Jacques Bouchez CEA/DAPNIA-Saclay & APC-Paris ISS meeting, detector WG KEK, Jan23 rd, 2006 MEMPHYS :...
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Transcript of Jacques Bouchez CEA/DAPNIA-Saclay & APC-Paris ISS meeting, detector WG KEK, Jan23 rd, 2006 MEMPHYS :...
Jacques Bouchez
CEA/DAPNIA-Saclay & APC-Paris
ISS meeting, detector WG
KEK, Jan23rd, 2006
MEMPHYS :
A megaton WČ detector in Fréjus underground laboratory
• Proton decay
• Supernovae: explosion, relics
• Solar and atmospheric neutrinos
• Oscillations: θ13 and δCP using superbeam and betabeam from CERN
PHYSICS MOTIVATION
• The Frejus site
• Results of the excavation study
• The detector
• Photodetectors
• R&D
• Physics performance
• Schedule
most transparencies borrowed from Luigi Mosca (CARE/BENE, CERN, 23/11/05)
and from Jean-Eric Campagne (GDR neutrino, Paris, 21/10/05)
LAYOUT
The MEMPHYS Project
65m
65m
Fréjus
CERN
130km130km
4800mweExcavation engineering pre-study has been done for 5
shafts
Water Cerenkov modules at FréjusCERN to FréjusNeutrino Super-beam and Beta-beam
13km(12 870 m)
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 2122 232425262728293031323334
70m x 70m x 250m
France Italy
FutureLab.
PresentroadTunnelatFréjus(grey)andfutureTunnel(black)forsafetywith34bypasses(shelters)connectingthetwoTunnels
A Very Large Laboratory In the middle of the Fréjus tunnel at a depth of4800
m.w.e a preliminary investigation shows the feasibility to excavate up to five shafts of about 250,000 m3 each
Henderson
HK
Main results of the Preliminary Study
1) the best site (rock quality) is found in the middle of the mountain,
at a depth of 4800 mwe
2) of the two considered shapes : “tunnel” and “shaft”,
the “shaft (= well) shape” is strongly preferred
3) Cylindrical shafts are feasible up to :
a diameter = 65 m and a full height h = 80 m (≈ 250 000 m3)
4) with “egg shape” or “intermediate shape” the volume
of the shafts could be still increased
5) The estimated cost is ≈ 80 M€ X Nb of shafts
80.00
R22.07R44.53
R44.00
72.04
34.64
44.00
36.00
Exemple of “egg shape” simulation, constrained by the rock parameter measurements made during the present tunnel and laboratory excavation.
The main feasibility criterium is that the significantly perturbated region around the cavity should not exceed a thickness of about 10 m
65m
~ 4 x SK
65m
Detector basic unit
Detector:
cylinder (a la SK) 65 m diameter and 65 m height: : → 215 000 tons of water (4 times SK)
taking out 4 m from outside for veto and fiducial cut →146 000 ton fiducial target
3 modules : 440 kilotons (like UNO) BASELINE
4 modules would give 580 kilotons (HK)
→Simulations done using 440 kt
each cavity 70 m diameter and 80 m total height
PHOTODETECTION
Baseline choice: use photomultipliers
get the highest possible coverage to get the lowest possible threshold
Ideally, we want the same light/MeV as SuperK.
…but the solution with 20’’ PMT’s becomes too expensive (cf. UNO)
(40 000 20’’ PMT’s/module with 40% coverage)
R&D on HPD started in France (with Photonis)
encouraging results from ICRR/Hamamatsu with 13’’ HPD
PMT size <=> costPhotonis @ NNN05
• Diameter 20“ <=> 12“ • projected area 1660 615 cm²• QE(typical) 20 24 %• CE 60 70 %
Cost 2500 800 €
Cost of useful PE/cm2 = PM cost/(areaxQExCE)
12.6 7.7 €/PE 40% saving
• 30% coverage (12’’) gives the same # of PE/MeV as 40% coverage (20’’)
• the required # of 12’’ PMT’s is twice the # of 20’’ PMT’s
•BONUS: better timing (risetime+jitter), better pixel localization
R&D on electronics (ASICs)• Integrated readout : “digital PM (bits out)”
– Charge measurement (12bits)– Time measurement (1ns)– Single photoelectron sensitivity
• High counting rate capability (target 100 MHz)
• Large area pixellised PM : “PMm2”– 16 low cost PMs– Centralized ASIC for DAQ– Variable gain to have only one HV
• Multichannel readout– Gain adjustment to compensatenon uniformity– Subsequent versions of OPERA_ROC ASICs
ASIC requirements• High speed discriminator for autotrigger on single photoelectron
• Coincidence logics to reduce dark current counting rate (to be defined by MC studies)
• Digitisation of charge over 12 bits
• Digitisation of time of arrival over 12 bits to provide nanosecond accuracy
• Variable gain to equalize photomultipliers response and operate with a common high voltage
• Data out wireless (why not?)
