Point-like Source Searches
with the ANTARES and KM3NeT Neutrino Telescopes
Giulia Illuminati on behalf of the ANTARES and KM3NeT Collaborations IX CPAN DAYS - 23/10/2017 – Santander
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Outline
o Neutrino Astronomy o Neutrino telescopes
• Detection Principle
• Operating Neutrino Telescopes v ANTARES
v KM3NeT
• Event Topologies
o ANTARES point-like source analysis
• Data sample
• Analysis Method
• Results
o ANTARES on-going analyses
• ANTARES-IceCube combined analysis
• ANTARES time correlation analysis with IceCube events
o Expectations for KM3NeT
Neutrino Astronomy
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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
o Cosmic rays and photons current main cosmic messengers o CRs deflected by magnetic fields
o Photons absorbed by dense regions
𝑝 + 𝛾 → Δ' → 𝜋'+ 𝑛
𝜋' → 𝜇' + 𝜈, → 𝑒' + 𝜈. + 𝜈̅, + 𝜈,
𝜈.: 𝜈,: 𝜈1 = 1: 2: 0 𝜈.: 𝜈,: 𝜈1 = 1: 1: 1
at the source at Earth
Ø Produced in astrophysical sources where hadrons are accelerated Ø Provide a strong indication of
hadronic acceleration
𝑝 + 𝛾 → Δ' → 𝜋6+ 𝑝 𝜋6 → 𝛾𝛾 𝑛 → 𝜋7+ 𝑝
𝜋7 → 𝜇7 + 𝜈̅, → 𝑒7+ 𝜈̅.+ 𝜈̅, + 𝜈,
ν
4ν
µ
Neutrino telescopes:
Detection principle
νµ µ
N W X
key interaction:
ν
ℓ+ N -> ℓ+ X
µ
Cherenkov angle in water θC~ 42°
• Cherenkov radiation
detected by arrays of PMTs
• Position, time and charge used to reconstruct
direction and energy
• 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
ɣ
ɣ
Neutrino telescopes
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o ANTARES and KM3NeT Mediterranean Sea
o IceCube
Antartic Ice o Baikal
Lake Baikal
~ 3.5π sr sky coverage
The European neutrino telescopes:
ANTARES
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~60 m 450 m
Junction boxes
Electro-optical cable
Buoy
o Largest neutrino telescope in the Northern Hemisphere 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
The European neutrino telescopes:
KM3NeT
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KM3NeT/ARCA 36°16’ N 16°06’ E
KM3NeT/ARCA
o Under construction
o 3500 m depth in the Mediterranean Sea
o 100 km offshore from Porto Palo di Capo Passero, Sicily o 2 sparse building blocks
o 1-10 TeV energy threshold
o High-energy neutrino astronomy
KM3NeT/ORCA 42° 48’ N 06° 02’ E
KM3NeT/ORCA
o Under construction
o 2450 m depth in the Mediterranean Sea o 40 km offshore from Toulon
o 1 dense building block o GeV energies
o Oscillations, mass hierarchy
ORCA 9 m ARCA 36 m
~210 m ORCA
~1 km ARCA
3 building blocks
115 strings per building block 18 optical modules per string 31 PMTs per OM
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Event topologies - TRACKS
Track-like events:
νμ (ντ ) neutrino
CC interaction near the detector è track
ANTARES
Angular resolution < 0.4° for Eν > 10 TeV Angular resolution < 0.1° for Eν> 100 TeV
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Event topologies - SHOWERS
Shower-like events:
all neutrinos NC
νe,ντCC interaction inside or very close to the
detector è shower
ANTARES
Angular resolution < 3° Angular resolution < 1.5°
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ANTARES all-flavour neutrino point source analysis:
Data sample
sinδ
−1 −0.8 −0.6 −0.4 −0.2 0 0.2 0.4 0.6 0.8 1
s)2 cm-1 GeV8 /(10S A
0 0.5 1 1.5 2 2.5 3 3.5 4
Tracks Showers x 3
PRELIMINARY
Acceptance as a function of the source declination for a E-2 energy spectrum.
