Searches for point-like sources of cosmic neutrinos with the ANTARES
telescope
Giulia Illuminati on behalf of the ANTARES Collaboration X CPAN DAYS - 29/10/2018 – Salamanca
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Neutrino Astronomy
Neutrinos:
• electrically neutral -> trajectory not affected by magnetic fields, point back to the source
• stable -> travel long distances
• weakly interacting -> penetrate regions which are opaque to photons
𝑝 + 𝛾 → Δ' → 𝜋'+ 𝑛
𝜋' → 𝜇' + 𝜈, → 𝑒' + 𝜈. + 𝜈̅, + 𝜈,
Ø Provide a strong indication of hadronic acceleration in astrophysical sources
𝜈.: 𝜈,: 𝜈1 = 1: 2: 0 𝜈.: 𝜈,: 𝜈1 = 1: 1: 1
at the source at Earth
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µ
Cherenkov angle in water θC~ 42°
• Cherenkov radiation
detected by arrays of PMTs
• Position, time and charge used to reconstruct
direction and energy
ɣ
ɣ
ν
ν
µ
νµ µ
N W X
key interaction (CC):
ν
ℓ+ N -> ℓ+ X
• Earth used as shield against up-going atmospheric muons
• Detector deployed in deep water/ice to reduce down-going atmospheric muons
• Low ν cross section requires large detector volumes
• Either CC or NC interaction with a nucleus inside or nearby the
detector volume
Neutrino telescopes:
Detection principle
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Global Neutrino Network (GNN)
o ANTARES and KM3NeT Mediterranean Sea o IceCube
Antarctic Ice o Baikal
Lake Baikal
~ 3.5π sr sky coverage
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The ANTARES neutrino telescope
~60 m 450 m
Junction boxes
Electro-optical cable
Buoy
o First detection line installed in early 2006 o Completed in 2008
o 2475 m depth in the Mediterranean Sea o 40 km offshore from Toulon
• Three-dimensional array of 885 PMTs
• 12 vertical lines, 25 storeys
• 3 PMTs per storey
• PMT facing 45° downwards
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Event topologies: TRACKS and SHOWERS
Track-like events:
νμ (ντ ) neutrino
CC interaction near the detector
è track
Angular resolution < 0.4° for Eν > 10 TeV Angular resolution < 3°
Shower-like events:
all neutrinos NC
νe,ντCC interaction inside or very close to the
detector è shower
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ANTARES standard point-source search method
Maximum likelihood ratio approach
𝑆 7 = 𝑆 89:;. ⋅ 𝑆 .=.>?@
𝐵 7 = 𝐵 89:;. ⋅ 𝐵 .=.>?@
Signal PDFs:
Background PDFs:
δ
RA
E
Background
Signal
Source with E
-ɣspectrum assumed
𝐿 𝑛
C, 𝛾, … = F F [ 𝑛
CH𝑁
H𝑆
7H+ 1 − 𝑛
CH𝑁
H𝐵
7H]
7∈H
H
𝑇𝑆 = −2 log 𝐿 𝑛
C= 0
𝐿 𝑛Q
C, 𝛾Q
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Recent searches for point-sources
1) Search for neutrinos from TXS 0506+056
1.1) Online search
1.2) Time integrated search 1.3) Time dependent search
2) Search for time and space correlation between ANTARES data and IceCube high-energy events
3) ANTARES-IceCube combined search for point-sources
1) TXS 0506+056
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• IceCube-170922A detected on 22 September, 2017
• ~290 TeV neutrino induced muon track
• High probability of being of astrophysical origin
• Coincident in direction and time with a gamma-ray flare from the blazar TXS 0506+056 (Fermi-LAT, MAGIC)
• 9.5 years of IceCube neutrino observations investigated to search for excess emission at the position of TXS 0506+05
• 3.5σ evidence for neutrino emission from the direction of the blazar between September 2014 and March 2015 found
Three different searches for neutrino candidates, associated with the IceCube-170922A event or from the direction of TXS 0506+056,
performed by the ANTARES Collaboration
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1.1) TXS 0506+056: Online search
Visibility map for the ANTARES detector of IC170922A (x) in equatorial coordinates
.• Alert of extremely High Energy (EHE) track event
• Searches in the ANTARES online data stream for up- going muon neutrinos in a 3º cone centered on the IceCube event coordinates in two time-windows centered on the event time:
• ±1 h
• ±1 day (46% visibility probability)
• No coincident up-going muon neutrino recorded
• 90% C.L. fluence upper limit for a RSRT ∝ 𝐸WX source:
Spectrum 90% C.L. FluenceU.L. [GeV cm−2] 5%-95%
energy range
E-2.0 15 3.3 TeV – 3.4 PeV
E-2.5 34 450 GeV – 280 TeV
(RA, δ) = (77.43º, 5.72º) 14.2º below the horizon
1.2) TXS 0506+056: Time integrated search
Standard fixed source analysis applied to the 2007-2017 ANTARES data (livetime: 3136 days)
• Best fitted # of signal events 𝜇
87?= 1.03
• 3.4% pre-trial p-value
• 90% C.L. flux upper limits on the flux:
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Events close to TXS 0506+056 in the ANTARES data:
13 track-like and1shower-like candidates within 5º
Spectrum Φ
Z[[TeV
\[% [10WZ^ GeV−1cm−2s−1]
E-2.0 1.6
E-2.3 1.4
E-2.5 1.0
Closest event at 0.3º from the source position Recorded on December 12, 2013 Only 9% of ν events have higher estimated energy
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1.3) TXS 0506+056: Time dependent search
P𝐷𝐹 = 𝑃
89:;.⋅ 𝑃
.=.>?@⋅ 𝑃
c7d.t0 t σ t0 = MJD 57004 σ = 55 days
Δt = 550 flaring days (±5σ)
t Background time PDF estimated from data
Gaussian flare
t
Box flare
tstart tend
tstart= MJD 56937.81 tend = MJD 57096.21 Δt = 158.40 flaring days
𝐿 𝑛
C= F F [ 𝑛
CH𝑁
H𝑆
7H+ 1 − 𝑛
CH𝑁
H𝐵
7H]
7∈H H
• ANTARES time dependent search method
• Two signal time profiles provided by the IceCube Coll.
