Fermilab ILC School, July 07 1 ILC Global Control System John Carwardine, ANL.
ILC Global Design Effort
Transcript of ILC Global Design Effort
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Global Design Effort 1
Barry BarishNRC BPA7-Nov-09
ILC Global Design Effort
FLASH TESTS
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ILC Global Context• Advancing the energy frontier has been and will
continue to be our most important tool for probing the central scientific questions in our field– Worldwide consensus through long range
planning studies that LHC followed by a complementary lepton collider (ILC is the leading candidate) is the highest priority for the future of particle physics (e.g. EPP2010)
– Total global cost of a future investment will be about the same scale as LHC or ITER.
– If the U.S. is to remain a leader in the field, it must have a significant role in a global lepton collider
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Proton-Proton Collisions at the LHC 2835 + 2835 proton
bunchesseparated
by
7.5 m→
collisions
every
25 ns= 40 MHz crossing
rate
1011
protons
per bunch
at 1034/cm2/s≈
35 pp
interactions
per crossingpile-up
→ ≈ 109
pp
interactions
per second !!!
In
each
collision≈
1600 charged
particles
produced
Enormous
challenge
for
the
detectors
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Exploring the Terascale• The LHC
– It will lead the way and has large reach– Quark-quark, quark-gluon and gluon-gluon
collisions at 0.5 -
5 TeV– Broadband initial state
• The ILC– A second view with high precision– Electron-positron collisions with fixed
energies, adjustable between 0.1 and 1.0 TeV– Well defined initial state
• Together, these are our tools for the terascale
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What will e+e-
Collisions Contribute?
• elementary particles
• well-defined
– energy,– angular momentum
• uses full COM energy
• produces particles democratically
• can mostly fully reconstruct events
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LHC ILCe+ e– Z H
Z e+ e–, H b …
Higgs event Simulation Comparison
b
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LHC: Low mass Higgs:
H MH < 150 GeV/c2
Rare decay channel: BR~10-3
Requires excellent electromagnetic calorimeter performance
acceptance, energy and angle resolution,
/jet and /0 separation
Motivation for LAr/PbWO4 calorimeters for CMS
Resolution at 100 GeV:
1 GeV
Background large: S/B
1:20, but
can estimate from non signal areas
CMS
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Precision Higgs physics
Model-independent Studies• mass
• absolute branching ratios
• total width
• spin
• top Yukawa coupling
• self coupling
Precision MeasurementsGarcia-Abia et al
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The linear collider will measure the spin of any Higgs it can produce by measuring the energy dependence from threshold
ILC: Is it really the Higgs ?
Measure the quantum numbers. The Higgs must have spin zero !
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What can we learn from the Higgs?
Precision measurements of Higgs coupling
Higgs Coupling strength is proportional to Mass
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Possible TeV Scale Lepton Colliders
ILC < 1 TeVTechnically possible
~ 2015 +
QUADQUAD
POWER EXTRACTIONSTRUCTURE
BPM
ACCELERATINGSTRUCTURES
CLIC < 3 TeVFeasibility?
ILC + 5-10 yrsMain beam –
1 A, 200 ns from 9 GeV to 1.5 TeV
Drive beam -
95 A, 300 nsfrom 2.4 GeV to 240 MeV
Muon Collider< 4 TeV
FEASIBILITY??ILC + 15 yrs?
Much R&D Needed• Neutrino Factory R&D +• bunch merging• much more cooling?• precision detectors??
ILC
CLIC
Muon Collider
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ICFA: e+e-
Linear Collider
• Physics Parameters– International subcommittee
report
• Technology– Superconducting RF
• International Design Team– Global Design Effort (2005)
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ILC Collider Parameters ICFA Report
• Ecm adjustable from 200 – 500 GeV
• Luminosity
∫Ldt = 500 fb-1 in 4 years
• Ability to scan between 200 and 500 GeV
• Energy stability and precision below 0.1%
• Electron polarization of at least 80%
• The machine must be upgradeable to 1 TeV
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The ILC SCRF Cavity
- Achieve high gradient (35MV/m); develop multiplevendors; make cost effective, etc
- Focus is on high gradient; production yields; cryogeniclosses; radiation; system performance
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main linacbunchcompressor
dampingring
source
pre-accelerator
collimation
final focus
IP
extraction& dump
KeV
few GeV
few GeVfew GeV
250-500 GeV
Designing a Linear Collider
Superconducting RF Main Linac
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ILC Global Context (ILC)
• Large R&D and Design Effort Worldwide on Accelerator and Detectors for the ILC– Total program is ~ $100M / year worldwide to
be compared with a total world HEP program of ~$2500M / year.
– The underlying technology –
Superconducting RF acceleration is developing rapidly and is strong candidate for next generation particle accelerators (XFEL, ILC, Project X, etc). Also, broad applications beyond particle physics
– SCRF accounts for about half the total ILC R&D program
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– 11km SC linacs operating at 31.5 MV/m for 500 GeV– Centralized injector
• Circular damping rings for electrons and positrons• Undulator-based positron source
– Single IR with 14 mrad crossing angle– Dual tunnel configuration for safety and availability
ILC Reference Design
Reference Design – Feb 2007
Documented in Reference Design Report
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RDR Design Parameters
Max. Center-of-mass energy 500 GeV
Peak Luminosity ~2x1034 1/cm2s
Beam Current 9.0 mA
Repetition rate 5 Hz
Average accelerating gradient 31.5 MV/m
Beam pulse length 0.95 ms
Total Site Length 31 km
Total AC Power Consumption ~230 MW
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International Costing
• “Value” Costing System: International costing for International Project– Provides basic agreed to “value”
costs– Provides estimate of “explicit”
labor (man-hr)]
• Based on a call for world-wide tender:– Lowest reasonable price for required quality
• Classes of items in cost estimate:– Site-Specific: separate estimate for each sample site– Conventional: global capability (single world est.)– High Tech: cavities, cryomodules (regional estimates)
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RDR Design & “Value”
Costs• The reference design was “frozen”
as of 1-Dec-06 for
the purpose of producing the RDR, including costs.
