SixTrack: Minor bug fixes and pencil beam R. Bruce.

Slides:



Advertisements
Similar presentations
Photon Collimation For The ILC Positron Target Lei Zang The University of Liverpool Cockcroft Institute 24 th March 2007.
Advertisements

Test process essentials Riitta Viitamäki,
Collimation with retracted TCSGs R. Bruce, R. Kwee, S. Redaelli.
Combined cleaning in IR3 - MD results and simulations Adriana Rossi R.W.Assmann, R. Bruce, F. Burkart, M. Cauchi, D. Deboy, L. Lari, S. Redaelli, G. Valentino,
Simulation priorities for 2015 R. Bruce for task 5.2.
Programming Types of Testing.
TUPEC057 Advances With Merlin – A Beam Tracking Code J. Molson, R.J. Barlow, H.L. Owen, A. Toader MERLIN is a.
1 Validation and Verification of Simulation Models.
Programming. Software is made by programmers Computers need all kinds of software, from operating systems to applications People learn how to tell the.
The HiLumi LHC Design Study (a sub-system of HL-LHC) is co-funded by the European Commission within the Framework Programme 7 Capacities Specific Programme,
GRD - Collimation Simulation with SIXTRACK - MIB WG - October 2005 LHC COLLIMATION SYSTEM STUDIES USING SIXTRACK Ralph Assmann, Stefano Redaelli, Guillaume.
Loss maps of RHIC Guillaume Robert-Demolaize, BNL CERN-GSI Meeting on Collective Effects, 2-3 October 2007 Beam losses, halo generation, and Collimation.
Understand Application Lifecycle Management
+ The Practice of Statistics, 4 th edition – For AP* STARNES, YATES, MOORE Chapter 8: Estimating with Confidence Section 8.1 Confidence Intervals: The.
06/03/06Calice TB preparation1 HCAL test beam monitoring - online plots & fast analysis - - what do we want to monitor - how do we want to store & communicate.
External Review on LHC Machine Protection, CERN, Collimation of encountered losses D. Wollmann, R.W. Assmann, F. Burkart, R. Bruce, M. Cauchi,
CSC Programming for Science Lecture 16: Debugging.
Status of Phase II Energy Loss Studies 1. FLUKA with “simple” CERN-provided input file modeling ~40m around primary collimators used for all SLAC studies.
Optimising Cuts for HLT George Talbot Supervisor: Stewart Martin-Haugh.
Beam MC activity A.K.Ichikawa for beam group For more details,
+ DO NOW. + Chapter 8 Estimating with Confidence 8.1Confidence Intervals: The Basics 8.2Estimating a Population Proportion 8.3Estimating a Population.
Simulations of TCT beam impacts for different scenarios R. Bruce, E. Quaranta, S. RedaelliAcknowledgement: L. Lari, C. Bracco, B. Goddard.
Introduction to Testing CSIS 1595: Fundamentals of Programming and Problem Solving 1.
Simulation comparisons to BLM data E.Skordis On behalf of the FLUKA team Tracking for Collimation Workshop 30/10/2015 E. Skordis1.
Pedro Arce Introducción a GEANT4 1 GAMOS tutorial RadioTherapy Exercises Pedro Arce Dubois CIEMAT
Improving Collimator Setup Efficiency LHC Beam Operation Committee, G. Valentino, R.W. Assmann, R. Bruce, F. Burkart, M. Cauchi, D. Deboy, S.
Work in progress: Improved models of collimation margins with TCT damage limit R. Bruce, L. Lari 1 Input and discussions: R. Assmann, A. Bertarelli, C.
LHC off-momentum collimation simulation Hector Garcia Morales Royal Holloway University of London Roderik Bruce, Danielle Mirarchi, Belen Salvachua, Kyrre.
Case study: Energy deposition in superconducting magnets in IR7 AMT Workshop A.Ferrari, M.Magistris, M.Santana, V.Vlachoudis CERN Fri 4/3/2005.
Schematics for simplified energy deposition study in IR7 R. Assmann.
NM4SixTrack Implementation of new composite materials for HL-LHC collimator upgrades in SixTrack “Tracking for SixTrack” workshop – CERN, R.
STAR Simulation. Status and plans V. Perevoztchikov Brookhaven National Laboratory,USA.
The HiLumi LHC Design Study (a sub-system of HL-LHC) is co-funded by the European Commission within the Framework Programme 7 Capacities Specific Programme,
R. Miyamoto, MEBT Lattice Optimization, ESS AD Beam Physics Internal Review 1 MEBT Lattice Optimization Ryoichi Miyamoto (ESS) For Beam Physics Group,
R.W. Assmann, V. Boccone, F. Cerutti, M. Huhtinen, A. Mereghetti
Development Environment
Chapter 8: Estimating with Confidence
Chapter 8: Estimating with Confidence
TCT BLM response from tertiary halo at 6.5 TeV
Tracking simulations of protons quench test
HDF5 in SixTrack Regina Kwee-Hinzmann, Yngve I. Levinsen,
Overview of Needs for SixTrack on-line Aperture Check
Problem: A kicker failure can deposit 9 x 1011 protons on any metallic
Status of CHIPS cross sections and migration of the physics lists
Update on loss maps for input to energy deposition studies
Update on multi-turn particle debris tracking
Valloni A. Mereghetti, E. Quaranta, H. Rafique, J. Molson, R. Bruce, S. Redaelli Comparison between different composite material implementations in Merlin.
Beam collimation for SPPC
Summary of Week 11: 14 – 21 March
Programming.
Global aperture measurements at 450 GeV with 170 mrad crossing angle
Chapter 8: Estimating with Confidence
Status of energy deposition studies IR7
Discussion of High Energy Proton Losses in Arc 7
Efficiency of Two-Stage Collimation System
Chapter 8: Estimating with Confidence
Chapter 8: Estimating with Confidence
Chapter 8: Estimating with Confidence
Improving Collimator Setup Efficiency
FLUKA Energy deposition simulations for quench tests
Chapter 8: Estimating with Confidence
Collimator Efficiency Study
Chapter 8: Estimating with Confidence
Chapter 8: Estimating with Confidence
Chapter 8: Estimating with Confidence
Chapter 8: Estimating with Confidence
Chapter 8: Estimating with Confidence
Chapter 8: Estimating with Confidence
Chapter 8: Estimating with Confidence
Study of Beam Losses and Collimation in JLEIC
Presentation transcript:

SixTrack: Minor bug fixes and pencil beam R. Bruce

Output of single diffractive events Inelastic interactions printed out on FLUKA_impacts.dat for use by FLUKA team In IR7, FLUKA team re-tracks all single diffractive events to correct for approximations in the K2 cross section Also single diffractive events needed in FLUKA_impacts.dat In present release version checked out from svn, this is NOT the case (discovered during the review preparations) R. Bruce, Interaction type

Output of single diffractive events Reason: output inside if-statement. Only inelastic written out First, coordinate transformation. Then writeout, then set to mm …. R. Bruce,

Fix of output of single diffractive events Include also single diffractive in if-statement (nabs=4) But apply coordinate transformation NOT to x as in old code, as we need to keep tracking the x for single diffractive. Instead, set x_flk=x and then transform x_flk. R. Bruce,

Fix of output of single diffractive events Apply change to 99.99mm only for particles with nabs=1 All changes enclosed within tags /* start RB fix */ and /* end RB fix */ Benchmark: ran SixTrack for 256 particles with IDENTICAL random seeds with old and new code. All files and output numbers are identical except additional lines in FLUKA_impacts with additional lines for single diffractive. Fix seems to work R. Bruce,

Minor changes to error modeling In fort.3, one can set the range in s to which errors on collimators should be applied. In release version this does not work (errors applied everywhere) After some serious debugging, error found Fix: Including TCRYO R. Bruce,

Pencil beam Can choose starting conditions between different types of annular phase space distribution (standard halo) and pencil beams Example loss maps for 3.5 TeV, b*=1.5m, hor halo B1. Identical inputs apart from starting conditions R. Bruce, Pencil beam Halo Inefficiency the same within 5% higher TCT losses in with pencil beam

Pencil beam TCT leakage per plane and beam Pencil beam Halo Pencil beam seems to overestimate losses on vertical TCTs. Reason presently unknown

Pencil beam routine Tried to look in detail on pencil beam routine Minor inconsistencies found Tilt angle applied at TCP on first turn and not later Distribution perpendicular to collimation plane not mathced (all angles set to 0) Correct angle of pencil beam, accounting for beam divergence Other differences: With the halo deformation over several turns by non-linearities, halo routine tends to load one TCP jaw more than the other. Pencil beam splits the hits equally between jaws. Detailed explanation of discrepancies still to be understood. Halo seems to better reproduce measurements. Agreement good if FLUKA factor accounted for (see IPAC).

Ideas for improvement and pending issues Observed unnaturally high amount of inelastic inetractions at the end of TCP. Probably not critical, but should be understood. Pointed out by FLUKA team Store history of each particle for debugging and easier understan- ding of loss maps (already done by Daniele?) When using random seed = 0, one could write out the actual used seed to a file so that the run can be repeated afterwards for debugging Inelastic interactions on TCP