new results from the opera experiment tomoko ariga aec-lhep, university of bern on behalf of the...
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New results from the OPERA experiment
Tomoko Ariga
AEC-LHEP, University of Bern
On behalf of the OPERA Collaboration
Motivation of the OPERA experiment
Neutrino oscillations have been studied in disappearance mode• Atmospheric sector : Super-Kamiokande, MACRO, MINOS, K2K,
T2K, ..
Long way to appearance• Super-Kamiokande : ντ appearance in atmospheric neutrino data
(statistical separation in background-dominated sample)• T2K : νe appearance in νμ beam
Main goal of OPERA•Verify νμ→ ντ oscillations in appearance mode (S/N ~ 10)
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Physics results from OPERA
•ντ appearance in νμ beamObservation of ντ appearance (4.2 σ), PTEP (2014) 101C01 In this talk, new results from the analysis of an enlarged data sample
Other topics• Sterile neutrino analysis (Talk by M. Tenti in SESSION 24.08. E)
• νμ→ νe oscillations (Talk by S. Zemskova in SESSION 24.08. E)
• Cosmic-ray physicsTeV atmospheric muon charge ratio, published in Eur. Phys. J. C (2014) 74:2933
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Principle of the experiment
•Detection of τ leptons in ντ charged-current interactions
Experimental requirements• Large target mass•Micrometric spatial resolution to detect short-lived τ lepton decays
τ’s life time 2.9x10-13 s (cτ 87 μm)
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Key technology: Emulsion particle detectors (unbeatable position resolution)
Cross-sectional view
Plastic base (200 m)
Emulsion layer (44 m)
Emulsion layer (44 m)
AgBr crystal
200 nm
OPERA film
20 m
10 GeV/c beam
Sensitivity 36 grains/100 m
3D tracking deviceIntrinsic resolution 50 nm
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The CNGS νμ beam (CERN Neutrinos to Gran Sasso)
The OPERA detector at LNGS exposed from 2008-2012
A total 17.97 x 1019 protons on target (20% less than the design value) resulted in 19505 ν interactions
CERN
LNGS
732 km
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produced by the SPS 400 GeV proton beam
Target section(~75000 units)
μ spectrometer Target section(~75000 units)
μ spectrometer
The OPERA detector
Total target mass 1.2 kton
2 identical super modules
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Analysis of neutrino interactions
• τ decay search• Impact parameter• Kink search• Parent search(Eur. Phys. J. C (2014) 74:2986)
5 mm
Emulsion gives 3D vector data with vertex position resolution of a few μm
Location efficiencyJHEP 11 (2013) 036
Tracks found in the interface films
Track follow-up
Volume scanningVertex reconstruction
(Animation)
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Charm decays: control sample for the τ decay searchCharm and τ decays have similar topologies
Good agreement between data and expectationsEur. Phys. J. C (2014) 74:2986
ντ analysis: kinematical selection
p2ryT
p2ry m
Cuts fixed since the beginning of the experiment
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τντ
zdec
θkink
pmissT
τ
ϕlH
Emulsion film
Transverse plane pmissT : vectorial sum of the
transverse momenta of primaries (except the parent) and daughters wrt beam directionp2ry
T : transverse momentum of the daughter wrt the parent direction
ντ analysis: data sample
•The 1st and 2nd most probable bricks for all runs• 15% larger than the previous one reported in PTEP (2014) 101C01
Number of events used in the analysis
5408 events analyzed and 5 events observed
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The 1st candidate: τ→1hPhys. Lett. B 691 (2010) 138-145
The 2nd candidate: τ→3hJHEP 11 (2013) 036
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The 4th candidate: τ→1hPTEP (2014) 101C01
The 3rd candidate: τ-→μ-
Physical Review D 89, 051102(R) (2014)
The 5th candidate: τ→1h recently reported
P1
Transverse plane
90 mrad kink with a 960 μm flight length
New
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The 5th candidate: particle identification
• Primary particle: hadronic interaction in the downstream brick
(measurement of dE/dx, consistent with proton hypothesis)charm background hypothesis discarded
(charm can be a background if the primary μ is not identified)
• Daughter: hadronic interaction in the 1st brick
Hadronic decay channel15
The 5th candidate: measured parameters
Fully consistent with the expected distributions for signal 16
Summary of all candidate events
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psum : the scalar sum of the momenta of all particles measured in the emulsion films
Fully consistent with the expected distribution
CC interactions with charm production
Hadronic interactions
Large angle μ scattering
Background sources
μ-
νμ
D+
νμνμ
h
μ-νμ
Monte Carlo simulation tuned on CHORUS data
Reduced by multi-brick tracking
FLUKA and test beam data
Reduced by nuclear fragment search and large angle scanning
New estimate by implementing a proper form factor for Lead : (1.2±0.1(stat.)±0.6(sys.))x10-7/νμCC well below the conservative value considered so far (arxiv.org/abs/1506.08759)
if the primary lepton is not identified and the daughter charge is not measured
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Significance
Expected signal and background events for the analyzed data sample
5 observed events with 0.25 background events expected
Probability to be explained by backgroundFisher 1.1x10-7
Profile likelihood 1.1x10-7
Corresponding to 5.1 σ exclusion of the background-only hypothesis
Probability of observing ≥5 candidates (2.9 S+B events expected): 17%Frequency of configurations being less probable than the observed one: 6.4%
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Estimation of Δm223
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90% confidence interval[2.0, 5.0] x 10-3 eV2
(assuming full mixing)
using profile likelihood, Feldman-Cousins, Bayesian
statistics, the difference among the
methods negligible
Conclusions
•Data sample including the first and second most probable bricks for all runs analyzed
• 5 ντ candidate events observed with 0.25 background events expected 5.1 σ significance for the exclusion of the null hypothesis
Discovery of ντ appearance
arxiv.org/abs/1507.01417 (accepted for publication in Phys. Rev. Lett.)
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The OPERA collaboration
BelgiumIIHE-ULB
Brussels
CroatiaIRB Zagreb
FranceLAPP Annecy
IPHC Strasbourg
GermanyHamburg
IsraelTechnion Haifa
ItalyBari
BolognaFrascati
LNGSNaplesPadova
RomeSalerno
JapanAichiTohoKobe
NagoyaNihon
KoreaJinju
RussiaINR RAS Moscow
LPI RAS Moscow
SINP MSU Moscow
JINR Dubna
SwitzerlandBern
TurkeyMETU, Ankara
140 physicists from 26 institutions in 11 countries
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Thank you for your attention
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Backup slides
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Measurement of the TeV atmospheric muon charge ratio
25Vertical surface energy
Eur. Phys. J. C (2014) 74:2933
Validation of the hadronic background by test beams
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Interaction rate
Dots with error bars : dataHistogram : simulation
Kink angle (1-prong events)
Black : dataRed : simulation (FLUKA)
Probability of associated nuclear fragments
Muon/hadron separation by “track follow-down"
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(primary tracks are followed until the stopping point)
: track length: range in lead of a muon: average density along the path: lead density
LR(p)<ρ>ρ
A track is classified as a muon if DTFD is above 0.8