the international linear collider project
DESCRIPTION
The International Linear Collider Project. Akiya Miyamoto KEK. Particle Accelerators and Colliders. Explore micro-world. CERN/LHC p-p collider, 14 TeV Radius ~ 9km. 1932 Lowlence’s cyclotron : 80 keV. p-p collider. International Linear Collider : ILC. e + e - Collider - PowerPoint PPT PresentationTRANSCRIPT
16 November 2007 Akiya Miyamoto
Do Son ACGRID School Symposium
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The International Linear Collider Project
Akiya Miyamoto
KEK
Particle Accelerators and Colliders
16 November 2007 Akiya Miyamoto
Do Son ACGRID School Symposium
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Explore micro-world
1932 Lowlence’s
cyclotron : 80 keV p-p collider
2008 CERN/LHC
p-p collider, 14 TeV
Radius ~ 9km
~x p
International Linear Collider : ILC
• e+e- Collider• Ecm: 0.2 ~0.5 TeV 1TeV• ∫Ldt = 500 fb-1 in 4 years
16 November 2007 Akiya Miyamoto
Do Son ACGRID School Symposium
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Why e+e- collider ?
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p p
e+ e–
Collisions of elementary particles
• Uses all energy for collisions• Clean measurements• Sensitive to faint signals of
new particles/phenomena• State-of-the-art detector
• Initial 4 vectors and polarizationsare known and controllable
• Precise tests of theory
Well known initial state
Progress of e+e– colliders
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Do Son ACGRID School Symposium
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J/
Circular collider
Linear Collider
Tera Scale: EW symmetry breaking
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Do Son ACGRID School Symposium
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dee
us
cb
t Wg G
HH
• Standard ModelLEP WG 2006
Theoretical Higgs mass bound
ILC reach
Higgs – Vacuum
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Higgs coupling proportional to mass in the SM
Did Higgs break the symmetry ?
Condensed
in vacuum ?
Supersymmetry
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Do Son ACGRID School Symposium
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Fermion Boson
• Do forces unify ?• Do Quarks and Leptons unify ?
Extending to Higher energy/Early Universe
Cosmology and ILC
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Do Son ACGRID School Symposium
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00
00
00
is a dark matter candidate
- Does exist ?
- Can be the dard matter ?
Extra Dimention
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Do Son ACGRID School Symposium
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Brane world ?- graviton may live in bulk
our world (4D)
extr
a di
m.
(bul
k)
e+e–
Linear collider
Number of Extra Dimension
Precision Physics
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Do Son ACGRID School Symposium
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ILC
ACFA WG
Top mass: mt < 100MeV( 1/10 better than LHC )
Top couplings
ILC, ILCSC, GDE
• The ILC project was initiated in 2004 with the endorsement by ICFA and ILCSC
• GDE was formed to develop the ILC accelerator design.
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Do Son ACGRID School Symposium
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High Gradient Acceleration
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3 types of cavity shapes under study
9 cell cavity~ 1m long
Towards 31.5 MeV/m
1 Cell RE cavity: > 50 MeV/m
10MWL band klystron
High Luminosity
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Do Son ACGRID School Symposium
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~ 5 nm
• Low emittance machine optics• Contain emittance growth• Squeeze the beam as small as possible
e- e+
KEK, ATF since 1993
Test bench for ILC-DR
ATF2 line
ILC Facility
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Two tunnels for
Accelrator and service
Particle detector
~31km tunnelResearch Area
Dumping Ring
ILC Reference Design Report
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Released 2007 summer: http://www.linearcollider.org/cms/?pid=1000437
Executive Summary
Physics at the ILC
Accelerator Detectors
RDR: 4 volumes/ 774 pages
RDR Authors
AsiaNorthAmerica
Europe
~1800 authors
~325 institutes
Connected through Internet
GDE plan and Schedule
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Next milestore
Detector Roadmap
• Detector time line should be synchronized with accelerator time line– because detector construction time would be similar to
accelerator construction time
• 2010: ‘light’ two detector EDRs– To be ready together with the accelerator EDR– Not for construction– Cost accuracy consistent with that for accelerator
• 2008: Select two groups to write EDRs based on LOIs.• October 4, 2007:
– ILCSC announces call for LOIs, due 1 October 2008.
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Do Son ACGRID School Symposium
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Detectors for ILC experiments
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Tracker: Charged particles
pt/pt : 1/10 of LHC
Higgs recoil to Z
Calorimeter:Neutral particlesE/E <½ of LEP
good badW/Z separation
WWZ
Z
Vertex Detectorb/c/ taggingRvtx<1/5 LHC
Improves (c-tag)
Detector concepts
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Do Son ACGRID School Symposium
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GLD
Small cell CAL.
Gaseous Tracker
3T
Asian based
LDC
Small cell CAL.
Gaseous Tracker
4T
European based
SiD
Small cell CAL.
Silicon Tracker
5T
NA based
4th
Dual RO CAL.
Gaseous Tracker
3.5T (Dual Sol.)
GLD+LDC ILD
ILC Detector R&D
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CPCCD Vertex
Detector Sensor Design
KPiX FE RO chip
Silicon Sensor test
Cutting-edge detector technologies
For TPC beam test
Scintillator sensors MPPCCalorimeter test
Simulation Studies
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Geant4 simulation ILC event
bcuds
Vertexreconstruction
Challenging perfect reconstruction of ILC events
Cal hits and track matching: PFA
Reconstruct Higgs in jet-mode
GRID for ILC
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Why GRID ?• A large CPU and storage resources for detector
optimizations and physics performance studies• Share CPU/storage/human resources for studies in a global
framework
Two VOs, ILC and CALICE, are in place• ILC VO
• a global VO of EGEE• a number of GRID sites world wide support ILC
• CALICE VO• CALICE is an international collaboration for calorimeter R&D
( ~ 200 phys.&eng. / 29 labs./12 countries in Asia/EU/NA• Test beam data (~14TB) is maintained and heavily used.
Conclusion
• ILC is crucial to push forward our understanding of fundamental low of nature.
• Research and Developments for accelerators and detectors for ILC are extensively pursued world wide.
• GRID is the indispensable elements of ILC studies.
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ILC NewsLine
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NewsLine Q
ILC Passporttranslating to many languages
http://www.linearcollider.org/
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B A C K U P
S L I D E S
ILC Design Parameters
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Max. Center-of-mass energy 500 GeV
Peak Luminosity ~2x1034 1/cm2s
Beam Current 9.0 mA
Repetition rate 5 Hz
Average accelerating gradient 31.5 MV/m
Beam pulse length 0.95 ms
Total Site Length 31 km
Total AC Power Consumption ~230 MW