CHIPP Sept 2005 Jean-Sébastien Graulich Slide 1 What is MICE What is MICE M M uon uon I I onisation onisation C C ooling ooling E E xperiment xperiment What is Ionisation Cooling ? What is Ionisation Cooling ? Cooling = Reduction of Beam Emittance Energy Loss + Reacceleration = Reduction of p T /p L Limited Multiple Scattering Works better with light materiel (low Z) Works only for low energy muons No Energy Loss by Radiation No Hadronic Interaction
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CHIPP Sept 2005Jean-Sébastien GraulichSlide 1 What is MICE Muon Ionisation Cooling Experiment What is Ionisation Cooling ? Cooling = Reduction of Beam.
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CHIPP Sept 2005 Jean-Sébastien Graulich Slide 1
What is MICEWhat is MICE
MMuon uon IIonisation onisation CCooling ooling EExperimentxperiment What is Ionisation Cooling ?What is Ionisation Cooling ?
Cooling = Reduction of Beam Emittance Energy Loss + Reacceleration = Reduction of
pT /pL
Limited Multiple Scattering Works better with light materiel (low Z)
Works only for low energy muons No Energy Loss by Radiation No Hadronic Interaction
CHIPP Sept 2005 Jean-Sébastien Graulich Slide 2
Standard Cooling doesn’t work for Standard Cooling doesn’t work for muonsmuons
Stochastic and electron cooling are too slow
Never testedNever tested No doubt on the principle but practical challenges
Large RF Cavities in Strong Magnetic Field Liquid Hydrogen (Energy) Absorbers
Major source of uncertainty on the cost Major source of uncertainty on the cost and complexity of a Muon Storage Ringand complexity of a Muon Storage Ring
Better to PrototypeBetter to Prototype/study/study it it !!……
Why MICE is NeededWhy MICE is Needed
A factor 10 in intensity and 20% of the cost…A factor 10 in intensity and 20% of the cost…
CHIPP Sept 2005 Jean-Sébastien Graulich Slide 3
Why a Muon Storage Why a Muon Storage RingRing
Possible future big projects for PPossible future big projects for P International Linear Collider Neutrino Factory Muon Collider …
There is interest for a NuFact in EuropeThere is interest for a NuFact in Europe RAL: Very positive sign : Approval ! + Call for a scoping study CERN (report from Scientific Policy Committee to council):“Future neutrino facilities offer great promise for fundamental
discoveries. CERN should join the world effort in developing technologies for new facilities : Beta beams, Neutrino Factory…wherever they are sited.”
“Focus now on enabling CERN to do the best choice by 2010 on future physics programme.”
ECFA recommended “a co-ordinated collaborative R&D effort to determine the feasibility and practical design of a neutrino factory based on a high energy muon storage ring” (already in Sept 2001).
EMCOG (European Muon Coordination and Oversight Group):“The issue of ionisation cooling is critical and this justifies the important
effort that the experiment [MICE] represents” (Feb 2003)
Require Muon Storage Require Muon Storage Ring Ring
Trackers 1 & 2 measurement of emittance in and out
Spectrometer solenoid 1
Spectrometer solenoid 2
Beam PIDTOF 0
CherenkovTOF 1
Downstreamparticle ID:
TOF 2 Cherenkov
Calorimeter
MICE concept:MICE concept:Beam Diagnostic using particle per Beam Diagnostic using particle per
particle trackingparticle tracking
Matching coils 1&2
Focus coils 1
Coupling Coils 1&2
Focus coils 2Matching coils 1&2
Focus coils 3
CHIPP Sept 2005 Jean-Sébastien Graulich Slide 8
MICE SummaryMICE Summary
200MHz RF cavity with beryllium windowsLiquid-hydrogen
absorbersScintillating-fiber tracker
Muon Ionization Cooling Experiment
Status: Approved at RAL(UK)First beam: 04-2007
Funded in: UK,CH,JP,NL,USRequests: CH,It,JP,US
Single-beam ~200 MeV/c
4T spectrometer I
4T spectrometer II
TOF
Cooling cell (~10%)=5-45cm, liquid H2, RF
Final PID:TOFCherenkovCalorimeter
Aims: - Engineer and run a section of cooling channel- Measure emittance with 0.1 % accuracy
Main challenges:- RF in magnetic field!- Safety issues
Some prototyping:
CHIPP Sept 2005 Jean-Sébastien Graulich Slide 9
MICE PlanMICE Plan
- STEP I: April 2007
STEP II: October 2007
STEP III: 2008
STEP IV: 2008
STEP V2008?
STEP VI 2009?2009?
PHASE I- Understand systematics- Check optical match
PHASE II
Test ionization cooling
CHIPP Sept 2005 Jean-Sébastien Graulich Slide 10
Geneva in MICEGeneva in MICE
Management (Alain Blondel)Management (Alain Blondel) AB is Spokesperson
FundingFunding Trigger and Data Acquisition R&D for a tracker upgrade
TPC with GEM readout Request for a Swiss coupling coil being
submitted(contact: Bruker Biospin Faellanden-CH)
CHIPP Sept 2005 Jean-Sébastien Graulich Slide 11
Coupling CoilsCoupling Coils
If MICE is delayed, the neutrino factory might miss the next take off…
Currently, the coupling coils Currently, the coupling coils would be funded by the US…in would be funded by the US…in 2011! 2011!
MICE results would be *very* MICE results would be *very* late… late…
Fact
EURO P
2010…
A STRATEGIC contribution!A STRATEGIC contribution!
CHIPP Sept 2005 Jean-Sébastien Graulich Slide 12
Geneva in MICE (1)Geneva in MICE (1) RF Background Simulation (Rikard Sandstrom)RF Background Simulation (Rikard Sandstrom)
High-gradient Cu RF cavities in high magnetic field !
Field emission of electrons (dark current)-> Magnetic field focuses dark currents and lowers onset of breakdown-> Electrons produce X-ray by Bremsstrahlung, and produce breakdowns-> X-rays convert into the detectors
Direct measurement + Simulation => Tracker validation tests of 200 MHz cavity about to begin in FermiLab. Coupling coil will be necessary to test cavity with realistic
magnetic field!
Operation of Operation of
RF cavities in RF cavities in
Mag. Field is the Mag. Field is the
hardest challengehardest challenge
of MICE!of MICE!
CHIPP Sept 2005 Jean-Sébastien Graulich Slide 13
Geneva in MICE (2)Geneva in MICE (2)
PID Simulation (Rikard Sandtrom)PID Simulation (Rikard Sandtrom)- Muons decay in flight-> positrons- Cause systematics error on the emittance measurement-Bias must remain below 10-3 - PID detectors used in
Neural Network-> weight for “muonness”
+ study role of time measurements in determination of 6D emittances+ study role of time measurements in determination of 6D emittances
CHIPP Sept 2005 Jean-Sébastien Graulich Slide 14
Geneva in MICE (3)Geneva in MICE (3)
DAQ DAQ 600 muons per 1 ms Spill, repeated at 1 Hz All the tracking and PID data have to be buffered
in the FEE and read out at the end of the spill About 20 MB / Spill (20 GB / Run)
=>=> Architecture based on HARP experienceArchitecture based on HARP experience
Control and MonitoringControl and Monitoring Detector + Beam Line + Cooling Channel
Several 100 of parameters Should react at the spill rate (> 1Hz)