Radar pulse compression using stepped Frequency train of pulses
Short Introduction to CLIC and CTF3, Technologies for ... · frequency multiplication pulse...
Transcript of Short Introduction to CLIC and CTF3, Technologies for ... · frequency multiplication pulse...
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Short Introduction to CLIC and CTF3,Technologies for Future Linear Colliders
Explanation of the Basic Principles and GoalsVisit to the CTF3 Installation
Roger Ruber
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2Roger Ruber - CLIC/CTF3 Visit - Introduction
Collider History
• hadron collider at the frontier of physics– huge QCD background– not all nucleon energy available
in collision
• lepton collider for precision physics– well defined CM energy– polarization possible
• next machine after LHC– e+e- collider– energy determined by LHC discoveries
consensus Ecm ≥0.5 TeV
p p
e+ e-
Simulation of HIGGS production e+e– → Z H Z → e+e–, H →
bb
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3Roger Ruber - CLIC/CTF3 Visit - Introduction
Circular versus Linear Collider
Circular Collidermany magnets, few cavities, stored beamhigher energy → stronger magnetic field
→ higher synchrotron radiation losses (∝E4/R)
Linear Colliderfew magnets, many cavities, single pass beamhigher energy → higher accelerating gradient
higher luminosity → higher beam power (high bunch repetition)
source main linac
N
S
N
S
accelerating cavities
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4Roger Ruber - CLIC/CTF3 Visit - Introduction
Cost of Circular & Linear Accelerators
Circular Collider• ΔE ~ (E4/m4R)• cost ~ aR + b ΔE• optimization: R~E2 → cost ~ cE2
Linear Collider• E ~ L• cost ~ aL
cost
energy
CircularCollider
LinearCollider
200 GeV e-
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5Roger Ruber - CLIC/CTF3 Visit - Introduction
e+ Linac
Interaction Point with Detector
e- Linace+ source e- source
RF powerSource
RF powerSource
Linear Collider R&D
CTF3 goals:1. high accelerating gradient2. efficient power production3. feasibility demonstration
accelerating cavities accelerating cavities
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6Roger Ruber - CLIC/CTF3 Visit - Introduction
Acceleration of Charged Particles
• Lorenz (EM) force most practical
• increasing particle energy
• to gain 1 MeV energy requires a 1 MV field
Direct-voltage acceleration used in• TV tube: 20~40 kV• X-ray tube: ~100 kV• tandem van de Graaff: up to ~25 MV
)( EBvF +×= e
eUdeE =⋅=Δ ∫ rE +-
e-
+-
+
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7Roger Ruber - CLIC/CTF3 Visit - Introduction
Drift Tube Linac: Higher Integrated Field
Courtesy E. Jensen © C
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680
8042
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8Roger Ruber - CLIC/CTF3 Visit - Introduction
• electrons β~1(v~c)
• short pulses• high frequency
>3 GHz
• typical10~20 MV/m
• CLIC:– 12 GHz– 240 ns– 100 MV/m
Travelling Wave Structure
RF powersource
electric fieldd
particle bunch
RFload
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9Roger Ruber - CLIC/CTF3 Visit - Introduction
Accelerating Cavities
CERN PS 19 MHz Cavity (prototype 1966)CLIC 30 GHz Cavity(prototype 2006)
ILC 1.3 GHz Cavity (prototype 2005) © K
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10Roger Ruber - CLIC/CTF3 Visit - Introduction
Surfing: or How to Accelerate Particles
DC Accelerator RF Accelerator
synchronize particlewith an
electromagnetic wave!
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11Roger Ruber - CLIC/CTF3 Visit - Introduction
e+ Linac
Interaction Point with Detector
e- Linace+ source e- source
RF powerSource
RF powerSource
Linear Collider R&D
Challenges:1. high accelerating gradient2. efficient power production3. feasibility demonstration
accelerating cavities accelerating cavities
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12Roger Ruber - CLIC/CTF3 Visit - Introduction
Electromagnetic Waves
• static electron→ electric field
• moving electron→ electromagnetic wave
• constant electron beam→ static electric field
+ static magnetic field
• bunched electron beam→ electromagnetic wave
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13Roger Ruber - CLIC/CTF3 Visit - Introduction
CLIC Two-beam Acceleration Concept
• 12 GHz modulated andhigh power drive beam
• RF power extractionin a special structure(PETS)
• use RF power toaccelerate main beam
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14Roger Ruber - CLIC/CTF3 Visit - Introduction
Drive Beam Acceleratorefficient acceleration in fully loaded linac
Power Extraction
Drive Beam Decelerator Sector
Combiner Ring x 3
Combiner Ring x 4
pulse compression & frequency multiplication
pulse compression & frequency multiplication
Delay Loop x 2gap creation, pulse
compression & frequency multiplication
RF TransverseDeflectors
Recombination to Increase Peak Power & Frequency
140 µs train length - 24 x 24 sub-pulses - 4.2 A2.4 GeV - 60 cm between bunches
240 ns
24 pulses – 100 A – 2.5 cm between bunches
240 ns5.8 µs
Drive beam time structure - initial Drive beam time structure - final
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15Roger Ruber - CLIC/CTF3 Visit - Introduction
Drive Beam Generation Scheme
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16Roger Ruber - CLIC/CTF3 Visit - Introduction
e+ Linac
Interaction Point with Detector
e- Linace+ source e- source
RF powerSource
RF powerSource
Linear Collider R&D
Challenges:1. high accelerating gradient2. efficient power production3. feasibility demonstration
accelerating cavities accelerating cavities
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17Roger Ruber - CLIC/CTF3 Visit - Introduction
CLIC: Compact Linear Collider
Main LinacC.M. Energy 3 TeV
Peak luminosity 2x1034 cm-2s-1
Beam Rep. rate 50 Hz
Pulse time duration 156 ns
Average field gradient 100 MV/m
# accelerating cavities 2 x 71,548 Φ4.5m tunnel
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18Roger Ruber - CLIC/CTF3 Visit - Introduction
CTF3 Test Facility
• demonstration drive beam generation• evaluate beam stability & losses in deceleration• develop power production & accelerating structures
X 5 Combiner Ring
84 m
X 2Delay loop
42 mDrive BeamInjector
180 MeV Probe Beam Injector
Two-Beam Test-stand
Drive Beam Accelerator
30 A - 150 MeV140 ns
30 GHz High Gradient Test stand
CLEX
Decelerator Test Beam LineDrive beam stability bench marking
CLIC sub-unit
Drive beam generation scheme