mark Rayner 11 December 2008.
Mark Rayner – Analysis SessionCM25, 4 November Beam characterization by the TOFs Mark Rayner The University of Oxford MICE CM25.
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. apollonio 7/7/2010CM27 - RAL11 Beam-Line Analysis …
Lecture 4 - E. Wilson –- Slide 1 Lecture 4 - Transverse Optics II ACCELERATOR PHYSICS MT 2009 E. J. N. Wilson.
Monte Carlo simulation of the particle identification (PID) system of the Muon Ionization Cooling Experiment (MICE) Mice is mainly an accelerator physics.
Mark Rayner – Analysis SessionCM25, 4 November The TOF detectors: Beyond particle identification Mark Rayner The University of Oxford MICE CM25.
TOF Emittance Emittance measurements with the TOFs Mark Rayner 4 December 2008.
MICE Beamline Status m. apollonio 17 December 2009 MICE VC
Step 1 Analysis: Progress Towards the Emittance Paper
Parametric Resonance Ionization Cooling of Muons
Lecture 4 - Transverse Optics II
TOF Software and Analysis Tools
The time-of-flight reconstruction & calibration
Lecture 4 - Transverse Optics II
Lecture 4 - Transverse Optics II
Presentation transcript:

5 May 2009MICE Analysis - MR1 The December Shifts: Beam Characterization by the Time of Flight System Mark Rayner

5 May 2009MICE Analysis - MR2 ALL: calibrate SURVIVORS: characterize the beam

5 May 2009MICE Analysis - MR3 Characterization of the December beam trace space momentum spectrum of the beam emittance alpha beta gamma fit quantities interesting to beam line people time of flight transverse position at TOF0 and TOF1 TOFs measure momentum track calibrated Problem: Small number of particles means only the central pixels have been calibrated well, but the position measurement is essential to the emittance measurement  We must attempt to calibrate all pixels of TOF0 and TOF1  Basic method from Harbin CM (no time-walk, ignores trigger intricacies): today’s data  Time-walk + simplified cable length correction: in development, problems remain PID

5 May 2009MICE Analysis - MR4 TDC cabling of TOF0 and TOF1 Except TOF0 outer slabs (0 and 9 in both planes)  TDC board NS 021 B T Beam PMT number 0  TDC board 0 PMT number 1  TDC board 1 Plane 0Plane 1 Can compare S and B and N and T without worrying about the trigger

5 May 2009MICE Analysis - MR5 Simplified Cable Length Calibration sums over: (TDC S slab i) – (TDC B slab j) – linear correction n S0 n S6 0 0 n B0 n B6 0 0 n ij n ij T vector of cable length corrections = Depends only on number of hits per pixel Depends only on number of hits per PMT Write down everything we know per TDC board Form a matrix equation Minimize chi-square  One number per PMT  A best-guess calibration for every PMT with a hit Problem Too many zero entries Determinant = 0  Refining method

5 May 2009MICE Analysis - MR6 Trace Space Reconstruction Focusing transfer matrixDefocusing transfer matrix Effective length l [m] Central quadrupole gradient [T/m] MeV/c Defocusing Focusing Effective phase advance  [radians] Central quadrupole gradient [T/m] MeV/c Effective focusing strength k [m -2 ] Central quadrupole gradient [T/m] MeV/c

5 May 2009MICE Analysis - MR7

5 May 2009MICE Analysis - MR8 Emittance measurement ??? Horiz TOF0 Vert TOF0 Horiz TOF1 Vert TOF1