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The KM3NeT consortium aims at developing a deep-sea research infrastructure in the Mediterranean Sea. The construction of a multi-cubic-kilometre Cherenkov telescope for neutrinos with energies above 100 GeV is the principal KM3NeT goal. - PowerPoint PPT Presentation
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R. Coniglione INFN-LNSTEV PA Paris 19-23 July 2010
KM3NeT: a project for an underwater cubic kilometre neutrino telescope
R. Coniglione INFN-LNS for KM3NeT collaboration
The KM3NeT consortium aims at developing a deep-sea research infrastructure in the
Mediterranean Sea. The construction of a multi-cubic-kilometre Cherenkov telescope for
neutrinos with energies above 100 GeV is the principal KM3NeT goal
•Introduction•Main objectives•The KM3NeT Technical Design Report•Telescope physics performance•New developments•Summary
R. Coniglione INFN-LNSTEV PA Paris 19-23 July 2010
KM3NeT and the international context
High energy neutrino telescope world map
ANTARES, NEMO, NESTORjoined efforts to preparea km3-size neutrino telescope in the Mediterranean Sea: KM3NeT
IceCubeIC79 taking data since 2010IC59 data analysis started
AntaresTaking data in its final configuration (12 lines) since may 2008.5 lines data analyzed and ready to be published
R. Coniglione INFN-LNSTEV PA Paris 19-23 July 2010
The KM3NeT consortium
The KM3NeT consortium includes 40 Institutes from 10 European Countries (Cyprus, France, Germany, Greece, Ireland, Italy, The Netherlands, Rumania, Spain, U.K.)
KM3NeT Design Study (DS) -> define the telescope design and outline the main technological optionsApproved under the 6° FP (funded by EC for the period 2006-2009) Conceptual Design Report (CDR) published in 2008
(http://www.km3net.org/public.php)Activity of DS culminated with the publication of the Technical Design Report
(TDR) that outlines the main technological options for the construction, deployment and maintenance of a deep sea neutrino telescope (http://www.km3net.org/public.php) (TDR contents frozen in November 2009)
KM3NeT Preparatory Phase (PP) -> define legal, governance and funding aspects, production planes for the detector elements, infrastructure features and prototype validation will be also definedApproved under the 7° FP (funded by EC for the period 2008-2012)
R. Coniglione INFN-LNSTEV PA Paris 19-23 July 2010
Neutrino will provide unique info on High Energy Universe
on the origin of UHE cosmic rays (astrophysics, cosmology and particle physics)on the high energy gamma production mechanism (hadronic and/or leptonic)on the source dense inner core
Neutrino observation can be connected with the observed gamma fluxes for sources with low matter density while new high density sources can be observed
Motivation for the high energy neutrino detection
R. Coniglione INFN-LNSTEV PA Paris 19-23 July 2010
KM3NeT main objectives
Central physics goals:-Investigate neutrino “point sources” in the 1-100 TeV energy regime galactic ->Supernova Remnants, Microquasars… extragalactic -> Active Galactic Nuclei, Gamma Ray Bursts-Complement IceCube field of view-Exceed IceCube sensitivity
Other important physics items:- High energy diffuse neutrino flux detection- Indirect search of Dark Matter- Neutrino particle physics aspects- Exotics (Magnetic Monopoles, Lorentz invariance violation, …)
Interdisciplinary research- geophysics, oceanography, marine biology, …
Implementation requirements:• Construction time ≤5 years• Operation over at least 10 years
R. Coniglione INFN-LNSTEV PA Paris 19-23 July 2010
KM3NeT sky view
2 downward coverage assumed
>75%>25%
KM3NeT complements the IceCube field of view KM3NeT observes a large part of the sky (~3.5)
At the Mediterranean sea latitude the source visibility can be less than 24h
R. Coniglione INFN-LNSTEV PA Paris 19-23 July 2010
Neutrino detection principle
Interaction
point
• Upward-going neutrinos interact in rock or water ( is the golden channel for astronomy)
• Emerging charged particles (in particular muons) produce Cherekov light in water at 43° with respect to the neutrino direction
• Light detection by array of
photomultipliers
• From photon arrival times and PMT positions is possible to reconstruct the muon direction Detection volume of the order of 5 km3 to exceed IceCube sensitivity by a
substantial factor
43°
c
R. Coniglione INFN-LNSTEV PA Paris 19-23 July 2010
Technical items
The telescope consists of 3D array of photo-sensors supported by vertical structures (DU) connected to a seabed with a cable network
The construction of a deep sea neutrino telescope is technically highly challenging
Very high pressureEnvironment chemically aggressiveDeployment operation safe, robust and precise
Technical itemsOptical Modules Front-end electronicsReadout, data acquisition, data transportMechanical structures, backbone cableGeneral deployment strategySea-bed network: cables, junction boxesCalibration devicesShore infrastructureAssembly, transport, logisticsRisk analysis and quality control
Requirements
Cost-effective Reliable Producible Easy to deploy
R. Coniglione INFN-LNSTEV PA Paris 19-23 July 2010
Other issues addressed in the Design Study
Site characterization:• Characterization of the site and measure of the water properties optical background, currents, sedimentation, water properties (absorption and
scattering lengths….)
