KM3NeT The Birth of a Giant Vlad Popa, Institute for Space Sciences, Magurele-Bucharest, Romania.
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Transcript of KM3NeT The Birth of a Giant Vlad Popa, Institute for Space Sciences, Magurele-Bucharest, Romania.
![Page 1: KM3NeT The Birth of a Giant Vlad Popa, Institute for Space Sciences, Magurele-Bucharest, Romania.](https://reader038.fdocuments.us/reader038/viewer/2022110103/56649e4f5503460f94b46be3/html5/thumbnails/1.jpg)
KM3NeTThe Birth of a Giant
Vlad Popa,
Institute for Space Sciences, Magurele-Bucharest, Romania
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Overview
• Introduction: what, who and why?• Neutrino telescopes: how do they work?• Physics goals, but not only…• Present status, pilot experiments• Many choices to be made… • Conclusions
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Overview
• Introduction: what, who and why?• Neutrino telescopes: how do they work?• Physics goals, but not only…• Present status, pilot experiments• Many choices to be made… • Conclusions
![Page 4: KM3NeT The Birth of a Giant Vlad Popa, Institute for Space Sciences, Magurele-Bucharest, Romania.](https://reader038.fdocuments.us/reader038/viewer/2022110103/56649e4f5503460f94b46be3/html5/thumbnails/4.jpg)
Overview
• Introduction: what, who and why?• Neutrino telescopes: how do they work?• Physics goals, but not only…• Present status, pilot experiments• Many choices to be made… • Conclusions
![Page 5: KM3NeT The Birth of a Giant Vlad Popa, Institute for Space Sciences, Magurele-Bucharest, Romania.](https://reader038.fdocuments.us/reader038/viewer/2022110103/56649e4f5503460f94b46be3/html5/thumbnails/5.jpg)
Overview
• Introduction: what, who and why?• Neutrino telescopes: how do they work?• Physics goals, but not only…• Present status, pilot experiments• Many choices to be made… • Conclusions
![Page 6: KM3NeT The Birth of a Giant Vlad Popa, Institute for Space Sciences, Magurele-Bucharest, Romania.](https://reader038.fdocuments.us/reader038/viewer/2022110103/56649e4f5503460f94b46be3/html5/thumbnails/6.jpg)
Overview
• Introduction: what, who and why?• Neutrino telescopes: how do they work?• Physics goals, but not only…• Present status, pilot experiments• Many choices to be made… • Conclusions
![Page 7: KM3NeT The Birth of a Giant Vlad Popa, Institute for Space Sciences, Magurele-Bucharest, Romania.](https://reader038.fdocuments.us/reader038/viewer/2022110103/56649e4f5503460f94b46be3/html5/thumbnails/7.jpg)
Overview
• Introduction: what, who and why?• Neutrino telescopes: how do they work?• Physics goals, but not only…• Present status, pilot experiments• Many choices to be made… • Conclusions
![Page 8: KM3NeT The Birth of a Giant Vlad Popa, Institute for Space Sciences, Magurele-Bucharest, Romania.](https://reader038.fdocuments.us/reader038/viewer/2022110103/56649e4f5503460f94b46be3/html5/thumbnails/8.jpg)
KM3NeT will be a very large volume (> km3 ) Neutrino Telescope, to be deployed in the Mediterranean Sea, after 2012.
Introduction
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KM3NeT will be a very large volume (> km3 ) Neutrino Telescope, to be deployed in the Mediterranean Sea, after 2012.
The consortium includes 40 Institutes or Universities from 10 European countries.
The research is financed trough 2 European projects: “KM3NeT-DS” (completed), “KM3NeT-PP”, and by national agencies
There will be room for Earth and Sea Sciences.
Introduction
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KM3NeT will be a very large volume (> km3 ) Neutrino Telescope, to be deployed in the Mediterranean Sea, after 2012.
The consortium includes 40 Institutes or Universities from 10 European countries.
The research is financed trough 2 European projects: “KM3NeT-DS” (completed), “KM3NeT-PP”, and by national agencies
There will be room for Earth and Ocean Sciences.
One of the Magnificent Seven of the ASPERA Roadmap
Introduction
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KM3NeT will be a very large volume (> km3 ) Neutrino Telescope, to be deployed in the Mediterranean Sea, after 2012.
