Summary of my work in September and my plan What I have done and my status –Finished programming and fixed some bugs of the preliminary version of the.

Slides:



Advertisements
Similar presentations
Debugging ACL Scripts.
Advertisements

Update on ILC ML Lattice Design Alexander Valishev, for the FNAL LET group FNAL AP Dept. Meeting March 7, 2007.
Assistive Technology Training Online (ATTO) University at Buffalo – The State University of New York USDE# H324M Co:Writer.
1 Collimation Simulations and Optimisation Frank Jackson ASTeC, Daresbury Laboratory.
BDS Change Request: Support of Single L* Optics Configuration Shared by both Detectors Glen White, Nick Walker Sept MDI/CFS Ichinoseki.
Flash Animation Using Linear Transformations By Kevin Hunter Kevin Hunter Marcus Yu Marcus Yu.
LCSC - 01 Monte Carlo Simulation of Radiation Transport, for Stereotactic Radio Surgery Per Kjäll Elekta Instrument AB
Introduction to Molecular Orbitals
Peyman Mostaghimi, Martin Blunt, Branko Bijeljic 11 th January 2010, Pore-scale project meeting Direct Numerical Simulation of Transport Phenomena on Pore-space.
Transport formalism Taylor map: Third order Linear matrix elementsSecond order matrix elements Truncated maps Violation of the symplectic condition !
Motion Analysis (contd.) Slides are from RPI Registration Class.
CSI 101 Elements of Computing Spring 2009 Lecture #2 Development Life Cycle of a Computer Application Monday January 26th, 2009.
Project Time Management
CS 1400 Using Microsoft Visual Studio 2005 if you don’t have the appropriate appendix.
Programming. Software is made by programmers Computers need all kinds of software, from operating systems to applications People learn how to tell the.
Update on ILC ML Lattice Design Alexander Valishev, for the FNAL LET group FNAL AP Dept. Meeting March 7, 2007.
Ground Motion + Vibration Transfer Function for Final QD0/SD0 Cryomodule System at ILC Glen White, SLAC ALCPG11, Eugene March 21, 2011.
DESY GDE Meeting Global Design Effort 1 / 14 LET Work at SLAC and Plans for the Future PT SLAC.
Programming. What is a Program ? Sets of instructions that get the computer to do something Instructions are translated, eventually, to machine language.
IV. Sensitivity Analysis for Initial Model 1. Sensitivities and how are they calculated 2. Fit-independent sensitivity-analysis statistics 3. Scaled sensitivities.
ATF2 Javier Resta Lopez (JAI, Oxford University) for the FONT project group 5th ATF2 project meeting, KEK December 19-21, 2007.
Trajectory Correction and Tuning James Jones Anthony Scarfe.
Smoothed Particle Hydrodynamics (SPH) Fluid dynamics The fluid is represented by a particle system Some particle properties are determined by taking an.
A Brief Introduction of SAD for ATF2 Flight Simulator S.Kuroda(KEK) mini work shop for flight simulator(LAL)2008.
Particle dynamics in electron FFAG Shinji Machida KEK FFAG04, October 13-16, 2004.
This material is approved for public release. Distribution is limited by the Software Engineering Institute to attendees. Sponsored by the U.S. Department.
STS track recognition by 3D track-following method Gennady Ososkov, A.Airiyan, A.Lebedev, S.Lebedev, E.Litvinenko Laboratory of Information Technologies.
Matching recipe and tracking for the final focus T. Asaka †, J. Resta López ‡ and F. Zimmermann † CERN, Geneve / SPring-8, Japan ‡ CERN, Geneve / University.
Fifth ATF2 Project Meeting, dec. 2007, KEK, Japan Emittance measurements with multiple wire-scanners and quadrupole scans in ATF EXT C. Rimbault,
Quantitative Optimisation Studies of the Muon Front-End for a Neutrino Factory S. J. Brooks, RAL, Chilton, Oxfordshire, U.K. Tracking Code Non-linearised.
September Bound Computation for Adaptive Systems V&V Giampiero Campa September 2008 West Virginia University.
Global Design Effort 1 Possible Minimum Machine Studies of Central Region for 2009 Reference, ILC Minimum Machine Study Proposal V1, January 2009 ILC-EDMS.
Serge Andrianov Theory of Symplectic Formalism for Spin-Orbit Tracking Institute for Nuclear Physics Forschungszentrum Juelich Saint-Petersburg State University,
1 MAUS Optics Clean up Peter Lane Illinois Institute of Technology MICE Collaboration Meeting 32 9 Feb 2012.
Global Design Effort - CFS ILC Accelerator Design and Integration Meeting 1 ILC AD&I MEETING CONVENTIONAL FACILITIES AND SITING GROUP UPDATE V.
ME451 Kinematics and Dynamics of Machine Systems Review of Differential Calculus 2.5, 2.6 September 11, 2013 Radu Serban University of Wisconsin-Madison.
Rough Estimation of energy spread produced in Final Focus line and effects to chromatic correction in ILC and ATF minor change Kiyoshi.
Final Presentation Avilés-Angélica, Blanco-Alberto, Fuentes-Alba, Pell-Xavier, Schenini-Juan, Talukder-Nurul.
J-PARC Trace3D Upgrades Christopher K. Allen Los Alamos National Laboratory.
BAR ELEMENT IN 2D (TRUSS, LINK)
CSC 4700 Software Engineering
Wake Fest 07 - ILC wakefield workshop at SLAC Dec , 2007 Shilun Pei with Chris Adolphsen, Zenghai Li, Karl L. Bane, et al. SLAC, Dec. 12, 2007 TTF.
ILC Main Linac Alignment Simulations John Dale 2009 Linear Collider Workshop of the Americas.
Beam Dynamics WG K. Kubo, N. Solyak, D. Schulte. Presentations –N. Solyak Coupler kick simulations update –N. Solyak CLIC BPM –A. Latina: Update on the.
Chapter 6Java: an Introduction to Computer Science & Programming - Walter Savitch 1 Chapter 6 l Array Basics l Arrays in Classes and Methods l Programming.
Coupler Short-Range Wakefield Kicks Karl Bane and Igor Zagorodnov Wake Fest 07, 11 December 2007 Thanks to M. Dohlus; and to Z. Li, and other participants.
Simulations - Beam dynamics in low emittance transport (LET: From the exit of Damping Ring) K. Kubo
Emittance measurements with multiple wire-scanners and quadrupole scans in ATF EXT C. Rimbault, Brossard, P. Bambade (LAL) Main goal : - Try to improve.
P2P storage trading system (A preliminary idea) Presenter: Lin Wing Kai (Kai)
BBFP J. Wei’s Fokker-Planck solver for bunched beams November 21 st, 2007 CLIC Beam dynamics meeting Y. Papaphilippou.
Status of EXT coupling measurement analysis 9 th ATF2 project meeting C.Rimbault (LAL) S. Kuroda, T. Tauchi, N. Terunuma (KEK), G. White, M. Woodley (SLAC)
Adiabatic buncher and (  ) Rotator Exploration & Optimization David Neuffer(FNAL), Alexey Poklonskiy (FNAL, MSU, SPSU)
BDS Status Update Glen White, SLAC July ADI Fuze Meeting.
Extrapolation Techniques  Four different techniques have been used to extrapolate near detector data to the far detector to predict the neutrino energy.
Wakefield effect in ATF2 Kiyoshi Kubo
Questionnaire-Part 2. Translating a questionnaire Quality of the obtained data increases if the questionnaire is presented in the respondents’ own mother.
Frank Stulle, ILC LET Beam Dynamics Meeting CLIC Main Beam RTML - Overview - Comparison to ILC RTML - Status / Outlook.
From Beam Dynamics K. Kubo
ILC DR Lower Horizontal Emittance, preliminary study
Overview of Needs for SixTrack on-line Aperture Check
Benchmarking MAD, SAD and PLACET Characterization and performance of the CLIC Beam Delivery System with MAD, SAD and PLACET T. Asaka† and J. Resta López‡
Update on ILC ML Lattice Design
Ben Cerio Office of Science, SULI Program 2006
Transverse Beam Jitter Propagation in Multi-bunch Operation at ATF2
Accelerator Physics Technical System Group Review
ILC DR instability simulations
6.5 Taylor Series Linearization
Ions in ATF ISG-X June 20th, 2003.
Fitting generalized linear models
Updates on the beam-beam effect in JLEIC
Presentation transcript:

