Geant Simulation of Muon Cooling Rings

Slides:



Advertisements
Similar presentations
PID Detector Size & Acceptance Chris Rogers Analysis PC
Advertisements

FODO-based Quadrupole Cooling Channel M. Berz, D. Errede, C. Johnstone, K. Makino, Dave Neuffer, Andy Van Ginneken.
Bunched-Beam Phase Rotation- Variation and 0ptimization David Neuffer, A. Poklonskiy Fermilab.
V.Daniel Elvira Status Report on Cooling Simulations using GEANT4 Motivation: Explore a realistic design of a 44/88 MHz based cooling channel for a -factory.
1 Downstream scraping and detector sizes Rikard Sandström University of Geneva MICE collaboration meeting CERN.
Μ-Capture, Energy Rotation, Cooling and High-pressure Cavities David Neuffer Fermilab.
PID Detector Size & Acceptance Chris Rogers Analysis PC
Kirk McDonald Monday, 28th May Report of the International Working Group on Muon Beamlines Bruno Autin, Roberto Cappi, Rob Edgecock, Kirk McDonald,
V.Daniel Elvira Status Report on Cooling Simulations using GEANT4 Motivation: Explore a realistic design of a 44/88 MHz based cooling channel for a -factory.
Chris Rogers, MICE CM16 Wednesday Plenary Progress in Cooling Channel Simulation.
Beamline-to-MICE Matching Ulisse Bravar University of Oxford 2 August 2004 MICE performance with ideal Gaussian beam JUNE04 beam from ISIS beamline (Kevin.
1 PID Detector Size & Acceptance Chris Rogers Analysis PC
WIN'05, June A. Klier - Muon Collider Physics1 Physics at a Future Muon Collider Amit Klier University of California, Riverside WIN’05 – Delphi,
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.
Helical Cooling Channel Simulation with ICOOL and G4BL K. Yonehara Muon collider meeting, Miami Dec. 13, 2004 Slide 1.
Chris Rogers, Analysis Parallel, MICE CM17 Progress in Cooling Channel Simulation.
1 Chris Rogers MICE Collaboration Meeting 11th Feb 2005 Tracking and Cooling performance of G4MICE.
FFAG Concepts and Studies David Neuffer Fermilab.
1 Front End Capture/Phase Rotation & Cooling Studies David Neuffer Cary Yoshikawa December 2008.
June 21, 2005 S. Kahn -- Small Muon Cooling Ring1 Small Muon Ring for a Cooling Demonstration Steve Kahn For S. Kahn, H. Kirk, A. Garren, F. Mills and.
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.
Storage Ring : Status, Issues and Plans C Johnstone, FNAL and G H Rees, RAL.
FFAG-ERIT Accelerator (NEDO project) 17/04/07 Kota Okabe (Fukui Univ.) for FFAG-DDS group.
Particle Production in the MICE Beam Line Particle Accelerator Conference, May 2009, Vancouver, Canada Particle Production in the MICE Beam Line Jean-Sebastien.
2002/7/02 College, London Muon Phase Rotation at PRISM FFAG Akira SATO Osaka University.
2002/7/04 College, London Beam Dynamics Studies of FFAG Akira SATO Osaka University.
Results from Step I of MICE D Adey 2013 International Workshop on Neutrino Factories, Super-beams and Beta- beams Working Group 3 – Accelerator Topics.
Magnet Issues Steve Kahn OleMiss Workshop Mar 11, 2004.
Quantitative Optimisation Studies of the Muon Front-End for a Neutrino Factory S. J. Brooks, RAL, Chilton, Oxfordshire, U.K. Tracking Code Non-linearised.
Bunched-Beam Phase Rotation for a Neutrino Factory David Neuffer Fermilab.
Forum March 2003H.Taureg1 Magnetic Fields in ALICE Mapping and Monitoring.
Calculation of the beam dynamics of RIKEN AVF Cyclotron E.E. Perepelkin JINR, Dubna 4 March 2008.
1 EPIC SIMULATIONS V.S. Morozov, Y.S. Derbenev Thomas Jefferson National Accelerator Facility A. Afanasev Hampton University R.P. Johnson Muons, Inc. Operated.
Muon cooling with Li lenses and high field solenoids V. Balbekov, MAP Winter Meeting 02/28-03/04, 2011 OUTLINE  Introduction: why the combination of Li.