o Jan 29, 2007 to Dec 31, 2015 o 2423.6 days of lifetime
o Track and Shower events
o 7622 tracks and 180 showers
ANTARES all-flavour neutrino point source analysis:
Search method: likelihood
𝑆 9 = 𝑆 :;<=. ⋅ 𝑆 .?.@AB
𝐵 9 = 𝐵 :;<=. ⋅ 𝐵 .?.@AB
Signal PDFs
Background PDFs
log𝐿 :'H = I I log 𝜇 :9A J 𝑆 9 J + 𝑁 J 𝐵 9 J − 𝜇 :9A
9∈J J
δ
RA −1 −0.8 −0.6 −0.4 −0.2 0 0.2 0.4 0.6 sin(0.8 δtr)1
Selected track events
0 100 200 300 400 500 600 700 800
PRELIMINARY
E
Background Signal
𝑄 = log𝐿
O<P:'H− log𝐿
HTest Statistic
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Source with E-2 spectrum assumed
ANTARES all-flavour neutrino point source analysis:
Search method: strategies
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o Full-sky search
• TS evaluated in squares of 1°x1° over the ANTARES visible sky
o Galactic Centre region search
• TS evaluated in squares of 1°x1° over a restricted region around the GC:
ellipse, 15° semi-axis in galactic latitude, 20° semi-axis in galactic longitude
[1] arXiv:1405.5303
[2] PoS ICRC2015 (2016) 1081
Free parameters:
Ø 𝜇
Q@Ø 𝜇
:RØ 𝛼
:TU@=.Ø 𝛿
:TU@=.o Candidate list searches
• 106 known astrophysical objects (Pulsars, SNRs, …)
• 13 IceCube tracks from the HESE sample [1][2]
o Sagittarius A* location
• Tested as an extended source by assuming a Gaussian emission profile of various widths
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ANTARES Results: Sensitivities and Limits
Full-sky and Candidate list searches
Sensitivities and upper limits at a 90% C.L. on the signal flux from the Full-sky and the Candidate list searches
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ANTARES Results: Sensitivities and Limits
Galactic Centre region search
sinδ
−0.7 −0.6 −0.5 −0.4 −0.3 −0.2 ]-1 s-2 [TeV cm90%CL Φ2 E
16 18 20 22 24 26 28
30×10−12
= 2.0° σ
° = 1.0 σ
= 0.5° σ
= 0.0° σ
PRELIMINARY
sinδ
−0.7 −0.6 −0.5 −0.4 −0.3 −0.2
]-1 s-2 cm-1γ [TeV090%CL Φγ E
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10−
−10
10
= 2.5 γ
= 2.3 γ
= 2.1 γ
= 2.0 γ
PRELIMINARY
90% C.L. upper limits of the search restricted to the region around the origin of the galactic coordinates at (α,δ) = (266.40°,-28.94°) assuming different spectral indices for the neutrino flux (left) and different
source extensions for ɣ= 2 (right).
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ANTARES Results: Sensitivities and Limits
Sagittarius A*
°] σ [
0 1 2 3 4 5 6
]-1 s-2 [TeV cm90%CL Φ2 E 11−10
−10
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Sensitivity (assuming width) Sensitivity (assuming point-source) 90% C.L. Limit
discovery flux (assuming width) 5σ
discovery flux (assuming point-source) 5σ
PRELIMINARY
Discovery flux (solid red), median sensitivity (dotted blue) and upper limits (solid blue) at 90% C.L. for a search for an extended source at Sagittarius A* at (α,δ) = (266.42°,-29.01°)
assuming different angular extensions σ. The dashed lines correspond to the point-like source assumption.
