Thesis: Introduction Study for a failsafe trigger generation system for the Large Hadron Collider beam dump kicker magnets prepared by Martin Rampl.

Slides:



Advertisements
Similar presentations
Fast and Precise Beam Energy Measurement at the International Linear Collider Michele Viti.
Advertisements

8:16 SB 25ns dumped by RF; integrated lumi 0.6 nb-1. 9:14 BIC problem in TI8 and CMS recovering their tracker 10:09 Abort gap cleaning commissioning. 16:29.
Particle Accelerator. Particle accelerators It is a device that provides – forces on charge particles – by some combinations of electric & magnetic fields,
Summary of Research on Time-to-Digital Converters Summer Exchange Program 2008 Istituto Nazionale di Fisica Nucleare Rome, Italy Creative Studies Honors.
Measurements on phase stability at CTF3 Giulio Morpurgo / CERN IWLC 2010.
Discovering the Unknown at the CERN Large Hadron Collider (LHC) Amy Gladwin University of Arizona.
LHC Experiments at Liverpool E2V Visit – Nov 2005 Introduction Si Technology Upgrade/Maintenance Summary.
DEVELOPMENT OF A READOUT SYSTEM FOR LARGE SCALE TIME OF FLIGHT SYSTEMS WITH PICOSECOND RESOLUTION Considerations and designs for a system of tdc’s with.
A. Bay Beijing October Accelerators We want to study submicroscopic structure of particles. Spatial resolution of a probe ~de Broglie wavelength.
An Online Calorimeter Trigger for Removing Outsiders from Particle Beam CalibrationTests Denis O. Damazio José Manoel de Seixas Signal Processing Lab –
Analog-to-Digital Converters
Large Area, High Speed Photo-detectors Readout Jean-Francois Genat + On behalf and with the help of Herve Grabas +, Samuel Meehan +, Eric Oberla +, Fukun.
Particle Accelerators and Detectors
FCC-hh Injection and Extraction
Beam Dynamics Tutorial, L. Rivkin, EPFL & PSI, Prague, September 2014 Synchrotron radiation in LHC: spectrum and dynamics The Large Hadron Collider (LHC)
Comparators  A comparator compares two input words.  The following slide shows a simple comparator which takes two inputs, A, and B, each of length 4.
The CMS Muon Detector Thomas Hebbeker Aachen July 2001 Searching for New Physics with High Energy Muons.
A. Castañeda 07 th September 2009 Generators and Detectors Permit Loop / CIBG / CIBO 0v0.
CLIC Kickers: Status and activities for 2013 in view of the budget discussions for 2013 CTC #65 M.J. Barnes CLIC Technical Committee, November M.J.
Oliver Bitterling  Introduction to the QPS  Radiation damage in electronic systems  Construction of radiation tolerant systems  Radiation test and.
Progress towards nanometre-level beam stabilisation at ATF2 N. Blaskovic, D. R. Bett, P. N. Burrows, G. B. Christian, C. Perry John Adams Institute, University.
LHC Beam Dump System Technical Audit Trigger Synchronisation Unit.
What are we made of ? Neutrinos Building a Particle Collider The ring is 27km round and on average 100m underground CERN – LEP, LHC.
Accelerator Physics with Relativity By Mark, Jack and Frances (Designing the LHC in an hour and a half)
Proposal for participation in Si-PM testing and Upgrade work HEP Group Department of Physics Panjab University Chandigarh M. India-CMS meeting,
Status of the Beam Phase and Intensity Monitor for LHCb Richard Jacobsson Zbigniew Guzik Federico Alessio TFC Team: Motivation Aims Overview of the board.
R&D Programme for RT Phase Feedback Giulio Morpurgo.
LER Workshop, CERN, October 11-12, 2006Detector Safety with LER - Henryk Piekarz1 LHC Accelerator Research Program bnl-fnal-lbnl-slac Accelerator & Detector.
ICALEPCS 2005 Advanced uses of the WorldFIP fieldbus for diverse communications applications within the LHC power converter* control system Quentin King.
Partikeldagarna, Göteborg 21 September 2007 LHC: Status and Plans Lyn Evans.
28/03/2003Julie PRAST, LAPP CNRS, FRANCE 1 The ATLAS Liquid Argon Calorimeters ReadOut Drivers A 600 MHz TMS320C6414 DSPs based design.
Timing Requirements for Spallation Neutron Sources Timing system clock synchronized to the storage ring’s revolution frequency. –LANSCE: MHz.
BEPC II TIMING SYSTEM EPICS Seminar Presented by Ma zhenhan IHEP 20.August 2002.
Progress in the construction of the MICE cooling channel and first measurements Adam Dobbs, EPS-HEP, 23 rd July 2011.
CERN, 27-Mar EuCARD NCLinac Task /3/2009.
TRIGGER DELAY 100µs. G. Gräwer AB/BT/ECLBDS Trigger Delay2 The trigger delay is a back-up system that generates an asynchronous dump trigger for MKD and.
Krzysztof Czuba1 REFERENCE FREQUENCY DISTRIBUTION SYSTEM FOR THE TESLA TECHNOLOGY BASED PROJECTS Krzysztof Czuba Matthias Felber.
Anatomy of Accelerators Marty Peters Summer 2006.
Bunch Numbering P. Baudrenghien AB/RF for the LHC/RF team.
05 Novembre years of research in physics European Organization for Nuclear Research.
Timing System R+D for the NLC Josef Frisch. NLC and PEPII Phase and Timing Requirements (approximate)
High precision phase monitoring Alexandra Andersson, CERN Jonathan Sladen, CERN This work is supported by the Commission of the European Communities under.
IoP HEPP/APP annual meeting 2010 Feedback on Nanosecond Timescales: maintaining luminosity at future linear colliders Ben Constance John Adams Institute,
Crystal Oscillator Circuit and Its Working
Lucio Rossi The High Luminosity LHC Project Distinguished Lecturer 2013.
ISIS – Rutherford Appleton Cockcroft -Walton LINAC Muons Neutrons Synchrotron.
FONT5 digital feedback boards
Work on Muon System TDR - in progress Word -> Latex ?
1.) Acquisition Phase Task:
How to build a particle hunter
M.J. Barnes : Canadian Involvement with LHC
European Organization for Nuclear Research
Surviving an Asynchronous Beam Dump?
LHC schedule.
Prospecting for Gold: Particle Detectors
Status of the Beam Phase and Intensity Monitor for LHCb
The Compact Muon Solenoid Detector
Hunting the Higgs Boson at the CERN Large Hadron Collider
CERN The world’s largest Particle Physics Research Center in Geneva
CERN, the LHC and the Grid
The Large Hadron Collider
Particle Physics at CMS
Intra-Pulse Beam-Beam Scans at the NLC IP
BESIII EMC electronics
Welcome to the CMS Virtual Visit
Stanford Linear Accelerator
LHC upadtes.
Explanation of the Basic Principles and Goals
LHC Fast Timing Commissioning
ACCELERATORS AND DETECTORS
Presentation transcript:

Thesis: Introduction Study for a failsafe trigger generation system for the Large Hadron Collider beam dump kicker magnets prepared by Martin Rampl

CERN - The European Laboratory for Particle Physics  Provides the world-leading facilities for particle physics (funded by 19 European countries)  Particles are accelerated and collided within huge detectors  Aim: Investigation of the deepest layers of matter

LHC - The Large Hadron Collider  27 km-proton accelerator with two counter-rotating beams (completion 2005)  Superconducting magnets steer and accelerate the particles up to 7 TeV  Collisions occur within huge particle detectors

General design of the LHC beam dump (beam absorber)  Stored Beam Energy per Ring ~334 MJ (equivalent to 150 kg of TNT)  Gap of ~3 µs is left in the 89 µs (=time for 27 km) beam cycle for the dumping action  dfgdfgfdgdfgh Kicker magnets ~1900m

Tasks of the Trigger Generator  Synchronises the rise of the magnetic field of the kicker magnet with the beam gap  Continues operation if the beam revolution frequency signal is failing

Critical part 1: Internal Oscillator (digital Phase-Locked loop)  Measures continuously the beam revolution frequency  Continues generation of the SYNCHR. PULSE TRAIN signal even if BEAM GAP SYNCHR. is failing

Numerical Controlled Oscillator: Digital Phase Accumulator  Programmed value is added with every clock cycle  Overflow of the adder = Output frequency signal  High resolution (f=100 MHz, N=32bit  Res.=23 mHz)  Stability depends only on quartz oscillator

Internal Oscillator: Advantages-Disadvantages Accuracy only dependent on the short-term stability of the high-frequency quartz oscillator  stable (no temperature drifts,..) Accuracy only dependent on the short-term stability of the high-frequency quartz oscillator  stable (no temperature drifts,..) Reliable Reliable Simple implementation into programmable logic chip Simple implementation into programmable logic chip Easy to adapt to new requirements Easy to adapt to new requirements  Design requires a state-of-the-art chip

Critical part 2: Output Switch OSCILLATOR and DUMP REQUEST = TRIGGER OUT

Implementation block diagram of the Trigger Generator

Conclusion  Digital realisation provides perfect accuracy and stability  Implementation into Programmable logic chip maintains high reliability  But: Redundant and failsafe systems necessary in every case

Future aspects  Prototype will be built until end of July 1999  Final installation will be in 2004  progress in electronics  Changes in the requirements will influence design of the Trigger Generator