V.Balbekov, 12/09/08 HCC simulation with wedge absorbers V. Balbekov, Fermilab Muon Collider Design Workshop December 8-12, 2008 JeffersonLab, Newport.
-Factory Front End Phase Rotation Gas-filled rf David Neuffer Fermilab Muons, Inc.
1 Advances for a Solenoid/Dipole 6D Cooling Ring X. Ding, UCLA Muon Accelerator Program-Winter Meeting Jefferson Lab 3/1/11.
Harold G. Kirk Brookhaven National Laboratory Progress in Quad Ring Coolers Ring Cooler Workshop UCLA March 7-8, 2002.
S. Kahn 5 June 2003NuFact03 Tetra Cooling RingPage 1 Tetra Cooling Ring Steve Kahn For V. Balbekov, R. Fernow, S. Kahn, R. Raja, Z. Usubov.
RAL Muon Beam Line Properties. ISIS 70 MeV H- injection Ring accelerates up to 800 MeV in about 10 ms 50 Hz cycle - Dual Harmonic System ~ 2 x 1.5 MHz;
WG3 Summary (Achievements in 2005) 28 Talks & 5 focus sessions 17 talks &2 focus sessions in this talk 12 taks & 3 focus sessions by H. Kirk.
MCTF Andreas Jansson MUTAC Meeting 8-10 April MCTF EXPERIMENTAL ACTIVITES - towards demonstrating 6D cooling.
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 PID Detector Size & Acceptance Chris Rogers Analysis PC
FFAG Acceleration David Neuffer Fermilab FFAG Workshop ‘03.
2 July 2002Realistic Fields for a Ring Cooler Magnet System -- S.Kahn Page 1 Realistic Fields for a Ring Cooler Steve Kahn 2 July 2002 NuFact’02 Meeting.
Simulating the RFOFO Ring with Geant Amit Klier University of California, Riverside Muon Collaboration Meeting Riverside, January 2004.
1 6D Cooling with a Rectilinear FOFO Channel Diktys Stratakis Brookhaven National Laboratory AAC Group Meeting July 18, 2013.
Harold G. Kirk Brookhaven National Laboratory Quad/dipole Ring Coolers * Nufact’03 Columbia University June 6, 2003 * With contributions from A. Garren.
Nufact02, London, July 1-6, 2002K.Hanke Muon Phase Rotation and Cooling: Simulation Work at CERN new 88 MHz front-end update on cooling experiment simulations.
28-Aug-2003 Steve Kahn Standardized MucGeant I/O Front End to MucGeant Standardize the input files for MucGeant: –The input should be in the ICOOL for003/4.
2 nd Muon Collider Design workshop, JLab, Newport News VA December 8-12, 2008 Helical FOFO Snake Simulations Y. Alexahin (FNAL)
Neutrino Factory & Muon Collider Collaboration meeting, LBL January 25-28, 2009 Helical FOFO Snake Simulations Y. Alexahin (FNAL)
Bunched-Beam Phase Rotation - Ring Coolers? - FFAGs? David Neuffer Fermilab.
1 Tracking study of muon acceleration with FFAGs S. Machida RAL/ASTeC 6 December, ffag/machida_ ppt.
Harold G. Kirk Brookhaven National Laboratory Rings with 400 and 800 MHz RF Ring Cooler Meeting Oxford, Ms. March 11-12, 2004.
1 Front End – gas-filled cavities David Neuffer May 19, 2015.
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.
Operated by JSA for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Alex Bogacz IDS- NF Acceleration Meeting, Jefferson Lab,
Research and development toward a future Muon Collider Katsuya Yonehara Accelerator Physics Center, Fermilab On behalf of Muon Accelerator Program Draft.
1 6D Cooling Chris Rogers, ASTeC-STFC Topical Workshop 23 Oct 2007.
Uncertainties in Cooling Simulations R.C. Fernow BNL Synergy Workshop FNAL 13 June 2008.
Uses of the HCC Mary Anne Cummings February 4, 2009 Fermilab AAC
+-- Collider Front end- Balbekov version
Parametric Resonance Ionization Cooling of Muons
M. Migliorati, C. Vaccarezza INFN - LNF
Design of the MANX experiment
An Anticyclotron For Cooling Muons
Uses of the HCC Mary Anne Cummings February 4, 2009 Fermilab AAC
Presentation transcript:

Geant Simulation of Muon Cooling Rings Amit Klier University of California Riverside

A. Klier - Geant simulation Outline A short reminder from Nufact03 The RFOFO ring Geometry Software improvements Simulation results The small dipole ring Some Results June 21 2005 A. Klier - Geant simulation

A. Klier - Geant simulation Muc_Geant Modified, data-driven Geant3 application for simulating muon cooling Electric fields added Runge-Kutta changed to include changing electric fields (eg RF cavities) Realistic magnetic fields can be read from external field maps June 21 2005 A. Klier - Geant simulation

From Nuact03 Tetra ring simulated Rajendran Raja – Nufact 03 June 21 2005 A. Klier - Geant simulation

A. Klier - Geant simulation The RFOFO ring A few code changes w.r.t. Tetra Realistic magnetic field maps read-in (R. Godang, S. Bracker – MC-Note 271) June 21 2005 A. Klier - Geant simulation

A. Klier - Geant simulation The RFOFO ring Full Geant simulation: A. Klier – MC-Note 298 June 21 2005 A. Klier - Geant simulation

A. Klier - Geant simulation The ring geometry 33 m circumference 12 cells (2.75m): A wedge absorber opening angle 110°, pointing ’upwards’ 6 RF cavities 28.75 cm long, iris radius 25 cm flat E field in z direction 2 tilted solenoids inner/outer r = 77/88 cm tilt angle ±3° Only for display here June 21 2005 A. Klier - Geant simulation

Closed orbits in a single cell Solid line – the reference orbit 200 MeV 270 MeV 227 MeV 250 MeV 227 MeV 250 MeV E = 200 MeV E = 270 MeV June 21 2005 A. Klier - Geant simulation

Software improvements ICOOL input/output format used, ecalc9 can be used to calculate emittance Use initial time of particle at entry Use virtual detectors June 21 2005 A. Klier - Geant simulation

A. Klier - Geant simulation Cooling of a muon beam June 21 2005 A. Klier - Geant simulation

A. Klier - Geant simulation Comparison with ICOOL Transmission 6-D emittance June 21 2005 A. Klier - Geant simulation

A. Klier - Geant simulation More comparisons Results after 10 turns: Merit factor Trans. W/O decay With decay Merit Factor Balbekov (MC-264) 70% 56% 55 ICOOL (Fernow) -- 58% 66 Geant 72% 57% 70 June 21 2005 A. Klier - Geant simulation

Change beam entry angle June 21 2005 A. Klier - Geant simulation

A. Klier - Geant simulation The small dipole ring “Weak” (edge) focusing (ideally) scaling Filled with ~10 Atm. hydrogen gas @ 77K Dipole field ~ 2 T For P~200 MeV/c, the radius should be ~60 cm June 21 2005 A. Klier - Geant simulation

A. Klier - Geant simulation Field map (from S. Kahn) By in a single quadrant By at R=60 cm Return yoke June 21 2005 A. Klier - Geant simulation

A. Klier - Geant simulation Reference orbit Scale B down to 90% closed orbit: P=171.25 MeV/c Rmin=56.32 cm (x=0 in virtual detectors) Rmin Virtual detector plane RF cavity (active region) June 21 2005 A. Klier - Geant simulation

A. Klier - Geant simulation Ellipses Stable up to y~13 cm Y plane symmetry imposed June 21 2005 A. Klier - Geant simulation

A. Klier - Geant simulation Acceptance of the ring “A blob” Py=~19 MeV/c y=~8.5 cm Px=~34 MeV/c More “natural” decrease with no x-z plane symmetry x=~6.5 cm June 21 2005 A. Klier - Geant simulation

“Cooling” with no scattering Xinitial=6 cm Yinitial=8 cm tinitial= –1.5 ns Xcentral=0.04 cm Ycentral=0 cm tcentral=0 ns PXinitial=30 MeV/c PYinitial=17.5 MeV/c Einitial=213 MeV PXcentral=0.12 MeV/c PYcentral=0 MeV/c Ecentral=201.8 MeV June 21 2005 A. Klier - Geant simulation

Software improvements More flexibility – less “hard-coding”, more external parameters Field map reading code used to be RFOFO-specific, now more general More RF parameters Cavities in small dipole ring are off-center So far, only perfect pillbox (or flat field..) cavity are simulated Flexibility: different frequencies, gradients, types can be used in the same channel June 21 2005 A. Klier - Geant simulation

A. Klier - Geant simulation To do Simulate the small dipole ring with a beam Introduce more realistic features: Injection Detectors June 21 2005 A. Klier - Geant simulation

A. Klier - Geant simulation June 21 2005 A. Klier - Geant simulation

A. Klier - Geant simulation Additional Slides June 21 2005 A. Klier - Geant simulation

A. Klier - Geant simulation Comparison with ICOOL Transverse emittance Longitudinal emittance June 21 2005 A. Klier - Geant simulation