Simulation:- Detector performances (sensitivity and discovery fluxes) optimizing the
detector parameters
- Earth and Sea science requirements:• Define the infrastructure needed to implement multidisciplinary
science nodes (marine biology, geology/geophysics, oceanography, environmental studies, alerts, …)
R. Coniglione INFN-LNSTEV PA Paris 19-23 July 2010
Optical modules
Two alternative solutions in the TDR for OM
Single-PMT Optical Module8-inch PMT with 35% quantum efficiencyinside a 13 inch glass sphere
Evolution from pilot projects
Multi-PMT Optical Module31 small PMTs (3-inch) inside a 17 inch glass sphere
• 31 PMT bases (total ~140 mW)
• Cooling shield and stem
First full prototype ready at the end of 2010
R. Coniglione INFN-LNSTEV PA Paris 19-23 July 2010
Optical modules
Two alternative solutions in the TDR for OM
Single-PMT Optical ModuleAdvantages
Multi-PMT Optical ModuleAdvantages
•photocathode surface greater than 3 8-inch PMTs
•insensitive to the Earth’s magnetic field -> no mu-metal shielding
•single-photon from multi-photon hits separation
•information on the arrival direction of Cherenkov light-> better track reconstruction
• large angular acceptance
• good timing response
• well known technology
R. Coniglione INFN-LNSTEV PA Paris 19-23 July 2010
Front-end electronics: Time-over-Threshold
Common solutions in the TDR for the front-end electronics
R. Coniglione INFN-LNSTEV PA Paris 19-23 July 2010
Detection Units
Three alternative solutions in the TDR for DUs
Flexible tower with horizontal bars equipped with single-PMTs or multi-PMT OMs
Triangular arrangements of OMs with single-PMTs or multi-PMT
Evolution of the ANTARES storey
Slender stringVertical sequence of multi-PMTs OMs
Simulations indicate that local 3D OM arrangement resolve ambiguities in the reconstruction of the muon azimuthal angle
R. Coniglione INFN-LNSTEV PA Paris 19-23 July 2010
Deployment strategy
Common deployment strategy in the TDRMain deployment concepts • Compact package• Self unfurling• Connection to seabed network by Remotely Operated Vehicle
Spherical deployment structure for string with single OM with multi-PMT
The packed flexible tower(20 storey)
Successful deployment test in February 2010 Successful
deployment test in December 2009
R. Coniglione INFN-LNSTEV PA Paris 19-23 July 2010
KM3NeT: an artistic view
Primary Junction box Secondary Junction boxes
Detection Units
Electro-optical cable
R. Coniglione INFN-LNSTEV PA Paris 19-23 July 2010
Simulations: optimization studies
Bar length optimization Optimization of Detection Unit separation
Examples for the flexible tower
Low energy region100GeV<E<500 GeV
Quality cuts applied -rec~ 2° (close to the -
)
Point like sources3TeV<E<100 TeV
Quality cuts applied -rec~ 0.4°(close to the search cone radius)
Diffuse flux studies & GRBE>100 TeV
No quality cuts applied -rec 0.9°
ratio of the effective area relative to 3m ratio of the effective area relative to 100m
R. Coniglione INFN-LNSTEV PA Paris 19-23 July 2010
Simulations: optimization studies
Sensitivity ratio for point like source - 1 year – =-60°
Flexible tower
180 m preferred DU distance
Final bar length choice is a compromise between physical performance and technical constraints
Bar length
Detection unit separation
R. Coniglione INFN-LNSTEV PA Paris 19-23 July 2010
Sensitivity to point source (flux E-2) vs declination for one year of observation time
Full KM3NeT detectors made of the three DU configurations at the same cost were considered in the simulations