o Exploit the complementarity of the detectors to gain in sensitivity
• Size
• Geographical location
• Atmospheric muon background
o First combined point-like source search in the Southern Hemisphere performed in 2015
• (Astrophys.J. 823 (2016) no.1, 65)
o ANTARES data from 2007 to 2012 (6 years) o IceCube from 2008 to 2011 (3 years)
• IC40, IC59, IC79
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ANTARES-IceCube combined analysis
Motivation
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ANTARES-IceCube combined analysis
Extending the analysis
o Adding more years:
- IceCube, 7 years - ANTARES, 9 years o Adding more samples:
- ANTARES
• Tracks
• Cascades - IceCube
• IC40
• IC59
• IC79
• IC86 (4 years)
• Starting tracks (IC79 + IC86 4 years)
Throughgoing tracks
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ANTARES-IceCube combined analysis
Samples
[TeV]
Eν 1
10− 1 10 102 103 104
]2 [meffA
−3
10
2
10−
−1
10 1 10 102
103
Graph
µ CC + ν νµ
ANTARES
e CC + ν νe
ANTARES
µ CC + ν νµ
IC Through-going µ
µ CC + ν νµ
µ IC Starting
Graph
ANTARES -90° < δ < -45°
IC Through-going µ -90° < δ < -30°
IC Starting µ -90° < δ < -5°
[TeV]
Eν
1 10 102 103 104
]° [Ψ∆
−1
10 1
Graph
ANTARES tracks ANTARES cascades IC Through-going µ IC Starting µ
Graph
Effective area Median angular resolution
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ANTARES time correlation analysis
IceCube neutrino candidates
HESE ID Obs. Time (MJD) Decl. (deg.) R.A. (deg.) Med. Angular error (deg.)
3 55451.07075 -31.2 127.9 1.4
5 55512.55163 -0.4 110.6 1.2
8 55608.82013 -21.2 -177.6 1.3
13 55756.11298 40.3 67.9 1.2
18 55923.53182 -24.8 -14.4 1.3
23 55949.56932 -13.2 -151.3 1.9
28 56048.57042 -71.5 164.8 1.3
37 56390.18876 20.7 167.3 1.2
38 56470.11038 14.0 93.3 1.2
43 56628.56885 -22.0 -153.4 1.3
44 56671.87788 0.0 -23.3 1.2
45 56679.20447 -86.3 -141.0 1.2
53 56767.06630 -37.7 -121.0 1.2
§ 13 HESE tracks in the ANTARES field of view (arXiv:1405.5303 , PoS(ICRC2015)1081)
§ Each HESE is treated as potential transient neutrino source
§ Search for astrophysical neutrinos in small time windows around source flares
§ First event observed in September, 2010
§ Last event observed in April, 2014
ANTARES time correlation analysis:
Search method: likelihood
𝑆 9 = 𝑆 :;<=. ⋅ 𝑆 .?.@AB ⋅ 𝑆 Q9O.
𝐵 9 = 𝐵 :;<=. ⋅ 𝐵 .?.@AB ⋅ 𝐵 Q9O.
