2 nd tpc workshop paris, december 2004 marco zito1 a large tpc for the t2k neutrino oscillation...
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2nd TPC Workshop Paris, December 2004
Marco Zito 1
A large TPC for the T2K neutrino oscillation experiment
Marco Zito
Dapnia-SPP
CEA-Saclay
Outline:•T2K project•Near detector•TPC studies
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The Tokai to Kamioka (T2K) project
Long baseline neutrino oscillation experiment with an intense (0.75 MW) beamOff-axis by 2.5° -> Eν peaks at 0.75 GeV
Eν
SKNear det.
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The J-PARC facility at Tokai
50 GeV PS : Budget 1.5 G$ over 7 yearsNeutrino beam line : 160 M$
1021 POT (130 days) = 1year
Site 60km NE of KEK
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J-PARC (Japan Proton Accelerator Reasearch Complex)
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Decay Volume Constructionviewed from downstream
3NBT
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Looking closer to the Decay Volume Construction
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The T2K schedule
Start data taking in 2009
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Precise measurement of Δm223 and θ23
Obs/expected5000 ev/year at SK105 ev/year at ND
1-sin2(2θ)
Δm2
νμ disappearance
Need flux and spectrum measurement at ND detector
P(νμ→ νμ)≈1- cos4 θ13 sin2
2θ23 sin2 (1.27 Δm2
23 L/Eν)
Eν(MeV)
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νe appearance and θ13 measurement
100 ev/5 years for sin2(2θ)=0.1, BKG 15
Need νe contamination at ND and study of other backgrounds
P(νμ→ νe)≈sin2 2θ13 sin2
(1.27 Δm213 L/Eν)
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The near detector at 280m
TargetNear detector
To SuperK
Aims of the near detector :•Measure flux and spectrum based on
the quasi-elastic CC reaction νn -> μ-p
(pμ ≈1 GeV/c, pproton ≈ 300 MeV/c)
•Control background to QE
•Measure νe contamination in beam
•Measure NC νn -> νn π° : background
to νe appearance in SK
cos
2/2
pEm
mEmE
N
Nrec
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Schematic of near detector
• 280 m from target• Measure the energy spectrum and the (flux • cross-
section)• Recycle the UA1 (and NOMAD) magnet : 0.2 T
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Schematic of near detector
• 5-10 tons active target : segmented scintillator (+water) surrounded by EM calorimeter for NC and π0 production
• Flux : active target + tracker to measure μ, p (π) based on the quasi-elastic reaction : νn -> μ-p
Target + Ecal Active target (scintillator bars)
2 or 3 TPC modules
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TPC schematic
•Readout : GEM or Micromegas. The first large surface (o(10m2)) readout based on micropattern!
2.5m
B (0.2T)
E (200V/cm)E
ν beam
HV membrane
2.5 m
30x30 cm2 RO detecteurs
1m
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Why a TPC ?
• Excellent spatial resolution• Excellent pattern • Low mass• dE/dx for e-μ id• Build on existing RD project for the LC • Bonus : few 103/year interactions in the gas
Typical design parameters :• 2.5x2.5x1 m3 per module (2 to 3 modules)
• Gas : Ar (Ne)-CO2 based mixture (low transverse diffusion)
• Drift 1.25 m with E=200V/cm (V=25kV)• Pad : 4 to 8 mm -> few 100 k to 1M channels
First estimations , design studies in progress !