Summary of my work in September and my plan What I have done and my status –Finished programming and fixed some bugs of the preliminary version of the XSIF to SAD Translator, successfully applied the program to the translation of the RTML, Main Linac and BDS lattice deck files. (Presented in the BDS meeting of September 13, 2006) –Made some tracking studies on the ATF2 lattice by using SAD, such as the lattice deck files from version 3.1 to and from version ff3.7.1 to ff –Made some studies on the higher order terms of the transfer matrix, some of the results will be shown later. My plan

Some study results of the higher order terms of the transfer matrix In six dimensional phase space, the change of the coordinate vector X i = (x, x’, y, y’, △ l, δ) is driven by the first order transfer matrix R such that X i out = R ij X j in. The second, third and so on terms are included in a similar manner, X i out = R ij X j in + T ijk X j in X k in + U ijkn X j in X k in X n in + …… In studying the final focus system, it is important to know the higher order terms such as T122, T126, and so on, since some of them have a large effect on the beam size. In SAD, there is no such function to calculate the higher order terms now, so some post process programs need to be written.

Kuroda-san write a simple program to calculate the higher order term T111, which is based on the following method: 1) Track particles with different initial conditions; 2) Fit the results to obtain the higher order term. But, the problem of Kuroda-san calculation is the accuracy, since if I change the initial conditions, different calculation results will be given. For example, for the calculation of T 111, we only change the initial condition of x. When the initial value of x is 1e-4, the fitted value of T 111 is , while when the initial value of x is 1e- 6, the value of T 111 is (Both smaller and larger change of initial conditions will produce wrong results, but the appropriate value of initial condition is difficult to estimate.)

On the basis of Kuroda-san’s program, I also wrote a program to calculate the value of T ijk when i = j = k. In my program, the initial conditions can be changed automatically until a convergence of the calculated T ijk is obtained. But, the calculated value of the T ijk depends on the stop condition of the automatic change of the initial condition, sometimes the calculation may fail. For example, if I set the stop condition to be Abs[Tijk/coeff[3]- 1]=>0.001, the calculated value of T 111 is , while if I set the stop condition to be Abs[Tijk/coeff[3]-1]=>0.0001, the calculation will fail. In addition, using my program to calculate T 111 and T 222 is OK, while for T 333, T 444, T 555 and T 666, the program will fail. More detail studies on the calculation method of higher order terms in SAD need to be done.

My plan To study the calculation method of the higher order terms of transfer matrix in SAD (started). To make some studies on the ATF2 beam dynamics (Started). To make some studies on the ILC beam dynamics by using different simulation codes (Just started). To explore and understand the XSIFParser source files maintained by PT, then make the XSIF to SAD translator by using Visual Fortran language (will be started). To write my own code (will be started). ……