Similar sensitivity per euro for the three configurations
Black Slender stringRed Flexible towerGreen Triangles
A detector with a total cost of about 220M€ is required to surpass the performance of IceCube by a substantial factor
Simulation results
conceptNumber of DU for 220M€
Flexible tower with 6 8” PMT per bar 20 bars
310(2x154)
Slender strings20 floors with 1 multi-PMT per floor
620 (2X310)
Triangles 6 8” PMT per floor 20 floors
254(2x127)
R. Coniglione INFN-LNSTEV PA Paris 19-23 July 2010
KM3NeT: effective area & resolution
☐Quality Cuts applied (0.2°@30TeV) Quality Cuts optimized for sensitivity
Neutrino effective areaDetector resolutionMedian of rec
Kinematics
median of the distribution
R. Coniglione INFN-LNSTEV PA Paris 19-23 July 2010
KM3NeT: sensitivity & discovery
KM3NeT sensitivity 90%CLKM3NeT discovery 5 50%IceCube sensitivity 90%CLIceCube discovery 5 50% 2.5÷3.5 above sensitivity flux. (extrapolation from IceCube 40 string configuration)
binned method
unbinned method
| Observed Galactic TeV- sources (SNR, unidentified, microquazars) F. Aharonian et al. Rep. Prog. Phys. (2008)Abdo et al., MILAGRO, Astrophys. J. 658 L33-L36 (2007) Galactic Centre
Sensitivity and discovery fluxes for point like sources with a E-2 spectrum for 1 year of observation time
R. Coniglione INFN-LNSTEV PA Paris 19-23 July 2010
Developments after the TDR
In the recent months developments towards a technology convergence on a unique design
• “bar” option with horizontal extent and 6 8-inch PMTs– Optimised design and plan for extensive deployment tests
defined
• Study of the advantages offered by a “hibrid” solution– DU with horizontal extent– Multi-PMT Optical Module
• Multi-PMT option– Needs validation of technology and integration procedures– Common development of the multi-PMT Optical Module and its
implementation on the tower– Optimization of simulation of the detector performance ongoing
R. Coniglione INFN-LNSTEV PA Paris 19-23 July 2010
Flexible tower DU with 6 13” spheres: stacking concept
Height = 1.43 m
R. Coniglione INFN-LNSTEV PA Paris 19-23 July 2010
Flexible tower DU with 2 17” OM: preliminary storey design
R. Coniglione INFN-LNSTEV PA Paris 19-23 July 2010
Summary
• A design for the KM3NeT neutrino telescope complementing the IceCube field of view and surpassing it in sensitivity by a substantial factor is presented
• The required sensitivity can be achieved within an overall budget of ≈ 250 M€
• Staged implementation, with increasing discovery potential, is technically possible
• Convergence process toward a unique technical design under way
• Development plan for qualification of a pre-production model of the detection unit defined
• Remaining technical decisions have to be taken within the next spring
• Readiness for construction expected at the end of the Preparatory Phase (march 2012)
• Installation could start in 2013 and data taking soon after
R. Coniglione INFN-LNSTEV PA Paris 19-23 July 2010
The end
R. Coniglione INFN-LNSTEV PA Paris 19-23 July 2010
Simulations: optimization studies
Sensitivity ratio for point like source - 1 year – =-60°
Flexible tower
180 m preferred DU distance
Final bar length choice is a compromise between physical performance and technical constraints
Bar length
Detection unit separation
=-2.2
=-2
R. Coniglione INFN-LNSTEV PA Paris 19-23 July 2010
Theta versus declination
Mediterranean sea latitude 36°
-80-70
-60-50
=-40
-30-20
-10
0 +20+40 +50
Above the horizon Below the horizon
Near the horizon the effect of Earth absorption is reduced for high energy neutrinos