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TPC view of a nu interaction
Thanks to Dean Karlen
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TPC design issues : field cage
Various design are considered : Various design are considered : ALICE, STAR, NA49ALICE, STAR, NA49
Issue : high efficiency for low energy protons. MC studies (F. Sanchez, IFAE) give indication that NA49-like design (more compact) is slightly more efficient
Study by Juergen Wendland (UBC postdoc)Study by Juergen Wendland (UBC postdoc)
E=200 V/cm V=25 kV (up to 50 kV)
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TPC design issues : gas mixture
• Low magnetic field (0.2 T) and long drift (1.25 m) → need low transverse diffusion
• CO2 is a good component. Drawback enhanced attachment on Oxygen
• Main component : Ar or Ne (closer to Oxygen in nuclear size)
• Various mixtures with 5 – 10 % CO2 are under study• Example : Ar-Methane-CO2 (85-10-5)• v(drift)= 2.7 cm/μs; Diffusion (T) = 230 μm/sqrt(cm); Diffusion (L) =
270μm/sqrt(cm); • Spatial resolution (diffusion term) = 420 μm (at 1.2 m drift, for 4mm
pad) • σ(pt)/pt = 4 % (for 60 cm track measurement, at 1 GeV)• Gas studies just started, will continue next year
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TPC design issues : gas amplification
GEM
OR
MICROMEGAS
Both concepts have been built and proven to work (COMPASS) Minor advantages/drawbacks each : •GEM : multistage, industrialization•Micromegas : sparks, charge spread (resistive foil ?)Both need to tackle the large surface, multidetectors problem (dead zones, mechanics, etc) !
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TPC design issues : pad geometry
Pad 8x8 mm2: CCQE at drift=60 cm, D = 300 mm/Pad 8x8 mm2: CCQE at drift=60 cm, D = 300 mm/cmcmStudy by Dean Karlen
Error budget pt / pt <10 %
pt / pt vs pt
pt / pt vs pt < 0.8 GeV/cpt / pt
pt (GeV/c)
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68 Channels
SCA
Digital Processor
(FPGA/DSP)
N x 68 channels
M x Mbits switches
600 Kchannels
Dig
itize
r
SyncTrigger1 chip
• How to build the whole system.
• How to transfer the whole set of data
TPC electronicsFirst ideas presented by F. Druillole (Saclay)
ASIC
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PAC Filters
Sampler control
Discri + decoder (selection of read part)
SCA(512 cells)
Tr
= 1
00n
s
Tsh
ap
ing
2
00n
s 2
µs Fs 1MHz to 10MHz
Anti-aliasing
Shaper
Low noise preamp
Options twoOptions two
x n
Column selector
Slow control
ADC
seri
aliz
er
ADC freq : 20MHz
50MHzOne integrated ADC/channel
TPC electronicsF. Druillole (Saclay)
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Timeline-Organisation
• Groups involved : Saclay, TRIUMF, Victoria U., Geneva U., Italy (Bari, Roma,…), Spain (Barcelona,…)
• Draft « Conceptual Design Report » : march 2005• Detector study and design : 2005• Ready to take data : 2009
• Next meeting 7-12 march 2005 at KEK• Lot of studies and prototype activity next year at
TRIUMF, CERN (Harp TPC) and Saclay
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The Saclay TPC prototype
SC magnet from NMR, field up to 2T
Thanks to Paul Colas, Vincent Lepeltier, Mike Ronan
TPC prototype with Micromegas r/o for LC, now being also used for T2K studies
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2x10 mm2 pads
1024 pads
1x10 mm2 pads
Readout anode pad plane
Berkeley Saclay OrsayChamber
diameter 50 cm length 50 cm
Copper mesh
50 m pitch
50 m gap
The TPC The TPC prototypeprototypeThe TPC The TPC
prototypeprototype
STAR electronics
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Example of Ne-CO2 (10%)Cosmic ray trackNovember 2004
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Conclusions
• The first large scale TPC based on micropattern techniques !
• Timescale : start data taking in 2009 • Plenty of opportunity to test technical solutions in a real-
size detector
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Backup slides
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Neutrino Facility overview
ND280mAug.2004 version
3NBT
Nowunder construction
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• Specification:
• Drift Time = 51 µs to 512µs• Number of cells : 512• Samples frequency : 1MHz to 10MHz• Anti-aliasing filter : 2µs• shaping time : 200ns to 2µs (discrete values)• Estimated dimension = 30mm² à 50mm²• Number of channel : 68 (Useable : 64)• Dynamic range = 10 bits• resolution : <10 bits• Input noise level < to be defined (relative to the detector gain)
The electronic must be able to adapt the signal processing in function of the gas inside the detector.
Asic cost will be negligible in the total electronic system.
Electronics specifications