The consortium includes 40 Institutes or Universities from 10 European countries.
The research is financed trough 2 European projects: “KM3NeT-DS” (completed), “KM3NeT-PP”, and by national agencies
There will be room for Earth and Ocean Sciences.
One of the Magnificent Seven of the ASPERA Roadmap
Introduction
Official web page: http://www.km3net.org
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•Cyprus: University of Cyprus• France: CEA, CNRS, Haute Alsace University• Germany: Erlangen – Nurnberg University• Greece: Hellenic Open University, NCSR Demokritos, Athens National Observatory, Athens National University• Ireland: Advanced Study Institute, Dublin• Italy: INFN ( + Universities)• Netherlands: FOM (NIKHEF), NIOZ• Romania: ISS (INFLPR)• Spain: CSIC, Barcelona University, Valencia Technical University, Valencia University• United Kingdom: Aberdeen University, Leeds University, Sheffield University
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Neutrino telescopes: how do they work?
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Muon neutrinos (the “golden channel”):
XN
• Signature: muon (+ hadronic shower if reaction inside the detector)
• Detectability: if muon crosses light acceptance
• Measurement precision: Energy – fair (factor 2 at best for muon energies > 1TeV Direction – very good (0.1o at high energies)
• Remarks: the golden channel for point source searches (neutrino astronomy)
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Electron neutrinos
XeNe
• Signature: electromagnetic + hadronic shower (superimposed)
• Detectability: if reaction is inside detector light acceptance
• Measurement precision: Energy – good Direction – fair (a few degrees at best)
• Remarks: Important for diffuse flux measurements and flavour studies. Not distinguishable from other shower signatures.
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Tau neutrinos
XN • Signatures: 1) if like 2) if like 3) if : hadronic shower
• Detectability: if reaction is inside detector light acceptance (except 1)
• Measurement precision: Energy – fair (large fraction goes to secondary ’s) Direction – good for (1), fair otherwise
• Remarks: Important for diffuse flux measurements and flavour studies. Only double-bang signatures might be distinctive.
XN e XeNe hadrons
for E > few TeV “double bang sinature”
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All neutrinos (neutral current interactions)
XN xx • Signatures: hadronic shower
• Detectability: if reaction is inside detector light acceptance
• Measurement precision: Energy – poor (large fraction goes to secondary ) Direction – fair
• Remarks: Important for diffuse flux measurements and flavour studies. Energy measurement much less precise, not distinguishable from other shower signatures.
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Physics goals, but not only…
. Neutrino astronomy
• Diffuse neutrino flux
• Dark Matter
• Exotic Particles
• Atmospheric muons and neutrinos
• Neutrino Cross Sections
• …
• Earth and Sea Sciences
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The main scientific goal: Neutrino Astronomy
• Point Sources• Supernova Remnants• Microquasars• Gamma Ray Bursters• Hidden Sources (not seen in other “wavelengths”)
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Neutrino Astronomy: Sky coverage (Galactic coordinates)
From the South: IceCube(angular resolution~ 10 )
From the North:KM3NeT(angular resolution ~ 0.10)
> 75% of time>25% of time
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Other physics goals
• Diffuse neutrino flux
• Dark Matter
• Exotic Particles
• Atmospheric muons and neutrinos
• Neutrino Cross Sections
• …
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Diffuse neutrino energy flux
Cosmogenic (extragalactic)
C.R. p (E > 1019.5 eV) / CMB (pions, HE neutrinos)
(GZK cutt-off)
From all GRB’s and AGN’s, during the complete Universe history, extragalactic for E > 1017 – 1018 eV
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Other physics goals
• Diffuse neutrino flux
• Dark Matter
Search based on WIMPS annihilation (in the center of the Sun) leading to HE neutrinos (directly in scenarios with extradimensions, or trough massive particle decays in supersymmetric scenarios).
