How to use it? Basically, given a fieldmap for an RF structure, the time-dependent fields are E(x,y,z,t) = maxGradient * Eo(x,y,z) * sin(ω(t – timeOffset))

Slides:



Advertisements
Similar presentations
Nominal and no CSR (R 56-1 = 55 mm, R 56-2 = 59 mm, R 56-3 = 0) L1 phase = 21 deg, V 3.9 = 55 MV CSR OFF BC3 OFF Elegant Tracking  z1 = mm (post.
Advertisements

RF Bucket Area Introduction Intense muon beams have many potential applications, including neutrino factories and muon colliders. However, muons are produced.
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 PID status MICE Analysis phone conference Rikard Sandström.
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 Simulation of RF background in MICE Rikard Sandström University of Geneva NuFact’04 Osaka.
Chris Rogers, MICE CM16 Wednesday Plenary Progress in Cooling Channel Simulation.
TJR 11/03/2003Slide 1 g4beamline A “Swiss Army Knife” for Geant4 Tom Roberts Illinois Institute of Technology.
RF background simulations MICE collaboration meeting Fermilab Rikard Sandström.
Helical Cooling Channel Simulation with ICOOL and G4BL K. Yonehara Muon collider meeting, Miami Dec. 13, 2004 Slide 1.
1 RF background simulation: proposal for baseline simulation Video conference 22/9 -04 Rikard Sandström Geneva University.
Eric Prebys, FNAL.  We consider motion of particles either through a linear structure or in a circular ring USPAS, Knoxville, TN, Jan , 2014 Lecture.
Eric Prebys, FNAL.  As you’ll show in homework, the synchrotron tune (longitudinal oscillations/turn) is generally
ABSTRACT The International Design Study for the Neutrino Factory (IDS- NF) baseline design 1 involves a complex chain of accelerators including a single-pass.
Field and Phase Error Studies in Normal Conducting Structures LLRF and Beam Dynamics in Hadron Linacs – EuCARD2 Workshop Ciprian Plostinar
Design Concepts for Magnetic Insulation Diktys Stratakis Advanced Accelerator Group Brookhaven National Laboratory NFMCC Meeting – LBL January 28, 2009.
MICE pencil beam raster scan simulation study Andreas Jansson.
1 Front End – present status David Neuffer March 31, 2015.
Ajit Kurup, C. Bontoiu, M. Aslaninejad, J. Pozimski, Imperial College London. A.Bogacz, V. S. Morozov, Y.R. Roblin Jefferson Laboratory K. B. Beard, Muons,
The 2010 NFMCC Collaboration Meeting University of Mississippi, January 13-16, Update on Parametric-resonance Ionization Cooling (PIC) V.S. Morozov.
Tracking at LHCb Introduction: Tracking Performance at LHCb Kalman Filter Technique Speed Optimization Status & Plans.
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.
Particle dynamics in electron FFAG Shinji Machida KEK FFAG04, October 13-16, 2004.
Feb 10, 2005 S. Kahn -- Pid Detectors in G4MicePage 1 Pid Detector Implementation in G4Mice Steve Kahn Brookhaven National Lab 10 Feb 2005.
A 3 Pass, Dog-bone Cooling Channel G H Rees, ASTeC, RAL.
Operated by JSA for the U.S. Department of Energy Muons, Inc. Winter MAP Mtg, Mar. 2 nd, 2011 Pre-Linac simulations in G4beamline Kevin B. Beard Muons,Inc.
Thomas Jefferson National Accelerator Facility Page 1 Muons, Inc. Epicyclic Helical Channels for Parametric-resonance Ionization Cooling Andrei Afanasev,
TJR 01/21/2003Slide 1 Simulations of the Study 2 Cooling Channel with Realistic Absorber Windows Tom Roberts Illinois Institute of Technology.
1 EPIC SIMULATIONS V.S. Morozov, Y.S. Derbenev Thomas Jefferson National Accelerator Facility A. Afanasev Hampton University R.P. Johnson Muons, Inc. Operated.
New G4beamline pillbox improvements K.B.Beard 4/26/2011.
Design of an Isochronous FFAG Ring for Acceleration of Muons G.H. Rees RAL, UK.
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;
Recent progress of RF cavity study at Mucool Test Area Katsuya Yonehara APC, Fermilab 1.
6-D dynamics in an isochronous FFAG lattice e-model Main topic : Tracking code development : 3-D simulation of the field in an isochronous FFAG optics.
FFAG Studies at RAL G H Rees. FFAG Designs at RAL Hz, 4 MW, 3-10 GeV, Proton Driver (NFFAGI) Hz,1 MW, GeV, ISIS Upgrade (NFFAG) 3.
Muons, Inc. TJR NuFact06 August 28, 2006G4BeamlineSlide 1 G4Beamline A “Swiss Army Knife” for Geant4 Tom Roberts Muons,
 A model of beam line built with G4Beamline (scripting tool for GEANT4)  Simulated performance downstream of the AC Dipole for core of beam using  x.
Eric Prebys, FNAL.  We consider motion of particles either through a linear structure or in a circular ring USPAS, Hampton, VA, Jan , 2015 Longitudinal.
Simulating the RFOFO Ring with Geant Amit Klier University of California, Riverside Muon Collaboration Meeting Riverside, January 2004.
Energy recovery linacs for commercial radioisotope production A. Sy, G. Krafft, V. S. Morozov, R. P. Johnson, T. Roberts, C. Boulware, J. Hollister May.
Multi-bunch acceleration in NS-FFAG Takeichiro Yokoi (Oxford University)
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.
Operated by JSA for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Alex Bogacz 1 Status of Baseline Linac and RLAs Design.
Basic of muon ionization cooling K. Yonehara 8/29/11HPRF cavity physics seminar - I, K. Yonehara1.
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.
Dark Current in ILC Main Linac N.Solyak, A.Sukhanov, I.Tropin ALCW2015, Apr.23, 2015, KEK LCWS'15, Tsukuba, 04/2015Nikolay Solyak1.
Operated by JSA for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Alex Bogacz NuFact’08, Valencia, Spain, July 4, 2008 Acceleration.
Operated by JSA for the U.S. Department of Energy Thomas Jefferson National Accelerator Facility Alex Bogacz 1 Recirculating Linac Acceleration  End-to-end.
Muons, Inc. Modeling the Upper, Middle, & Lower NF linac in G4beamline Kevin B. Beard, Muons,Inc. & Alex Bogacz, Jefferson Lab LEMC2009 workshop 8-12 Jun.
Progress on the Linac and RLAs
Parametric Resonance Ionization Cooling of Muons
M. Migliorati, C. Vaccarezza INFN - LNF
Modeling the Upper, Middle, & Lower
Modeling the Upper, Middle, & Lower
Modeling the Upper, Middle, & Lower
Effects of External Fields on RF Cavity Operation
Physics Processes Missing from our Current Simulation Tools
Muon RLA - Design Status and Simulations
Muon RLA - Design Status and New Options
K.B. Beard1#, S.A. Bogacz2, V.S. Morozov2, Y.R. Roblin2
Progress on the Linac and RLAs
6-D dynamics in an isochronous FFAG lattice e-model
RLA WITH NON-SCALING FFAG ARCS
Pre-Linac simulations in G4beamline Alex Bogacz & Yves Roblin
Accelerator Physics Particle Acceleration
Muon RLA - Design Status and New Options
Accelerator Physics Particle Acceleration
Accelerator Physics G. A. Krafft, A. Bogacz, and H. Sayed
Presentation transcript:

