Insertions for an Isochronous, 8-16 turn, 8-20 GeV, Muon FFAG
The Chorus Search for - Fermilablss.fnal.gov/conf/C000616/Ludovici.pdfand vertex predicted in...
Transcript of The Chorus Search for - Fermilablss.fnal.gov/conf/C000616/Ludovici.pdfand vertex predicted in...
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Neutrino 2000 - Sudbury, Canada - 16-21 June 2000
The Chorus Search forνµ→ ντ Oscillation
for the collaboration
Lucio LudoviciUniversity of Rome “La Sapienza” and INFN
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Outline• The Chorus search for Oscillation
• The experimental layout
• The analysis strategy
• Results from the “first round” analysis of thefull 1994-97 data sample
• Prospects for the final “second round” analysisresult
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Experimental Principles• Search for ντ appearance on a “pure” νµ beam
• High design sensitivity P(νµ→ ντ)=10-4 for∆m2≈1-10eV2 (relevant for cosmology & DM)
• The high background rejection calls for anunambiguous appearance signature
• A ντ is detected observing the τ- produced in aCC interaction and its subsequent decay vertexin an active nuclear emulsion target
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Detection Technique• 0.8 t emulsion as active neutrino target
– 4 stacks of 36 plates perpendicular to the beam– A µvertex with ~µm resolution, 300 3D hits/mm
• The scintillating fiber tracker– reconstructs the primary vertex, tracks leaving
the target and extrapolates back to emulsion:160 µm resolution, σθ=3mrad
emulsion target(4 stacks)
interface emulsions
8 fiber trackers planes
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Chorus Layout• Neutrino target• Active nuclear emulsion target• Scintillating fiber tracker
• Hadrons Sign and momentum• air-core magnet spectrometer
∆p/p = 0.035.p(GeV/c) ⊕ 0.221996-97 upgrade: ET, HC
• Showers energy, missing Pt• lead&fibers “spaghetti” calorimeter
∆E/E=32%/√E (hadrons)∆E/E=14%/√E (electrons)∆θhadr~60 mrad @10 GeV
air core-magnet
calorimeter
muon spectrometer
target emulsion
• Muon ID, sign and momentum• iron-core muon spectrometer
∆p/p~10%-15% (p<70 GeV)
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The Chorus τ “signature”• The τ lepton is identified by the three-fold
simultaneous observation of:the neutrino CC interaction vertexthe short τ− path, cτ=87µm, γ~O(10)paththe τ− decay topology: kink
kinkντ
µ-,h-
νµ, (πo’s)ντ
vertex
τ path
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Neutrino BeamCern SPS-WANF: 5.1019 PoT→ 840,000 νµ CC
ντ prompt contamination(from Ds decaying in theproton target) well belowthe Chorus sensitivity: ντ CC ~3.3.10-6 νµ CC
νµ : νµ : νe : νe 1.00 : 0.05 : 0.017 : 0.007
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Analysis StrategyElectronic detector reconstruction– pre-selection of events and tracks to reduce the scanning
loadEvent location in emulsion– location of tracks in the interface emulsion sheets and
follow-up to the interaction vertex (Scanback)Kink finding– Several “automatic” algorithms → confirmation by
operator eye-scan– (NETscan: search for all tracks in 1.5x1.5x6.3 mm3)
Post-scanning analysis– Kinematic study, kink Pt cut, precise momentum
measurement with ET
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Pre-Selection(electronic detector only)
τ-→ µ- ντ νµ Br=18%1 negative muon from the primary interaction vertexwith P < 30 GeV/c
τ-→ h- ντ n(πο) Br=50%τ-→ e- ντ νe Br=18%
No muons in the primary interaction vertex and atleast one negative track with P ∈ [-1,-20] GeV/c
τ-→ π+ π- π- ντ n(πο) Br=14%Not yet included in the analysis
1µ channel
0µ channel
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Automatic Emulsion Data Taking(pioneered by the Nagoya Chorus group)
Hardware video processorsreconstruct tracks asframe-to-frame emulsiongrain coincidence.