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Other physics goals
• Diffuse neutrino flux
• Dark Matter
• Exotic Particles
• Atmospheric muons and neutrinos
• Neutrino Cross Sections
• …
![Page 26: KM3NeT The Birth of a Giant Vlad Popa, Institute for Space Sciences, Magurele-Bucharest, Romania.](https://reader038.fdocuments.us/reader038/viewer/2022110103/56649e4f5503460f94b46be3/html5/thumbnails/26.jpg)
• GUT Magnetic Monopoles
• Intermediate mass Magnetic Monopoles
• Nuclearites
•Q-balls
• …
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Intermediate mass monopoles
GUT monopoles
Two categories
Magnetic charge g = n gD, n = 1,2,3,…? and gD= 137/2 e
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Gauge theories of unified interactions predict MMs
Mass mM ≥ mX/G > 1016 GeV ~ 0.02 g 1017 GeV
SU(5)1015 GeV
10-35 sSU(3)C x [SU(2)L x U(1)y]
102 GeV
10-9 sSU(3)C x U(1)EM
Grand Unification: virtual X,Y
Electroweak unification: W, Z
Confinement region: virtual s, gluons, condensate of fermions -antifermion, 4 fermion virtual states
B=g/r2 Magnetic field of a point Dirac monopole
Radius (cm)10-29 10-16 10-13
r few fm B ~ g/r2
Size: extended object
Slowly moving!
Proton decay catalysis
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Proton decay (Callan – Rubakov)
.........
)(
0
00
KMpM
eMpM
eMpM
227290
20 1010~17.0 cmwithc
A proton decay is expected every
10
10
2
9.5
9.5
H
H
nct
or
nL
Assuming Mon = 10-3, in water,
10 cm – 10m
30 s - 3 ms
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GUT MMs detectable trough the Cherenkov light emitted by the proton decay charged secondaries, between 3 × 104 – 105 photons with = 300 – 600 nm for each event.
A trigger should require multiple coincidences in a relatively large time window, and the efficiency of such a search depends strongly on the assumed value of 0 and Mon…
Best existing flux limit from MACRO: 1121610 srscm
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Intermediate mass MMs (105 - 1012 GeV)1994 De Rujula CERN-TH 7273/94
E. Huguet & P. Peter hep-ph/ 901370
T.W. Kephart, Q. Shafi Phys. Lett. B520(2001)313Wick et al. Astropart. Phys. 18, 663 (2003)
Produced in the Early Universe after GUT phase transitions
ex. (Shafi) M ~ 1010 GeV , g = 2 gD , no p-decay catalysis
IMMs can be accelerated in the galactic B field to relativistic
velocities
T = gD B L ~ 6 x 10 10 GeV (B/3x10-6 G) (L/300pc)
Galaxy T 6 x 1010 GeV
Neutron stars T 1011 - 1015 GeV
AGN T 1014 - 1015 GeV
Could they produce the highest energy cosmic ray showers E > 1020 eV ?
SO(10)1015 GeV
10-35 sSU(4) x SU(2) x SU(2)
109 GeV
10-23 sSU(3) x SU(2) x U(1)
Relativistic!
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Intermediate mass MMs in VLVTs
74.01
n
74.0. MonCherenkov light production
- By the monopole (and by electrons) for
- By electrons for 51.0. Mon
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Direct Cherenkov emission ( > 0.74)
22.
2
2
21
12
nng
dxd
Nd
MonD
Cherenkov emission enhanced by a factor about 8500 compared to Cherenkov light emission by a single muon
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Cherenkov light from δ rays (knock-on electrons), Mon>0.51
2
max222 /1
1535.0T
TT
A
Z
e
g
dxdT
Nd D
222
11
2
ndxd
dN
e
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Total number Cherenkov photons 300 < λ < 600 nm
Monopole•Direct• Recoil e-
Muon
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•Aggregates of u, d, s quarks + electrons , ne= 2/3 nu –1/3 nd –
1/3 ns
•Ground state of QCD; stable for 300 < A < 1057
Produced in Early Universe or in strange star collisions (J. Madsen, PRD71
(2005) 014026)
Candidates for cold Dark Matter! Searched for in CR reaching the
Earth
R (fm) 102 103 104 105 106
M (GeV) 106 109 1012 1015 1018
A qualitative picture…
[black points are electrons]
N 3.5 x 1014 g cm-3
nuclei 1014 g cm-3
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M (GeV)
1014 s e
du
u uu
u
dd
d s
ds
s s
e ee
- Essentially neutral (most if not all e- inside)- “Classical” properties: galactic velocities, elastic collisions, energy losses…- Could reach KM3NeT from above- Better flux limit from MACRO (for nonrelativistic velocities):
GeV10Mforsrscm102 1411216
M. Ambrosio et al., Eur.Phys. J. C13 (2000) 453; L. Patrizii, TAUP 2003
1010 Too low masses to reach KM3NeT
1022 Could traverse the Earth, but very low expected fluxes
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Nuclearites - basics•Typical galactic velocities 10-3