• Low cost (aim at 200 euros/channel )
R&D started at LAL Orsay, in connection with Photonis
Other interested french labs
Mechanics & PMT tests
Basic unit that we want to build and test under water
Electronic box water tight
IPNO
Taken in charge by IPNO: well experienced in photodetectors (last operation: Auger). With PHOTONIS tests of PMT 8”, 9” 12” and Hybrid-PMT and HPD
MEMPHYS physics reachA) non accelerator-based physics
• Nucleon decay (for 5 Megaton.years)
- 1035 yrs (p→e+0) - 2 1034 yrs (p→K+)- complementarity with liquid argon- some chance of discovery
– Neutrino bursts from Super-Novae explosion– 200,000 events from SN at 10kpc– 30 events from Andromeda– 2 events at 3 Mpc– collapse studies, explosion alerts (grav.antennas, telescopes)– mass hierarchy(θ13>10-3), θ13 sensitivity in [3 10-6 – 3 10-4]
– Relic Neutrinos from past Super-Novae explosions– 100 events in 5 Mt.y (with pure water)– 2000/4000 events in 5 Mt.y (with Gd loaded water)
MEMPHYS physics reachB) with CERN super and beta beams
ongoing studies within the ISS physics working group
A possible schedule for MEMPHYS at Frejus
Year 2005 2010 2015 2020
Safety tunnel Excavation
Lab cavity ExcavationP.S Study
detector PM R&D PMT production
Det.preparation InstallationOutside lab.
Non-acc.physics P-decay, SN
Superbeam Construction Superbeam
betabeam Beta beamConstruction
decision for cavity digging decision for SPL construction decision for EURISOL site
CONCLUSIONS
• The Frejus site can house a large scale (megatonne) detector
• The preferred geometry is made of cylindrical shafts
• 3 detectors give an overall fiducial mass of 440 kT
• A solution based on 12’’ PMT’s saves costs with same light as SK
• ongoing R&D for electronics (ASIC’s) and mechanics
• physicswise, MEMPHYS compares favourably to UNO and SK
• A full study on cavern + detector should be launched for EU FP7 in collaboration with liquid argon (GLACIER) and scintillator (LENA)
• Important milestone will be 2010
• Physics would start before 2020
• MEMPHYS welcomes all interested collaborators
• A document submitted to CERN council strategy group is available (see http:// council-strategygroup.web.cern.ch/council-strategygroup/SGcontrib.html)
BACKUP
SUPERBEAM BETABEAM
→ e e →
→ e e →
Superbeam + beta beam together
2 ways of testing CP, T and CPT : redundancy and check of systematics
2 beams
1 detector
2yrs
8yrs
5yrs
5yrs
pure4 flavours + K
ASICs submissions• MAROC : 64 ch multianode readout
– 64 fast digital outputs (2ns risetime)– Charge measurement with variable shaping– Gain adjustment (6bits)– 3 Digital thresholds (10bits)– Submitted June 05 (SiGe 0.35µm )
• MECANO2– Large dynamic range variable gain preamps– Fast unipolar shaper for 100 MHz counting rate– Submitted June 05 (SiGe 0.35µm)
MAROC1: BLOCK FUNCTIONALITY DIAGRAM • Complete front-end chip
with 64 channelsSubmitted in June 2005
Expected in October 2005
• Gain and Bandwidth flexibility:
–Gain adjustment per channel (6 bits: 0 to 4)
–Bipolar Fast Shaper:• Gain=5mV/fC• BW=10MHz
–Unipolar Fast Shaper:• Gain:5mV/fC• BW:100MHz• 3 thresholds: LSB=3mV, range=1V
to 3.5V
–Multiplexed charge measurement Peaking time with variable feedback network
• Tp=25ns to 200ns
Holdsignal
Photomultiplicator
Photons
VariableGain
Preamp.
VariableSlowShaper
S&H
BipolarFastShaper
UnipolarFastShaper
64Trigger
outputs
Gaincorrection(6bits)
4discriminatorthresholds(4*11bitsDACs)
Multiplexed
chargeoutput
cmd_LUCID
FS
_choice
LUCID
LUCID
Vth(BipFS)=2.3VVth1(UnipFS)=1.07V(1/3pe-)Vth2(UnipFS)=1.3V(1.5pe-)Vth3(UnipFS)=1.7V(3.5pe-)
• Possible use of IPs (expensive)
• Huge effort started in in2p3/CEA– Several designs in institutes
– 10 bit pipeline ADC (LPCC) 10MHz
– 10 Bit C/2C SAR (LAL) 1 mW 1 MHz
– 10 bit FADC (LAL) 100 MHz
– 12 bit Wilkinson (CEA,LAL,LPCC)
© J. Lecoq
Integrating the ADCs :
Pipeline ADC ©J. Lecoq100 MHz FADC ©V. Tocut