CERN Large Hadron Collider

Slides:



Advertisements
Similar presentations
Summary of Projects Kai Hock. LHC Upgrade About the project LHC is a 27 km circular accelerator in CERN that produces 7 TeV protons. The project is to.
Advertisements

Particle Physics Chris Parkes Accelerators & Detectors
Study of the Luminosity of LHeC, a Lepton Proton Collider in the LHC Tunnel CERN June F. Willeke, DESY.
1 Methods of Experimental Particle Physics Alexei Safonov Lecture #8.
Accelerators. Electron Beam  An electron beam can be accelerated by an electric field. Monitors Mass spectrometers  Any charged particle can be accelerated.
Discovering the Unknown at the CERN Large Hadron Collider (LHC) Amy Gladwin University of Arizona.
A. Bay Beijing October Accelerators We want to study submicroscopic structure of particles. Spatial resolution of a probe ~de Broglie wavelength.
Luminosity Prospects of LHeC, a Lepton Proton Collider in the LHC Tunnel DESY Colloquium May F. Willeke, DESY.
1 Where to Search for the Higgs  A direct search for the Higgs was carried out by the four LEP experiments from CMS energy of GeV The.
Beam Dynamics Tutorial, L. Rivkin, EPFL & PSI, Prague, September 2014 Synchrotron radiation in LHC: spectrum and dynamics The Large Hadron Collider (LHC)
Introduction to Accelerators Eric Torrence University of Oregon QuartNet 2005 Special Thanks to Bernd Surrow
The LHC: an Accelerated Overview Jonathan Walsh May 2, 2006.
March 2011Particle and Nuclear Physics,1 Experimental tools accelerators particle interactions with matter detectors.
Particle Accelerators
Future Accelerators at the energy frontier Peter Hansen february 2010 University of Copenhagen.
What are we made of ? Neutrinos Building a Particle Collider The ring is 27km round and on average 100m underground CERN – LEP, LHC.
An Introduction To Particle Accelerators A-Level Physics.
Accelerator Physics with Relativity By Mark, Jack and Frances (Designing the LHC in an hour and a half)
Magnetism The shadow of electricity. Magnetic Force Magnets apply forces to each other. Opposite poles attract, like poles repel.
Thomas Roser Snowmass 2001 June 30 - July 21, 2001 Polarized Proton Acceleration and Collisions Spin dynamics and Siberian Snakes Polarized proton acceleration.
What is the Higgs??? Prof Nick Evans University of Southampton.
Synchronization Andrew Hutton Slava Derbenev Yuhong Zhang.
Particle Accelerators
880.P20 Winter 2006 Richard Kass 1 The Large Hadron Collider LHC is located at CERN CERN is located near Geneva Part of CERN is in France The LHC collides.
Accelerator Group for LHeC LHeC Meeting at CERN; October Questions raised by Max  does the e-ring fit into the tunnel?  can one bypass ATLAS and.
J. Velkovska1 Lecture 17: Magnetic field sources. Ampere’s law PHYS 117B.02, Feb
How Are Electric And Magnetic Fields Used To Steer Particles In The Large Hadron Collider?
Improved electron cloud build-up simulations with PyECLOUD G. Iadarola (1),(2), G. Rumolo (1) (1) CERN, Geneva, Switzerland, (2) Università di Napoli “Federico.
3 November 2008 D.Acosta 1 Most Powerful Solenoid Magnet u 18kA, 3.8T solenoid u 3m radius, 15m length u 2.5 GJ stored energy u Can be discharged in a.
Introduction to Particle Physics I Sinéad Farrington 18 th February 2015.
An electron/positron energy monitor based on synchrotron radiation. I.Meshkov, T. Mamedov, E. Syresin, An electron/positron energy monitor based on synchrotron.
Synchronization Issues in MEIC Andrew Hutton, Slava Derbenev and Yuhong Zhang MEIC Ion Complex Design Mini-Workshop Jan. 27 & 28, 2011.
EU accelerator contributions to the IDS … R. Garoby ISS meeting RAL 28/04/2006.
E. Todesco, Milano Bicocca January-February 2016 Unit 2 Magnets for circular accelerators: the interaction regions Ezio Todesco European Organization for.
Pushing the space charge limit in the CERN LHC injectors H. Bartosik for the CERN space charge team with contributions from S. Gilardoni, A. Huschauer,
Research progress and plan CERN-KEK Committee, 2nd meeting 07/Dec/07 Masamitsu AIBA CERN-Japan fellow, AB/BI.
Presenter : Yang Wu McMaster University Work conducted at IHEP.
Note presentation: Performance limitations of circular colliders: head-on collisions M. Koratzinos TLEP ACC meeting no. 8, 25/8/2014.
CERN’s Large Hadron Collider
Lecture 2 - E. Wilson 16 Oct 2014 –- Slide 1 Lecture 2 - Overview of Accelerators II ACCELERATOR PHYSICS MT 2014 E. J. N. Wilson.
Beam Instability in High Energy Hadron Accelerators and its Challenge for SPPC Liu Yu Dong.
AXEL-2017 Introduction to Particle Accelerators
The Torque on a Current-Carrying Coil
Chapter 20: Magnetism Purpose: To describe magnetic field around a permanent magnet. Objectives: Describe a magnetic poles Describe magnetic field. Magnetic.
Circular Motion.
Lecture 2 Live Feed – CERN Control Centre
Future Collider Projects at CERN
C Top view Side view (28 – 13).
Hunting the Higgs Boson at the CERN Large Hadron Collider
CERN The world’s largest Particle Physics Research Center in Geneva
The operation of LHC accelerator complex Beam Measurement and Diagnostics Thanks to Stefano Redaelli CERN Beams Department Operations Group.
Synchrotron Ring Schematic
The Large Hadron Collider
Introduction to particle accelerators
Units The work done in accelerating an electron across a potential difference of 1V is W = charge x potential W = (1.602x10-19C)(1V) = 1.602x10-19 J W.
CASA Collider Design Review Retreat Other Electron-Ion Colliders: eRHIC, ENC & LHeC Yuhong Zhang February 24, 2010.
CSP Meeting CERN CERN Accelerators in th November 2010
Welcome to the CMS Virtual Visit
LHC (SSC) Byung Yunn CASA.
Particle Accelerators
Electron Rings Eduard Pozdeyev.
Lecture II.
Today 5-6 pm is a LAST chance
Explanation of the Basic Principles and Goals
ACCELERATORS AND DETECTORS
AXEL-2011 Introduction to Particle Accelerators
MEIC New Baseline: Luminosity Performance and Upgrade Path
MEIC Alternative Design Part V
CfE Higher Unit 2 – Particles and Waves
MEIC Alternative Design Part III
Presentation transcript:

