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How Do Particle Accelerators Work?. If you have an older tv, you own an accelerator!. Acceleration occurs when a charged particle “falls” through a voltage difference. So stack up some batteries. A battery is about a buck and provides a 1.5 Volt difference – a buck/ev = a Gigabuck/GeV.
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If you have an older tv, you own an accelerator! • Acceleration occurs when a charged particle “falls” through a voltage difference. • So stack up some batteries. A battery is about a buck and provides a 1.5 Volt difference – a buck/ev = a Gigabuck/GeV. • BNL AGS, Cern PS, and Fermilab original design were a megabuck/GeV – quite a bargain – 1/1000 cost of batteries and does not bump the moon as it goes by!
Brute Force Accelerators:Make a high voltage and drop a charged particle through it • Van de Graaff – Charge must go to surface of a conductor. Clever way to use voltage twice. • Cockroft-Walton – Clever modification of rectifier (AC to DC converter) to get up to 10 or 12 times the voltage. • Up to a few hundred Mev, more would arc to ground. • Right energy range for lots of nuclear structure studies.
Cheaters – multiple use • Trick the particle into falling through the same voltage many (billions) of times, adding to the particle energy each time. • Usually involves magnets • Demo – Force on a wire carrying a current – That’s how a motor works! • Demo --Deflection of bean of electrons by a magnetic field -- That’s how a Tv works!
Circles! • A charged particle moving in a plane perpendicular to a uniform magnetic field moves in a circle of radius R. • pc = 0.30 B R where p is momentum (pc is approximately energy in GeV at high energy), B is the magnetic field with max of 2 Tesla for normal magnets. • Energy Radius • 1 GeV 1.7 m Chicago Syn Cyc • 33 55 Brookhaven AGS, CERN PS • 450 750 Fermilab, CERN SPS
Cyclotron • Tunafish can cut vertically. • One side +, other – • Protons in neg half near cut attracted into other half. • Magnetic field bends paths into half circles. • Switch voltages while this is going on • Charges on cans are opposite, so accelerated on this crossing too. • Repeat many times.
Miracle • Higher energy, bigger circle, longer path but higher energy is faster and exactly compensates and time for half revolution stays the same. • Thus continuous bunches of beam come out. • Stronger magnet, or bigger can and should get to very high energies? • No, at kinetic energies above about half of rest mass, relativistic corrections invalidate equal time rule. Need different time (period) for faster particles on the outside.
Synchrocyclotron • Put in a few bunches and change the frequency as they speed up. Beam now comes in bunches (less flux) but higher energy. • Magnetic field is limited to 2 T, so at 1 GeV the diameter is 3.4 m, and iron is expensive. • Genius: We have lost on continuous bunches. Save on all that iron in the center by ramping the field so R is constant as energy increases. • Build Cosmotron (3 GeV) and Bevatron (6 GeV) using RF acceleration instead of halves of cans
Strong Focusing • Clever trick: Magnets with 4 poles act like lenses and keep refocusing the beam to keep it small – hold down magnet cost. • Build AGS, Cern Ps, Fermilab, and CERN SPS
Linacs • We want an electron beam – particle with no internal structure is a cleaner probe. • Electrons bent in a circle radiate too much. • Forget the magnets and just string 2 miles of expensive RF cavities out in a straight line. Expensive, but California is worth it – Build SLAC.
Colliders, why? • Wasted Energy: At these accelerators the beam hits a piece of metal and the physics was the study of a moving particle hitting a particle at rest. The produced particles had to have the same momentum as the beam, a lot of useless kinetic energy. • Example: Fermilab 500 GeV proton hits a proton at rest. If all the energy and momentum went into one particle, it’s mass would have to be less than 30 GeV. Proton mass 1 GeV. W mass turns out to be about 90 GeV, cannot be produced at Fermilab or CERN SPS
450 + 1 = 30450 + 450 = 900 • I prefer the second choice, but there is a problem. Particle beams are VERY low density compared with a metal. Will the “colliding” beams just pass through one another with too few proton-proton collisions to be of interest?
Venturesome Souls • Midwest Research Associates late 1950s • Italian group 1960s electron-positron • CERN 1970s p-p Intersecting Storage Rings • Carlo Rubia, CERN 1980 – proton, antiproton at 450 each. He had only one ring so it did not “intersect”. Alternative – protons going round one way, antiprotons going round the other way in the SAME pipe. TEVATRON at Fermilab. • Electrons – Spear and BaBar at SLAC, CLEO at Cornell, LEP at CERN, KEK and Belle in Asia • And now back to pp intersecting rings at LHC.