90 µm plastic support
350 µmemulsion sheet
CCDcamera
CCDcamera
microscope stroke
tomographicimages
x50 magnification~3µm focal depth
512x512 pixels120x150 µm view
350 µmemulsion sheetem
ulsio
n pl
ate
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Scanning speed• Impressive progress
of the automaticscanning speed sincethe Chorus start
• Almost one order ofmagnitude every twoyears 0,001
0,0100,1001,000
10,000100,000
1994 1996 1999 2000
#frames/s
• Scanning a large emulsion volume with automaticsystems is now feasible
• Emulsion data taking → database of measuredtracks
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Netscan(in progress for Chorus phase II)
1.5 mm
1.5 mm
All track segments
8 platesoverlapped
6.3 mm
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1.5 mm
1.5 mm
≥2 segmentsconnected
Netscan(in progress for Chorus phase II)
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1.5 mm
1.5 mm
Not passingthrough
Netscan(in progress for Chorus phase II)
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1.5 mm
1.5 mm
Small impactparameter
Netscan(in progress for Chorus phase II)
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Automatic Vertex Location
• Follow-up track, plate by plate to the vertex• Define the vertex plate as the first plate out of two
consecutive plates were a track segment is not found
• Fiber Tracker → Interface emulsion → Target emulsion• 100 µm most upstream of each target plate are scanned
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Kink Finding (Parent Search)(Large Angle-Long Path kinks)
• 100 µm most upstream of the vertex plate are searchedfor all track segments in a cone of width = 1/P(GeV/c)
• Segments with small impact parameters w.r.t. thefollow-up track are candidates track parent
→ Kink signature→ Manual scanning measurements
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Manual ScanningOperator computer-assisted measurements for about 3%of located vertices which are kink candidates afterautomatic scanning processing → detailed study of thekink topology
~78% ~5%
~13%
~3%
~1%
Decay topology: noblack prongs, no blobs,no recoil, no Augerelectrons
Pt > 250 MeV/c toreject π and K decays
Low momentumbackground track
Parent=DaughterNo angle difference
Backward-goingnuclear fragment
Hadron interaction
Decay (Kink)
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Data FlowProtons on target 5.06 . 1019
Good emulsion ~93% Emulsion triggers 2,305 K
Events with 1 negative muon and vertex predicted in emulsion 713,351
Pmuon < 30 GeV/c and angular cuts 477,625
Events scanned 359,506
1µ
Vertices located and kink search 136,357
Event with vertex predicted in emulsion 335,398 1 negative track with P[-20,-1] GeV/c
and angular cuts 122,412
Events scanned 82,551
0µ
Vertices located and kink search 20,081
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Expected Background EventsCharm from ν CC with missed primary lepton
νµ/e N → D− X µ+ /e+
µ− /h− + neutrals
Charm from ν CC with µ+ /h+ wrong chargeAssociated charm production in NC
D+ /Dο missed, associated to D− → µ− /h− + neutralsHadronic “White kinks
elastic scattering with no recoil or nuclear breakupPrompt beam ντ
1µ 0µ
< 0.05
0.11 0.03
< 0.03 0.69
--- 2.8
0.05 0.05No kine cuts, only Pt>250MeV/c, Ldecay<5plates(1µ), 3plates(0µ)
< 0.1
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White Kinks Evaluation• Poor previous knowledge of λWK(P,Pt). Difficult
to extrapolate (sensitive to the operativedefinition of “whitness”)
• Direct background evaluation from the 26 WKfound in 243m of hadron tracks measured inChorus → WK measurement in the signal-free“side-band” Ldecay > 3 plates (2.8mm)
• MC development to tune the cuts against theWK background– Fluka to model the hadron interactions in emulsion– Cuts to reproduce the minimum observable activity
(the white-gray transition) in the Chorus emulsions
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White Kinks Data vs MCWe measured λWK(Pt > 250MeV/c) = 21.3±7 mThis corresponds to 2.8±0.8 WK expected witha distance from the vertex L<3plates (2.8 mm)
Pt kink (GeV)Θ kink (rad)
WK WK
τ→ h τ→ h
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Further WK Reduction
Φ (rad)
ν
Φ t cut Ldecay cut
ε=0.83
• Θ t cut: τ opposite to the shower in the transverse plane•Ldecay cut: τ flight length shorter and correlated with Phad
Fligh
t len
gth (
cm)
Hadron momentum (GeV)
L90%
L80%L70%
L3plates
WK
τ→ h
WK
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Cuts Optimisation
0.39
0.60
0.66
1.08
1.46
1.57 BGtotNobserv
3.920.880.010.230.650.50
3.851.370.010.460.900.60
3.751.500.020.520.960.70
3.722.440.030.521.890.80
3.783.290.040.692.560.90
3.803.540.030.692.820.87
ExclusionPowerx 104Nobserv
BGtot Charmantineut
CharmneutrinoWK Ldecay
efficΦ t cut
4
6
1
1
0
0
2
2
0
0
0
0
Cuts optimisation by the a-priori criteria of maximisingthe exclusion power, independently from data.