CERN Large Hadron Collider Ref: www.cern.ch

What did the LHC do? Energies & Modes: Proton-Proton 2011 3.5+3.5 TeV 1380 on 1380 bunches 1368 on 1262 bunches Lead-208 (82+)- Lead 2011 1.38+1.38 TeV/u 2012 none (?) 358 on 358 bunches Proton-Lead 2013 4.0+1.577TeV/u 338 on 338 bunches

What “will” the LHC do? Restart in early 2015. Beam energy increase from 4 TeV to 6.5 TeV. So 13 TeV in proton-proton collisions. Consider shortening the spacing from 50 ns to 25. Can decrease the bunch population for same luminosity. Long term: HL-LHC, high luminosity LHeC, electron beam

LHC Magnets for your students... Superconducting dipole magnet has no iron and a lot of current current in its wire coils. Magnetic field limited by how well you make your supercond. wire and how much current it can carry. Usual dipole magnet (normally conducting), has a lot of iron and current in its wire coils. Magnetic field limited to all the magnetic domains in the iron aligned, about 1.8 Tesla.

More Magnets... A little Special Relativity... Just like the textbooks, almost... And the centripetal force for circular motion, All together In Accelerator physics it is usually written in the form

Any guesses? More Magnets... What we are doing: Some numbers for the LHC: 1232 Dipole Magnets, 15m Length, 27km circumference 7 TeV Design, 11850 Amps, 8.33 Tesla 4 TeV actual, 6770 Amps, 4.8 Tesla The radius of curvature of the orbit at 4.8 Tesla AND 4 TeV is... The radius of curvature of the orbit at 8.33 Tesla AND 7 TeV is... Any guesses?

More Magnets... What we are doing: Some numbers for the LHC: 1232 Dipole Magnets, 15m Length, 27km circumference 7 TeV Design, 11850 Amps, 8.33 Tesla 4 TeV actual, 6770 Amps, 4.8 Tesla The radius of curvature of the orbit at 4.8 Tesla AND 4 TeV is... The radius of curvature of the orbit at 8.33 Tesla AND 7 Tev is... The LHC ring does not change here. Its size is fixed, r is fixed.

Links https://lhc-statistics.web.cern.ch/LHC-Statistics/# http://www.lhcportal.com/ http://home.web.cern.ch/topics/large-hadron-collider http://cds.cern.ch/record/1165534/files/CERN-Brochure-2009-003-Eng.pdf http://home.web.cern.ch/ aa

Large Hadron Collider (LHC)‏ Circumference 27 km Two beams opposite directions proton on proton 8 TeV 1380 on 1380 bunches Energies: Linac 50 MeV PSB 1.4 GeV PS 28 GeV SPS 450 GeV LHC 3.5 TeV 4.0 TeV (soon) 6.5 TeV Ref: Introduction to Accelerators, Elena Wildner, CERN

Units?