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The Neutrino Factory and Muon Collider Collaboration
R&D Programand
Participation in the IDS
Alan Bross UKNF Meeting January 10, 2007 2
NFMCC Mission
Extensive experimental program to verify the theoretical and simulation predictions
To study and develop the theoretical tools, the software simulation tools, and to carry out R&D on the hardware that is unique to the design of Neutrino Factories and Muon Colliders
Alan Bross UKNF Meeting January 10, 2007 3
Current Organization
R&D Tasks
DOE/NSF
Laboratories/MCOGP. Bond, S. Holmes, J. Siegrist
MUTACR. Kephart
CollaborationSpokespersonsA. Bross, H. Kirk
ProjectManager
M. Zisman
Simul. COOL Target MICE
ExecutiveBoard
TechnicalBoard
Collaborating Institutions
Neutrino Factory and Muon Collider Collaboration (NFMCC)
Other
Alan Bross UKNF Meeting January 10, 2007 4
Collaborating Institutions
National LabsArgonne
BNLFermilab
LBNLOak Ridge
Thomas Jefferson
UniversitiesColumbiaCornell
IITIndiana
Michigan StateNorthern Illinois
PrincetonUC-Berkeley
UC-DavisUC-Los Angeles
UC-RiversideUniversity of
Chicago
National LabsBudkerDESYINFN
JINR, DubnaKEKRAL
TRIUMF
UniversitiesKarlsruhe
Imperial CollegeLancaster
OsakaOxfordPohangTel Aviv
US International
Corporate PartnersMuons Inc.
Tech-X Corporation
Alan Bross UKNF Meeting January 10, 2007 5
Core Program
Targetry R&D: Mercury Intense Target Experiment (MERIT)
Spokesperson: Kirk McDonaldProject Manager: Harold Kirk
Ionization Cooling R&D: MuCool and MICEMuCool Spokesperson: Alan BrossUS MICE Leader: Dan Kaplan
Simulations & TheoryCoordinator: Rick Fernow
Muon Collider Task Force*
*Being organized now @ Fermilab
Hardware Activities
MuCool
Alan Bross UKNF Meeting January 10, 2007 8
MuCool Program
Currently consists of 9 institutions from the US and Japan
RF DevelopmentANLFermilabIITJLABLBNLMississippi
Absorber R&DFermilabIITKEKNIUMississippiOsaka
SolenoidsLBNLMississippi
Mission Design, prototype and test all cooling channel components
(SFOFO) 201 MHz RF Cavities, absorbers, SC solenoids
Support MICE (cooling demonstration experiment) Perform high beam-power engineering test of cooling
section components
Alan Bross UKNF Meeting January 10, 2007 9
R&D Focus of MuCool Component testing Fermilab
RF Cavities– High RF-power Testing
Absorbers– Technology tests– High power-load testing
•With beam Magnets
Alan Bross UKNF Meeting January 10, 2007 10
MuCool Test Area
Facility to test all components of cooling channel (not a test of ionization cooling)
At high beam power Designed to accommodate full Linac Beam 1.6 X 1013
p/pulse @15 Hz – 2.4 X 1014 p/s
– 600 W into 35 cm LH2 absorber @ 400 MeV
RF power from Linac (201 and 805 MHz test stands)
Waveguides pipe power to MTA
Alan Bross UKNF Meeting January 10, 2007 11
MTA
The MTA is the focus of our Activities
RF testing (805 and 201 MHz)
High pressure H2 gas-filled RF
LH2 Absorber tests
Two parts of infrastructure yet to be completed
Cryo Plant Beam Line
Alan Bross UKNF Meeting January 10, 2007 12
MTA Hall
Alan Bross UKNF Meeting January 10, 2007 13
MTA Hall Instrumentation
805
201
CsI
Plastic Scintillator
Magnet
Chipmunk
Alan Bross UKNF Meeting January 10, 2007 14
Phase I of RF Cavity Closed Cell Magnetic Field Studies (805 MHz)
Data seem to follow universal curve
Max stable gradient degrades quickly with B field
Sparking limits max gradient
Copper surfaces the problem
Gra
die
nt
in M
V/m
Peak Magnetic Field in T at the Window
Alan Bross UKNF Meeting January 10, 2007 15
Phase II of 805 MHz studies
Study breakdown and dark current characteristics as function of gradient and applied B field in Pillbox cavity
Curved Be window Test TiN coated Cavity has been
conditioned to 32MV/m without B field
Measurements at 2.5T– Stable gradient
limited < 17MV/m Button test
Evaluate various materials and coatings
– TiN, ALD– W,Cu,Mo,SS,..
