Design studies for the future High Luminosity LHC Alan Cooper Supervisors: Dr Stephen Gibson Dr Laurence Nevay.

Slides:



Advertisements
Similar presentations
Optics and magnetic field calculation for the Hall D Tagger Guangliang Yang Glasgow University.
Advertisements

LP EXAMPLES: ANOTHER MAX AND A MIN Dr. Ron Lembke.
Senior Q2 Shy Tortoise. Sample >>> > > >>
Beam Delivery Simulation Development & BDS / MDI Applications L. Nevay, S. Boogert, H. Garcia-Morales, S. Gibson, J. Snuverink, L. Deacon Royal Holloway,
Status of the Tagger Hall Background Simulation Simulation A. Somov, Jefferson Lab Hall-D Collaboration Meeting, University of Regina September
HER and LER radiative bhabhas The next two figures show the trajectories of the off-energy beam particle from radiative bhabhas. The first figure shows.
Finite wall wake function Motivation: Study of multi-bunch instability in damping rings. Wake field perturbs Trailing bunches OCS6 damping ring DCO2 damping.
TMP112 Calibration. Slope 1 (Max) Slope 2 (Max) Slope 3 (Max) Slope 1 (Min) Slope 2 (Min) Slope 3 (Min) The slope regions below were created from characterization.
Creation Of Control Systems In PVSS For Devices In The ALICE Detector A Large Ion Collider Experiment A dedicated heavy-ion detector at LHC (Large Hadron.
Status of BDSIM Developments at RHUL L. Nevay, S. Boogert, H. Garcia-Morales, S. Gibson, R. Kwee-Hinzmann, J. Snuverink Acknowledgments: R. Bruce, S. Redaelli.
Determination of R – matrix Supervisors: Prof. Nikos Tsoupas Prof. Manolis Benis Sándor Kovács Murat Yavuz Alkmini-Vasiliki Dagli.
$100 $200 $300 $400 $500 $100 $200 $300 $400 $500 $100 $200 $300 $400 $500 $100 $200 $300 $400 $500 $100 $200 $300 $400 $500 $100 $200 $300.
AWAKE Electron Spectrometer Simon Jolly, Lawrence Deacon, Matthew Wing 28 th January 2015.
1/33CREX Workshop Jefferson Lab March 16-19, 2013 NASA/CXC/SAO.
Training in Vacuum Technology for JUAS 2013 Students
Recent Upgrades to BBSIM Code V. H. Ranjbar † † Tech-X Corporation We have made several improvements to BBSIM, a parallel beam dynamics simulation code.
March 23, 2010 CMAD a tracking and e-cloud beam instability parallel code (M.Pivi SLAC) Taking MAD(X) optics file at input, thus tracking the beam in a.
Rutherford’s alpha scattering experiment. source of alpha particles thin gold foil photographic film beam of  particles most pass straight through 1 in.
Positional and Angular Resolution of the CALICE Pre-Prototype ECAL Hakan Yilmaz.
Lecture 9: Inelastic Scattering and Excited States 2/10/2003 Inelastic scattering refers to the process in which energy is transferred to the target,
PyHEADTAIL-PyECLOUD Simulations for LHC and HL- LHC Aaron Axford 27/05/20151.
Structuring Experimenting Esmée Bertens Tim de Ridder Herman de Vos /Department of Mechanical Engineering Systems Engineering Group Masters Team Project.
Graham Sellers Simulations of the beamline and detector regions of the LHC and FP420.
Celso Figueiredo26/10/2015 Characterization and optimization of silicon sensors for intense radiation fields Traineeship project within the PH-DT-DD section.
Location of the LW detector- Simulation of the LW signals Lawrence Deacon RHUL ATF2 meeting August 23 rd 2006 KEK.
1J. Gu CERN CSC Meeting July 2008 DAQMB/FEBs Readiness for First Beam Jianui Gu The Ohio State University.
Simulation of the CMS Endcap Alignment Scheme Using COCOA.
Neasan O’Neill GridPP. The LHC is massive Lots of bits Scientists and engineers have built all the individual components all over the world and it is.
THIN FILMS FOR CLIC ELEMENTS Outline Motivation The role of MME-CCS DB and MB transfer lines Main beam Main beam quadrupoles Other issues conclusions CLIC.
The HiLumi LHC Design Study is included in the High Luminosity LHC project and is partly funded by the European Commission within the Framework Programme.
Applications as Residual Gas Analyzer (RGA)
18 th March 2008Measuring momentum using the TOFsSlide 1 Measuring momentum using TOF0 and TOF1 Progress report Mark Rayner (Oxford/RAL) Analysis Meeting,
RFA Simulations Joe Calvey LEPP, Cornell University 6/25/09.
Particle Tracking for CDC prototype Amangaliyev Temirlan.
High Luminosity LHC Robustness & tolerances Catia Milardi HL LHC Task 2.2, September 19 th 2012.
E.B. Holzer BLM Meeting: Q & A March 20, Questions and Answers.
Status of the magnet studies in the ARCS (FLUKA)
Compact Linear Collider
Lecture 18 - Detectors Detector systems
Simulation of Properties of COMPASS Drift-Chamber Prototypes
My Working Experience at CERN
M. Sullivan International Review Committee November 12-13, 2007
Preliminary Y-chamber specifications – First draft
Damping Rings - Homework I
Status and needs of dynamic aperture calculations
Tassielli G.F. INFN Lecce & Università del Salento
J.A.Crittenden, Y.Li, X.Liu, M.A.Palmer, J.P.Sikora (Cornell)
Estimation and Protection on Synchrotron Radiation in CEPC Main Ring
RF Absorption Measurements from Beam Pipe Coatings
Mass Spectroscopy (MS) Applications as Residual Gas Analyzer (RGA)
A beam of particles, all with the same momentum but with a variety of masses and charges, enters a region of uniform magnetic field, as shown in the picture.
Upgrade phase 1: Energy deposition in the triplet
Microscopes.
200 kV gun CST microwave studio simulations Shield modifications
200 kV gun CST microwave studio simulations Shield modifications
High Granularity Calorimeter Upgrade Studies
ILC DR Working Group on Collective Effect: Electron Cloud
Residual Gas Analyzer (RGA)
CINVESTAV – Campus Mérida Electron Cloud Effects in the LHC
A Mapping Approach to the Electron Cloud for LHC
Chicane and Bunch Spacing Scans
Mechanics of Materials Engr Lecture 20 More Mohr’s Circles
US LHC Accelerator Research Program
C.2.10 Sample Questions.
C.2.8 Sample Questions.
Electron Diff.
Bunch Profiling with a Rotating Mask
C.2.8 Sample Questions.
Hiroshi Masui For the PHENIX Collaboration Quark Matter 2004
Types of Errors And Error Analysis.
Presentation transcript:

Design studies for the future High Luminosity LHC Alan Cooper Supervisors: Dr Stephen Gibson Dr Laurence Nevay

First Beam Delivery Example Extra particles were recorded where no sample planes were present. Beam pipe radius was increased to get around problem.

Beam Delivery Example Three quadrupoles (shown in red) with drift chambers in between. Built using BdSim – Beam Delivery Simulation. Produced a Python script to plot data.

Analysing Three Quadrupoles Mean - _______________ σ Min & Max - _._._._._._._._._._._

Future Goals Produce one long continuous quadrupole to model errors. Simulate electrons striking thin metal film. Compare to FLUKA LHC simulations.