• Dominant interaction: elastic collisions with atoms in the medium• Dominant energy losses:
• Phenomenological flux limit from the local density of DM:
A. De Rújula and S.L. Glashow, Nature 312 (1984) 734
)M/g1(8.7))sr2(yrkm( 112
)cloude(ng5.1Mcm10
)insidee()GeV104.8(ng5.1M4/M3216
143/2
2
.medv
dxdE
MDM 2/v
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2
.medv
dxdE For M 8.4 1014 GeV it depends only on v2
The passage of a nuclearite in matter produces heat along its path
In transparent media some of the energy dissipated could appear as visible light (black body radiation)
The “optical efficiency” = the fraction of dE/dx appearing as light in water estimated to be = 3 10-5 (lower bound) (A. De Ruhula, S.L. Glashow, Nature 312 (1984) 734)
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ev)L(v0
L
0
.meddx)x(
M
The velocity of a nuclearite entering in a medium with v0, after a path L becomes
in the atmosphere:
a = 1.2 10-3 g cm-3; b = 8.6 105 cm; H 50 km
(T. Shibata, Prog. Theor. Phys. 57 (1977) 882.)
in water: w 1 g cm-3
ea)x(atm
bxH
At ~ 4000 m depth, nuclearites with masses larger than ~1015 GeV should bestill fast enough to produce detectable black body light. Expected light yield >106 visible photons/cm!
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Nuclearites could be seen by KM3NeT (as well as all other VLVnT’s) as correlated light hits distributed in a time window of ~ 10 ms.
Other possible exotic particles: Q-balls – nuggets of squarks and sleptons (“supersimetric nuclearites”…)
- neutral Q-balls would absorb normal hadrons emitting pions: their signature would be as for nuclearites, combined with the GUT monopole signals
- charged Q-balls would interact trough elastic collisions: would give nuclearite-like signals.
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KM3NeT sensitivity to exotic particles (one year of data tacking) should be at the level of 10-18 cm-2 s-1 sr-
1 , depending on:
• The actual geometry of the telescope• The efficiency of the dedicated triggers• The efficiency of the off-line analysis (background removal, reconstruction strategy, etc.)
Intensive simulations to be made after the completion of the telescope design…
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Other physics goals
• Diffuse neutrino flux
• Dark Matter
• Exotic Particles
• Atmospheric muons and neutrinos
• Neutrino Cross Sections
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Atmospheric muons and neutrinos
- More than 108 atm. muon (downward going) events expected each year: excellent callibration source, and CR primary composition from 10 TeV to 10 PeV
- About 100 000 atmospheric neutrino (upward going) events expected each year: very good statistics above 1 TeV, the tomography of the Earth interior possible, for E>10TeV.
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Flavor analysis
From pion photo-production: 0:2:1:: e
At distances >> oscillation length: 1:1:1:: e
For atmospheric neutrinos with E > 1 TeV, oscillation effects become negligible.
Flavor ratio at H.E. will test neutrino production mechanisms, but also hypothesis about : - neutrino decays - neutrino oscillations into sterile states - CPT & Lorentz invariance violations ….
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Other physics goals
• Diffuse neutrino flux
• Dark Matter
• Exotic Particles
• Atmospheric muons and neutrinos
• Neutrino Cross Sections: neutrino – nucleon interactions at very high energies (>> 200 GeV)
• …
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Earth and sea sciences
- continuous data collection for long periods at “high” (~1Hz) rates. - water dynamics, bioluminiscence and bioacoustics as byproducts of the telescope itself. - geophysics and seismology, geotechnics, chemistry, bio-chemistry, oceanography, biology, fisheries, environmental sciences… from dedicated junction boxes.
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KM3NeT will be part (node) of:
EMSO – European Multidisciplinary Seafloor Observatories
GMES – Global Monitoring for Environment and Security
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Present status, pilot experiments
- KM3NeT – Design Study completed (FP6)- KM3NeT – Preparatory Phase ongoing (FP7, will end in 2012)
- Construction and deployment foreseen to start mid 2012 or beginning 2013
- Telescope fully operational in 2016?