Quick Change over
Alan Bross UKNF Meeting January 10, 2007 16
New 805 MHz RF data
Recent repeat of Max Grad with B
No conditioning observed
Alan Bross UKNF Meeting January 10, 2007 17
805 MHz Imaging
Alan Bross UKNF Meeting January 10, 2007 18
RF R&D – 201 MHz Cavity Design
The 201 MHz Cavity is now operating Reached 16MV/m at B=0 (design gradient!)
Alan Bross UKNF Meeting January 10, 2007 19
X-ray rates From 201 MHz Cavity
1.00E+03
1.00E+04
1.00E+05
1.00E+06
1.00E+07
0 2 4 6 8 10 12
B=0
Alan Bross UKNF Meeting January 10, 2007 20
201 Program
Conditioning 201 Cavity through multipacting
Observed at very low field This is now ready to begin Configuration shown to right
Allows for approximately 2T on axis at window facing magnet
Magnet operating in solenoid mode at 5T (max)
Field falls off rapidly in both r and z
We have also full azimuthal coverage to measure x-ray rates
Thin and totally absorbing plastic scintillator counters
Spectroscopy - NaI
Alan Bross UKNF Meeting January 10, 2007 21
High Pressure H2 Filled Cavity WorkMuon’s Inc
High Pressure Test Cell Study breakdown
properties of materials in H2
Just finished run in B field No degradation in M.S.G.
up to 3.5T
Alan Bross UKNF Meeting January 10, 2007 22
2D Transverse Cooling
and Figure of merit: M=LRdE/ds
M2 (4D cooling) for different absorbers
Absorber Design Issues
Absorber Accelerator
Momentum loss is opposite to motion, p, p x , p y , E decrease
Momentum gain is purely longitudinal
Large emittance
Small emittance
H2 is clearly Best -Neglecting Engineering
Issues Windows, Safety
Alan Bross UKNF Meeting January 10, 2007 23
Convective Absorber Activities
First Round of studies of the KEK absorber performed in the MTA
GHe used to input power
Alan Bross UKNF Meeting January 10, 2007 24
Convective Absorber Activities II
Alan Bross UKNF Meeting January 10, 2007 25
Convective Absorber Activities III
Next Round of tests will use a modified absorber
Test Electrical Heater New
Temperature sensors
LH liquid level sensor
Absorber Body being modified in Lab 6 at Fermilab
Instrumentation will be usedin MICE
Alan Bross UKNF Meeting January 10, 2007 26
LiH Test Program
Produce encapsulating cast (not pressed) samples Small disk (5-10 cm) for intense radiation
exposure Look at Material stability primarily Temperature Profile
Large disk (30 cm) for detailed thermal conductivity studies
External Cooling + Internal Heating Potential absorber for MICE Phase I
– Non-instrumented, no cooling
MICE
Alan Bross UKNF Meeting January 10, 2007 28
Muon Ionization Cooling Experiment
MICE
Beam Diffuser
FocusCoils
LiquidHydrogenAbsorbers
RFCavities
Tracking Spectrometers
MatchingCoils
Radiation shield
Magneticshield
CouplingCoils
Alan Bross UKNF Meeting January 10, 2007 29
US MICE
Tracker Module Solenoids Fiber ribbons VLPC System
VLPCs, Cryostats and cryo-support equipment, AFEIIt (front-end readout board), VME memory modules, power supplies, cables, etc
Absorber Focus Coil Module LH2 and vacuum safety windows
Fabrication and QC
RF Module Coupling Coils RF Cavities
Particle ID Upstream Cerenkov
Alan Bross UKNF Meeting January 10, 2007 30
MuCool and MICE
MuCool Collaboration interface to MICE Design Optimization/develop of Study II cooling channel
Simulations Detailed engineering
Full component design Systems integration Safety
RF cavity development, fabrication, and test 201 MHz operation in B field
Absorber development, fabrication, and test Ends with KEK prototype tests
MuCool will prototype and test cooling hardware including MICE pieces for which the collaboration is responsible
MERIT
Alan Bross UKNF Meeting January 10, 2007 32
MERIT –Mercury Intense Target
Test of Hg-Jet target in magnetic field (15T) Submitted to CERN April, 2004 (approved April 2005) Located in TT2A tunnel to ISR, in nTOF beam line First beam ∼Summer, 2007
Test 50 Hz operation at 24 GeV 4 MW
Alan Bross UKNF Meeting January 10, 2007 33
34
nozzle A before reaming
ORNL 2006 Nov 28 runs10 m/s
ORNL 2006 Nov 29 run, uprighted image Nozzle C 20 m/s
Movies of viewport #2, SMD camera, 0.1 ms/frame