• Gaussian flare (centered on December 13, 2014)
• Box flare (centered on December 26, 2014)
• No signal found during either of the considered flares
• 90% C.L. upper limits on the neutrino flux:
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Spectrum 𝛷Z[[\[%TeV [10WZ^ GeV−1cm−2s−1]
E-2.0 4.6
E-2.1 4.4
E-2.2 4.2
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2) Time correlation with IceCube events
tobs day σ
σ= flare duration tobs= source
observation time
P𝐷𝐹 = 𝑃
89:;.⋅ 𝑃
.=.>?@⋅ 𝑃
c7d.E
Background Signal
δ
RA
Maximum likelihood method
Four free parameters:
• number of signal events
• signal spectral index
• flare duration
• source position
Candidates:
54 IceCube high energy neutrino events ANTARES data sample:
6310 tracks 147 cascades
(days) σt
−1
10 1 10 102
) σ(50%@5s n
0 2 4 6 8 10 12 14 16
Time dependent analysis, E-2.5
Time integrated analysis, E-2.5
Time dependent analysis, E-2.0
Time integrated analysis, E-2.0
PRELIMINARY
PRELIMINARY
log𝐿
8'f= g g log 𝜇
87?H𝑆
7H+ 𝑁
H𝐵
7H− 𝜇
87?7∈H H
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sinδ
1
− −0.8 −0.6 −0.4 −0.2 0 0.2 0.4 0.6 0.8 1
]-2 Fluence [Gev cm
1 10 102
103
S(E) = E-2.0
Limits Sensitivity
S(E) = E-2.0
γ
2 2.1 2.2 2.3 2.4 2.5
,ICν90 N
0 0.5 1 1.5 2 2.5 3 3.5 4
EHE27 HESE45
sinδ
1
− −0.8 −0.6 −0.4 −0.2 0 0.2 0.4 0.6 0.8 1
]-2 Fluence [Gev cm
1 10 102
103
S(E) = E-2.5
Limits Sensitivity
S(E) = E-2.5
𝑁hi\[% = j Φ[,Xkl ×𝐴.oohi ×𝐸WX𝑑𝐸
PRELIMINARY PRELIMINARY
PRELIMINARY
No correlation with IceCube events observed.
90% C.L. upper limits on fluence:
90% C.L. upper limit on the number of signal events expected to be observed by IceCube
2) Time correlation with IceCube events
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3) ANTARES-IceCube combined analysis
Complementarity for the Southern sky:
• Size
• Geographical location
• Atmospheric muon background
~60 m 450 m
Junction boxes
Electro-optical cable
Buoy
[TeV]
Eν 1
10− 1 10 102 103 104
]2 [meffA
3
10− 2
10− 1
10−
1 10 102
103
Graph
ANTARES IceCube
Graph
Effective Area Data sample:
• 9 years of ANTARES data (tracks and showers)
• 7 years of IceCube data (through-going tracks)
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3) ANTARES-IceCube combined analysis
sinδ
−1 −0.8 −0.6 −0.4 −0.2 0
] -1 s-2 [GeV cmν/dEΦ dν2 E
−9
10
−8
10
−7
10
= 2.0 90% C.L. Sensitivity for γ
IceCube 7 years ANTARES 9 years IceCube+ANTARES
= 2.0 90% C.L. Sensitivity for γ
sinδ
−1 −0.8 −0.6 −0.4 −0.2 0
] -1 s-2 [GeV cmν/dEΦ dν2 E
7
10− 6
10−
−5
10
= 2.5 90% C.L. Sensitivity for γ
IceCube 7 years ANTARES 9 years IceCube+ANTARES
= 2.5 90% C.L. Sensitivity for γ
90% C.L. sensitivity for different energy source spectra
RSRT∝ 𝐸
WXPRELIMINARY PRELIMINARY
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Conclusions
Ø Neutrinos are expected to provide complementary information to gamma-rays and protons of the high-energy universe
Ø IceCube has shown the first evidence for high-energy astrophysical neutrinos from a diffuse isotropic flux and the first association with a point-source
Ø Three different searches for neutrino candidates in the ANTARES data promptly triggered by the detection of IC170922A and the subsequent potential association with TXS 0506+56
Ø Time correlation analysis performed to possibly constrain the origin of the IceCube astrophysical diffuse signal from transient sources
Ø No significant evidence of cosmic neutrino sources found
Ø Most sensitive limits for a large fraction of the Southern Sky set, especially at neutrino energies below 100 TeV, expected to be significantly improved by combining ANTARES and IceCube data
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Backup
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Neutrino candidates registered by the ANTARES detector within an angular distance ∆Ψ from TXS 0506+056.
2) Time integrated search for neutrinos from
TXS 0506+056