L3plates
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Limit Evaluation
⋅∆⋅⋅=
ELm
P2
22 27.1sin2sin µτ
µτµτ θ
{ }∑ = ⋅⋅⋅=
0µ,1µkink
i ii
iCCµ
CCt
ii
µt
AANBR
NP
εσσ
µ
ττ
1µN 0µNCCCCµτ σσ µτ
1µ1µAA µτ
0µ0µAAkink
1µe kink
0µe
0.53 143,742 0.97 0.39 20,081 2.3 0.13
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Systematics• Dominant sources are:
1 - Reconstruction and location efficiency2 - Kink detection efficiency
– - largely cancels in the ratios– - From MC, with cross-check on charm events
and hadron interactions (80 founds, 84.4expected)
{ }∑ = ⋅⋅⋅=
0µ,1µkink
i ii
iCCµ
CCt
ii
µt
AANBR
NP
εσσ
τµ
ττ
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Systematics∆σCC = 10 %∆εkink = 15 % for 1µ, 20% for 0µ∆NWK = 30%∆Ncharm = 30%
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Exclusion PlotPµτ < 3.4.10-4Or, for large ∆m2
sin22θµτ < 6.8.10-4
at 90% CL [1]
[1] T.Junk, NIM A434 (1999) 435
Our exclusion power(sensitivity) is:
Pµτ = 3.7.10-4
Using a differentapproach[2] to CLintervals we could
have quotedPµτ = 2.2.10-4
[1] G.J.Feldman and R.D. Cousins, Phys.Rev. D57 (1998) 3873
0.6eV2
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νe→ ντ Exclusion Plot
νµ→ ντ νe→ ντ
Peτ < 2.6.10-2 at 90% CLOr, for large ∆m2
sin22θτµ < 5.2.10-2
7 eV2
5.2.10-2
Maximum mixing isexcluded at 90% CLfor ∆m2 > 7 eV2
Including an additionalsystematic of 25% onΦ νe/Φ νµ
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Chorus Phase II Analyis• New scanning methods (Netscan,...) with higher kink
finding efficiency (also charm physics)• Improved reconstruction (tracking, vertex finding,
muon ID,momentum)• Additional vertices located
0,0001
0,001
0,01
0,1
1
Hels
inki
1996
Jeru
salem
1997
Taka
yama
1998
Tamp
ere
1999
Sudb
ury
2000
Design sensitivityCurrent sensitivity
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Conclusions• We have completed our first run of data analysis
(phase I)• We expected 0.11 background events in the 1µ
channel and 1.08 in the 0µ channel with an exclusionpower (sensitivity) of Pµτ=3.7.10-4 (including systematic)
• We observed no candidates, and we interpreted thisin an excluded CR at 90%CL for νµ→ ντ and for νe→ ντoscillation.
• We have started our phase II analysis with the aimof reaching our design sensitivity of Pµτ = 10-4