nozzle A after reaming
Alan Bross UKNF Meeting January 10, 2007 35
Merit Instrumentation
Developed Full Mars Simulation
Particle fluxes, energy deposition, absorbed dose and residual activity in the experimental hall
Absorbed dose and activation of mercury system
Secondary particle production
Study/define diagnostics needed for experiment
Radiation load in components
Radiation shielding Particle production in
secondary beam
Design and Simulation
Alan Bross UKNF Meeting January 10, 2007 37
Design and Simulation -Some Specific Areas of Study
beam Drift Buncher
Rotator
Cooler
Overview of transport
Cool here
Capture/Bunch/Rotation/Cool
TimeTime
E
ner
gy
En
erg
yTwo fixed point acceleration: half synchrotron oscillation + path between fixed points
Linear nonscaling Linear nonscaling FFAGFFAG
H2 filled cavities
Alan Bross UKNF Meeting January 10, 2007 38
Design and Simulation - Acceleration
Dogbone RLA - footprint
-5000
-3000
-1000
1000
3000
5000
-15000 -10000 -5000 0 5000 10000 15000 20000 25000 30000 35000
z [cm]
x [cm]
Alan Bross UKNF Meeting January 10, 2007 39
NF Detector - Design and Simulation
Looking at Totally-Active Sampling Detector Scintillator Based
Magnetized 0.5T
Alan Bross UKNF Meeting January 10, 2007 40
Totally Active Segmented Detector
Simulation of a Totally Active Scintillating Detector (TASD) using Noa and Minera concepts with Geant4
3 cm
1.5 cm15 m
15 m
15
m
100 m
3333 Modules (X and Y plane) Each plane contains 1000 slabs Total: 6.7M channels
Momenta between 100 MeV/c to 15 GeV/c Magnetic field considered: 0.5 T Reconstructed position resolution ~ 4.5 mm
Alan Bross UKNF Meeting January 10, 2007 41
TASD Performance
Muon reconstructed efficiency Muon charge mis-ID rate
Alan Bross UKNF Meeting January 10, 2007 42
Large Magnetic Volumes
Possible magnet schemes
Steel
15 m x 15 m x 15m solenoid modules; B = 0.5 T
Magnet
Superconducting coil magnet cost extrapolation formulas:• Use stored energy – 14M$/module• Use magnetic volume – 60M$/module• GEM magnet extrapolation – 69 M$/module
x10 modules!
Warm coil magnets:• Total cost: $5m x 10 = $50M (.1-.2T)• Problem: operational cost (>$13M/year with factor of 3 uncertainty)
Alan Bross UKNF Meeting January 10, 2007 43
Large Magnetic Volumes II
Cost Driver is not stored energy Vacuum Loading for vacuum insulated cryostats (A. Herve, CERN)
P0 = 0.33 S0.8 (Price of equivalent zero energy) P = P0 + 0.17 E0.7 (Total Price of magnet)
S = Surface of the cryostat V = Mean magnetized volume E = Stored energy
Must get rid of vacuum loading Foam Insulated
High Tc SC
SC “Pipe”
SC Pipe?
Alan Bross UKNF Meeting January 10, 2007 44
Back to the Future - VLHC
Fermilab TM-2149 (2001)
SC Transmission Line
3”
45
Magnetic cavern design
1 m iron wall thickness.
~2.4 T peak field in the iron.
46
|B| in XZ cross-section
Without iron With iron
Better field uniformity with iron in the end sections
47
Parameters
DESIGN PARAMETER UNIT No iron With iron
Isolenoid MA 7.5 Nturns/solenoid 150 Iturn kA 50 |B|average in XZ T 0.562 0.579 Wtotal GJ 3.83 3.95 Ltotal H 3.06 3.16 Fr maximum kN/m 15.66 15.67 Fx maximum kN/m 48.05 39.57
$1000/m $50M
100 kA op demonstrated
48
US – NFMCC 5 Year Budget Plan
Note: The Advanced Accelerator R&D Sub-panel recommended that a doubling of our funds would be appropriate. Our Muon Technical Advisory Council recommended a similar scenario
For FY07 - DOE has asked what we would do with additional fundsif a +10% or +20% budget increase were forthcoming. This is on thetotal including base ($3.6M)
Base Program funds: remain as in FY06: BNL ($0.9M); Fermilab ($0.6M); LBNL ($0.3M)
Alan Bross UKNF Meeting January 10, 2007 49
NFMCC Participation in the IDS
Areas of Interest Proton Driver
BNL, Fermilab Targetry
BNL, Fermilab, Princeton Capture and phase rotation
Fermilab Cooling
BNL, Fermilab, IIT, LBNL, UCLA, UC Riverside Acceleration
BNL, Fermilab, TJNL Detector Design and Simulation
Fermilab, IIT, University of Mississippi
Our level of effort, however, will depend on our budget in the out years. But there is some reason to be optimistic