• It is important to recognize this is a snapshot and the design will continue to evolve, due to results of the R&D, accelerator studies and value engineering
• The value costs have already been reviewed three time
Total Value
Estimate = 6.62 B$ (US 2007)(+ 24M person-hours explicit labor ~ $1.4 B U.S.)
• ILCSC MAC review• International Cost Review Total ~ 8.0 B 2007$
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RDR Design & “Value”
Costs
SummaryRDR “Value”
Costs
Total Value Cost (FY07)4.80 B ILC Units Shared
+1.82 B Units Site Specific
+14.1 K person-years
(“explicit” labor = 24.0 M person-hrs
@ 1,700 hrs/yr) 1 ILC Unit = $ 1 (2007)
Host Cost$1.82 B Site Specific$0.70 B (~ 1/2 manpower)$1.60 B (Shared Costs)-------------$4.1 B (approx 50% total)
Partners (off-shore cost)$0.30 B (manpower)$1.00 B (shared costs------------$1.30 B (~ 15-20% total)
FY 07 $$
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Translating to “U.S. Costs”
• No official or detailed translation has been performed
• What are the factors?• Add some contingency (note GDE estimates include some, but not all (DoE) contingency. It needs to be done item by item. (conservatively + 20%) [ $8B ~$10B]
• Escalation to “then year dollars.”
This is the big factor that people use –
escalating for ~ 15-20 years would be ~ 200%
• For the total project, this gives ~$20B+
(then year $$)
• Comments:• US costs will only be a fraction of total project costs (off shore or on shore).
• Thinking in “then year”
$$ in the far future can be quite misleading. (Wages, GDP, etc also scale with inflation; Japan no
inflation, etc)
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Major R&D Goals for TDP 1SCRF
• High Gradient R&D -
globally coordinated program to demonstrate gradient by 2010 with 50%yield
• Preview of new results from FLASH
ATF-2 at KEK• Demonstrate Fast Kicker performance and Final Focus
Design
Electron Cloud Mitigation – (CesrTA)• Electron Cloud tests at Cornell to establish mitigation
and verify one damping ring is sufficient.
Accelerator Design and Integration (AD&I)• Studies of possible cost reduction designs and
strategies for consideration in a re-baseline in 2010
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Gradient GoalElectropolished 9-cell Cavities
0
10
20
30
40
50
60
70
80
90
100
>10 >15 >20 >25 >30 >35 >40
max gradient [MV/m]
yiel
d [%
]
DESY last test (25 cavities)JLab best test (14 cavities)DESY first successful test of cavities from qualified vendors - ACCEL+ZANON (15 cavities)JLab first successful test of cavities from qualified vendors - ACCEL (7 cavities)
OldNew
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TTF/FLASH 9mA Experiment
XFEL ILC FLASH design
9mA studies
Bunch charge
nC 1 3.2 1 3
# bunches 3250 2625 7200* 2400
Pulse length s 650 970 800 800
Current mA 5 9 9 9
Full beam-loading long pulse operation “S2”
• Stable 800 bunches, 3 nC at 1MHz (800 s pulse) for over 15 hours (uninterrupted)
• Several hours ~1600 bunches, ~2.5 nC at 3MHz (530 s pulse)
• >2200 bunches @ 3nC (3MHz) for short periods
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RF Gradient Long-Term Stability
Outliers caused by beam-loss trips prematurely shortening the beam pulse
Example Result
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Major R&D Goals for TDP 1SCRF
• High Gradient R&D -
globally coordinated program to demonstrate gradient by 2010 with 50%yield
• Preview of new results from FLASH
ATF-2 at KEK• Demonstrate Fast Kicker performance and Final Focus
Design
Electron Cloud Mitigation – (CesrTA)• Electron Cloud tests at Cornell to establish mitigation
and verify one damping ring is sufficient.
Accelerator Design and Integration (AD&I)• Studies of possible cost reduction designs and
strategies for consideration in a re-baseline in 2010
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Technical Design Phase and Beyond
AD&I studies
2009 2010
RDR ACD concepts
R&D Demonstrations
TDP Baseline Technical Design
2011 2012 2013
RDR Baseline
New
baseline inputs
TDR
TDP-1 TDP-2 ChangeRequest
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Final Remarks• We will be well positioned to propose a robust well-
developed project on a 2012-2013 timescale. NO COST GROWTH
• Earliest start for a construction project is ~ 2015, assuming science case, funding, siting, etc are in place
• CERN (see Sept Physics World) has stated its intent (or desire) to host a linear collider (either ILC or CLIC). This must be considered the most serious possibility, because of CERN ‘stable’
funding (earliest start ~ 2018)
• Japan or US are possible alternatives for hosting (Russia?). Japan is actively working toward the possibility (strong support group, siting efforts, industrialization, etc). Hosting efforts in the US are presently dormant, but the option remains viable, since we are developing key US technical infrastructures, etc.