Signal PDFs
Background PDFs
log𝐿 :'H = I I log 𝜇 :9A J 𝑆 9 J + 𝑁 J 𝐵 9 J − 𝜇 :9A
9∈J J
𝑄 = log𝐿
:'H− log𝐿
HTest Statistic
day t0 day
σ0
σ0 = flare duration t0 = source obs time
# of data
events per day
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ANTARES time correlation analysis:
5σ Discovery potential for HESE3
(days) σt
1 10 102
)σ> (50%@5 s <n
0 2 4 6 8 10 12 14 16
18 Time dependent analysis
Time integrated analysis
Time dependent analysis without energy estimator Time integrated analysis without energy estimator
PRELIMINARY
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Expectations for KM3NeT/ARCA
Strategies
q Only up-going track-like events
(estimated contribution from cascades from previous analyses ~ 20%) q Discovery fluxes for:
o Generic point-like source with spectrum ∝E-2
o Benchmark fluxes from candidate Galactic neutrino sources
v Expected neutrino fluxes estimated from the observed ɣ-ray spectra following [1] (RXJ1713.7-3946(1) from [2]) v Assumptions:
• Hadronic scenario for the ɣ-ray production
• Transparent sources
[1] F. Vissani, Astr. Phys. 26 (2006) 310
[2] S. R. Kelner, Phys. Rev. D 74 (2006), 063007
Φ0 [10-11TeV-1 s-1 cm-2]
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KM3NeT/ARCA Results:
Galactic Sources analysis
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KM3NeT/ARCA Results:
E
-2spectrum
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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
Ø No significant clustering at any point of the sky, including the intriguing accumulation close to the galactic center Ø ANTARES is an ideal candidate for a follow-up study of the IceCube “hotspot”
Ø No significant evidence of cosmic neutrino sources found in the last point-source analysis
Ø Most sensitive limits for a large fraction of the Southern Sky set, especially at neutrino energies below 100 TeV Ø NEXT: Expected improvement in the Southern sky combining ANTARES and IceCube data
Ø NEXT: Possibility of constraining the origin of the IceCube astrophysical signal from transient sources Ø Detector combining a km3-size with high visibility towards the Galactic Centre needed
Ø KM3NeT/ARCA is expected to make definite statements about neutrino fluxes from Galactic candidates in a few years of operation
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Backup
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Candidate list
arXiv:1706.01857
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IceCube HESE candidates
arXiv:1706.01857
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Selection criteria
arXiv:1706.01857
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Selection criteria
Track-like events selection cuts
§ Quality parameter: Λ
tr> -5.2
§ Estimated angular error: β
tr< 1°
§ Up-going: cosθ
tr> -0.1
§ Energy estimator: log
10(𝜌) > 1.6
§ Muon track length: L
μ> 360 m
Shower-like events selection cuts
§ Track veto: not selected as track
§ Estimated angular error: β
sh< 1°
§ Up-going: cosθ
sh> -0.1
§ Interaction vertex: R
sh< 300 m, |Z
sh| < 250 m
§ M-estimator: Mest < 1000
§ Random Decision Forest: RDF > 0.3
§ Muon likelihood: 𝓛
μ> 50
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Systematic uncertainties
tr) sin(δ
−1 −0.8 −0.6 −0.4 −0.2 0 0.2 0.4 0.6 0.8 1
Selected track events
0 100 200 300 400 500 600 700 800
PRELIMINARY
sh) sin(δ
−1 −0.8 −0.6 −0.4 −0.2 0 0.2 0.4 0.6 0.8 1
Selected shower events
0 5 10 15 20 25 30 35
PRELIMINARY
o Absolute Pointing Accuracy Uncertainty
0.13° uncertainty on the horizontal (ϕ) direction 0.06° uncertainty on the vertical (𝜃) direction
o Angular Resolution Uncertainty
15% (12%) degradation on the angular resolution in the track (shower) channel
o Acceptance Uncertainty
15% uncertainty
o Background Uncertainty
declination-dependent distribution of background events parameterized as a linear combination of the two different spline functions (the red and blue
lines)
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The IceCube detector
Antarctic ice
1450 m depth
5160 DOMs
1 km
333
The IceCube signal
Six years HESE analysis, events with interaction vertices contained within the instrumented volume PoS(ICRC2017)981
X tracks, + showers Ɣ = 2.92
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The IceCube signal
Six years HESE analysis, events with interaction vertices contained within the instrumented volume PoS(ICRC2017)981
Ɣ = 2.92
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The IceCube signal
Eight years
complementary measurement using CC νµ events where the interaction vertex can be outside this volume PoS(ICRC2017)1005
Purely
atmospheric origin excluded at 5.6σ
significance Ɣ = 2.19
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Neutrino interactions
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