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KM3NeT takes advantage on the 3 pilot experiments
ANTARES
NEMO
NESTOR
All in the Mediterranean Sea
Most of the involved people are members of the KM3NeT
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KM3NeT takes advantage on the 3 pilot experiments
ANTARES
NEMO
NESTOR
This is why other neutrino telescopes (AMANDA, IceCUBE, Baikal, DUMAND) are not included in the list.
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KM3NeT takes advantage on the 3 pilot experiments
ANTARES
NEMO
NESTOR
-The only undersea neutrino telescope successfully deployed and tacking data
- Introducing and testing a different structure concept: the towers.
- First successful long term operation of a neutrino telescope floor at ~4000 m in 2003 .The star structure, and a new deployment strategy
- All have taught us that the marriage between neutrino physics and deep sea is not always a happy one…
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Many choices to be made…
• The site
• The telescope “architecture”
• Legal aspects and governance• Power and data transfer• Shore infrastructure• Ships and ROV’s• Industrial production• Deployment / maintenance / decommissioning strategies• …
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The site3 candidate locations, corresponding to the pilot
experiments• The depth. (Deeper is better? Not really!)• Water optical properties• Distance to the shore station• The bioluminescence• The 40K concentration• Current flow• Sediment flux• Shore infrastructure (ports, roads, airports…)• Cost effectiveness (including possible contributions from the local Governments)• Synergy with other undersea projects (GMES – Global Monitoring for Environment and Security, GOOS - Global Ocean Observing Systems, EuroGOOS, DEOS –Dynamics of Earth and Ocean System, EMSO – KM3NeT will be one of its nodes)• …
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The site3 candidate locations, corresponding to the pilot
experiments• The depth. (Deeper is better? Not really!)• Water optical properties• Distance to the shore station• The bioluminescence• The 40K concentration• Current flow• Sediment flux• Shore infrastructure (ports, roads, airports…)• Cost effectiveness (including possible contributions from the local Governments)• Synergy with other undersea projects (GMES – Global Monitoring for Environment and Security, GOOS - Global Ocean Observing Systems, EuroGOOS, DEOS –Dynamics of Earth and Ocean System, EMSO – KM3NeT will be one of its nodes)• …
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The site3 candidate locations, corresponding to the pilot
experiments• The depth. (Deeper is better? Not really!)• Water optical properties• Distance to the shore station• The bioluminescence• The 40K concentration• Current flow• Sediment flux• Shore infrastructure (ports, roads, airports…)• Cost effectiveness (including possible contributions from the local Governments)• Synergy with other undersea projects (GMES – Global Monitoring for Environment and Security, GOOS - Global Ocean Observing Systems, EuroGOOS, DEOS –Dynamics of Earth and Ocean System, EMSO – KM3NeT will be one of its nodes)• …
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58
AUV Site Surveys*
Remus 6000 AUVDeepest site 5200 mNavigational accuracy app <
10 mHigh resolution MultibeamSide scan sonarImagerySub Bottom ProfilerEtc, etc
*) courtesy of IFM-Geomar, Kiel
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Telescope architecture
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Architecture: Optical Modules
• Single large (8”, 10”) PMTs?
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Architecture: Optical Modules
• Many (31) small (~3”) PMTs?
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Architecture: the detection units. “MEDUSA”
• ANTARES-like strings.
SOMMOM
SOM
Breakout
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Architecture: the detection units “NuONE”
• NEMO-like towers.
8m
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Architecture: the detection units. “SeaWiet”
Self-sustained OMs
Many strings might be deployed in the same operation
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Decisions to be taken soon, based on intensive detector simulations and cost estimations
Common Layout91 Detector UnitsHexagon20 storeys per DU30m between storey
Compare configurationsDU spacing: 100, 130m, 160mfor each analysed configurations
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Architecture: overall layouts
Homogeneous Cluster Ring …….
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Conclusions…
Some KM3NeT-PP targets:
- Have the largest effective area at a given cost (250 M€)
- Deploy the telescope within 3 years
- Have an easily expandable facility
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More information at: http://www.km3net.org
April 2008
KM3NeT
Technical Design Report
July 2009
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Conclusions…