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Introduction to particle accelerators

Walter Scandale

CERN - AT department

Lecce, 17 June 2006

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Introductory remarks

Particle accelerators are black boxes producing � either flux of particles impinging on a fixed target� or debris of interactions emerging from colliding particles

In trying to clarify what the black boxes are one can� list the technological problems� describe the basic physics and mathematics involved

Most of the phenomena in a particle accelerator can be described in terms of classical mechanics and electro-dynamics, using a little bit of restricted relativity

However there will be complications:� in an accelerator there are many non-linear phenomena (stability of motion, chaotic

single-particle trajectories)� there are many particles interacting to each other and with a complex surroundings� the available instrumentation will only provide observables averaged over large

ensembles of particles

In two hours we can only fly over the problems just to have an overview of them

W.Scandale, Introduction to Particle Accelerators 12 June 2005 3

Inventory of synchrotron components

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Bending magnet

Efficient use of the current -> small gap heightField quality -> determined by the pole shapeField saturation -> 2 Tesla BEarth = 3 10-5 Tesla

B > 2 Tesla -> use superconducting magnets BLHC = 8.4 Tesla

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Quadrupole magnet

Vertical focusingHorizontal defocusing

g=gradient [T/m]

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Alternate gradient focusing

QF QF QFQD QD

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Mechanical analogy for alternate gradient

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Basic 2-D equation of motionin a dipolar field

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Basic 2D equation of motion

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Basic 2D equation of motion

FODO structure

Periodic envelop

Cos-like trajectory

Sin-like trajectory

Multi-turn trajectory

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Longitudinal stability

Momentum compaction

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Chromaticity and sextupole magnet

Dispersion orbit

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Chromaticity correction and non-linear resonance

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Emittance

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Synchrotron radiation

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Synchrotron radiation and beam size

Adiabatic damping Synchrotron light emission

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Effect of synchrotron light

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Collective effects

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Instabilities and feedback

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Space charge

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Beam size

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Fixed target versus collider rings

AdvantageColliderFixed target

Bruno Touschek

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Lepton versus hadron colliders

->

->

(At the parton level )

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Lecture II

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LHC lay-out

C = 26658.90 m

Arc = 2452.23 m

DS = 2 x 170 m

INS = 2 x 269 m

Free space

for detectors: ± 23 m

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LHC features

Technological challenge

(+1)

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Bunch spacing25 ns - 8.3 m

ε∗ = 3.75 10-6 m

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Maximum B-field

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Cos(θ) coil

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Superconducting dipole

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Collider luminosity

High L needs:

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Beam-beam interaction

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Head-on collisions

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LHC luminosityPerformances limitations

Luminosity:

L = event rate cross section �

= 1 �

N1 N2 k f �

S

2for equal, round, bi-Gaussian beams: N1 N2 = N

S --> 4š σσσσ 2

εεεε* = σ γσ γσ γσ γ2222

ββββ*

∗∗∗∗L = N k f γγγγ

2222

4π ε β4π ε β4π ε β4π ε β∗∗∗∗

protons in a bunch

no. of bunches

revolution frequency

beam cross section

invariant emittance

Head-on beam-beam:

detuning ξ = ξ = ξ = ξ = rp N4 π ε4 π ε4 π ε4 π ε∗∗∗∗

ξ ∗ ξ ∗ ξ ∗ ξ ∗ nb. of interactions Š 0.02

* εεεεL =

γγγγ

4πβ4πβ4πβ4πβN N

* ²t

Transverse beam density: • head-on beam-beam • space-charge in the injectors • transfers dilution

Beam current: • long range beam-beam • collective instability • synchrotron radiation • stored beam energy

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LHC insertions

56 m

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High luminosity experiments

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Ion-ion experiment

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