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Physics of Particle Accelerators

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Physics of Particle Accelerators Kalanand Mishra Department of Physics University of Cincinnati How a Particle Accelerator Works Speed up particle with E/M field ... – PowerPoint PPT presentation

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Title: Physics of Particle Accelerators


1
Physics of Particle Accelerators Kalanand
Mishra Department of Physics University of
Cincinnati
2
How a Particle Accelerator Works
  • Speed up particle with E/M field
  • Smash particles into target or other particles
  • Record collisions with detectors
  • Able to identify product particles

3
Physics of a Particle Accelerator
  • Beam production
  • Bunching
  • Electron guns
  • Beam focusing
  • Colliding and Detecting




4
Beam production
  • Electron Beam
  • Thermoionic Emission

5
Proton Beam
  • Ionizing Hydrogen
  • Glow Discharge Column
  • From H- Ion

6
Other Beams
Secondary Beams
  • Proton
  • Antiproton
  • Other Particle Beams

7
Bunching
Bring the Particles in phase.
As spread out beam gives fewer collisions than a
narrowly focused one, e- e bunches are sent
into damping rings (e- to north, e to south).
8
Colliding
  • Fixed target
  • E ?(2mEp)
  • Colliding beam
  • E 2Ep

9
Beam Focusing
u As spread out beam gives fewer collisions than
a narrowly focused one, e- e beams have
to be focused. u This is done by bent
magnets.
10
Two Types
  • Linear Path
  • Travel once
  • Circular Path
  • Travel several times

11
Linear Accelerator
12
LINAC Operation
13
Methods of Acceleration in Linear Accelerator
SLC Polarized Electron Gun
14
Methods of Acceleration in Linear Accelerator
  • Basic idea
  • Synchronization
  • Length of the tube
  • Shielding

15
  • LINAC contd
  • Klystron Microwave generator
  • 1. Electron gun produces a flow of
  • electrons.
  • 2. Bunching cavities regulate speed of
  • electrons so that bunches arrive at the
    output cavity.
  • 3. Bunches of electrons excite microwaves
    in output cavity of the klystron.
  • 4. Microwaves flow into the waveguide ,
    which transports them to the accelerator. 5.
    Electrons are absorbed in beam stop.





16
Overall Operation of LINAC Electrons are
Accelerated in a Copper Structure
Bunches of electrons are accelerated in the
copper structure of the linac in much the same
way as a surfer is pushed along by a wave.
Changing Electric and Magnetic Fields

17
Klystron Operation
  • E/M waves that push the electrons in the linac
    are created by higher energy versions of the
    microwaves used in the microwave ovens in
    our kitchens.
  • The microwaves from the klystrons in the
    Klystron Gallery are fed into the accelerator via
    waveguides.
  • This creates a pattern of EB fields, which
    form an E/M wave traveling down the
    accelerator.


18
LINAC Structure
The 2-mile SLAC linear accelerator (linac) is
made from over 80,000 copper discs and cylinders
brazed together.
  • Microwaves set up currents that cause E
    pointing along accelerator and B in a
    circle around interior of accelerator.
  • Want e- and e to arrive in each cavity at
    right time to get max. push from E.
  • e needs to arrive when field polarity is
    opposite.


19
Circular Accelerator
20
Methods of Acceleration in Circular Accelerator
Cyclotron
  • The Ds
  • Electric field across the gap
  • Circular orbit
  • Increasing radius

21
Cyclotron
  • The maximum speed a proton could have
  • in a dee of radius R and strength B is given
  • by (ignoring relativistic effects.)
  • vm BeR / mp

22
Methods of Acceleration in Circular Accelerator
Synchrotron (synchro-cyclotron)
  • Electromagnetic resonant cavity
  • Magnetic field for circular orbit
  • Field synchronization with increasing
    particle energy
  • Synchrotron radiation
  • Storage ring

23
Synchrotron
  • The radius of curvature of the path of particles
    of momentum p and charge q in a synchrotron is
    given by the formula
  • R p / q B
  • where B is the field strength.
  • If a synchrotron of radius R has 4 straight
    sections of length L each and period of the radio
    frequency oscillator corresponds to the time of
    one revolution then
  • (a) The speed of the particles is
  • v ( 2pR 4L ) f

24
Synchrotron
(b) By considering the relativistic momentum
of particles of mass M, the magnetic field
strength of the synchrotron is given by
where f is the frequency.
25
Storage Rings
  • Similar to a synchrotron, but designed to keep
    particles circulating at const. energy not
    increase energy further
  • SPEAR 3 GeV
  • PEP I 9 GeV
  • PEP II e- 9 GeV
  • e 3.1 GeV

26
Detection
  • Tracking bubble, radiation
  • Tracking curvature (charged particle)

27
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