How to use it? Basically, given a fieldmap for an RF structure, the time-dependent fields are E(x,y,z,t) = maxGradient * Eo(x,y,z) * sin(ω(t – timeOffset)) B(x,y,z,t) = maxGradient * Bo(x,y,z) * -cos(ω(t – timeOffset)) timeOffset contains the RF phase phaseAcc. If two of three (timeOffset or phaseAcc, maxGradient, and a fixed output) are specified, pillbox will determine the missing quantities, if possible. An overdefined system is reported as an error. The timingMethod specifies how to find timeOffset; the default is atZ (set time of arrival) to emulate the old pillbox, while maxE (find maximum energy gain) is more typical of how cavities are actually timed. For example, an RF cavity might follow an absorber in a cooling channel with a maximum peak field, and so be asked to find the appropriate phase: pillbox RF1 … maxGradient=20 timingMethod=maxE fixMomentum=200 or given the phase to find the appropriate voltage pillbox RF2 … timingMethod=maxE fixMomentum=200 phaseAcc=45 or the phase and voltage could be set, and 0 o RF determined pillbox RF3 … timingMethod=maxE maxGradient=20 phaseAcc=45 or fix everything pillbox RF4 … maxGradient=20 timeOffset= Note that the fixed value is at the atZlocal location, not necessarily the exit. IMPROVEMENTS TO THE G4BEAMLINE PILLBOX * * K.B. Beard 1#, S.A. Bogacz 2, V.S. Morozov 2, T.J. Roberts 1, Y.R. Rob lin 2 1 Muons Inc, 2 Jefferson Lab What was changed? Basically, the pillbox was rewritten with new options, but is 100% compatible with previous versions except that phaseAcc no longer defaults to 40 o (50 o before crest for a positive particle). G4beamline defines 0 o to be the zero crossing on the rising slope of the E field. New options: timingMethod Method for determining the nominal timeOffset {atZ, maxE, noE, minE, maxT, nomT, minT, maxX, noX, minX, maxY, noY, minY}. timingAtZ Local Z location for timing (mm). fixMomentum Specify total output momentum (MeV/c). fixEnergyGain Specify energy gain (MeV). fixTransitTime Specify transit time (ns). fixXdeflection Specify local output XZ angle (deg). fixYdeflection Specify local output YZ angle (deg). fixTolerance Specify allowable error on fixed settings [1.e-3]. timingDisplay Set nonzero to show timing volume and print info messages References [1] [2] Thomas J. Roberts et al., G4Beamline particle tracking in matter-dominated beam lines. In Proceedings of EPAC08, Genoa, Italy [484]. [3] Geant4 – Muons, Inc. Acknowledgements *Supported in part by US DOE STTR Grant DE-FG02-08ER m ABSTRACT G4beamline 1,2 is a powerful, flexible, user-friendly, and OpenSource tool for using the Geant4 library 3 to simulate many systems of interest. In particular, it has an many enhancements to aid in the modelling of particle accelerators. Its pillbox, used to model an RF cavity, is being extended to allow it to model multi-cell and transverse-mode cavities and to allow better tuning of those structures. Why? The old pillbox didn’t: handle multicavity structures gracefully phase particles with β<<1 very well. phase deflecting cavities at all locally adjust gradients A pillbox is a roughly cylindrical container – the RF fields are inside the container. The timingVolume is just a region within the pillbox used to determine the timing of the RF, if needed. It usually extends from the entrance of the pillbox to either the center (timingMethod=atZ) or to the exit all other methods). time of arrival min Y deflection max energy gain ; logic flow