1
XXIII International Conference on Neutrino Physics and Astrophysics 2008 Christchurch, New Zealand Contacts: [email protected] [email protected] Detector Design Studies for a Cubic Detector Design Studies for a Cubic Kilometre Deep Sea Neutrino Telescope Kilometre Deep Sea Neutrino Telescope – KM3NeT – KM3NeT J. Carr 1 , F. Cohen 2 , D. Dornic 1 , F. Jouvenot 3 , G. Maurin 4 and C. Naumann 4 for the KM3NeT consortium 1 CPPM – Centre de Physique des Particules de Marseille, CNRS/IN2P3, France 2 IReS - Institut de Recherches Subatomiques, Strasbourg, France 3 previously University of Liverpool, Oliver Lodge Laboratory – United Kingdom 4 CEA Saclay – DSM/IRFU – Service de Physique des Particules, France The case for a km 3 neutrino telescope Many known astrophysical objects such as AGNs, GRBs and SNRs, are expected to also produce TeV – PeV neutrinos by means of hadronic acceleration. Dark matter, accumulated in gravitational wells, is also expected to create neutrino signatures. In both cases, a detector volume of the order of cubic kilometres will be necessary. To achieve this goal, the European KM3NeT consortium is currently in the preparatory phase for the construction of a cubic-kilometre neutrino telescope in the Mediterranean Sea. Similar to its South Pole counterpart IceCube, it will be able to survey a large part of the galactic plane and the extragalactic sky, while its location on the northern hemisphere will also allow it to directly view the galactic centre. fixed: 127 strings variable: string spacing 3 optical modules = 10’’ PMTs variable tilt (9525 in total) 25 storeys, variable spacing Example: Hexagonal Geometry (m) (m) X X Expected Performance (for NESSY Result) Hexagonal Configuration with - 225 strings spaced by 100 m - 25 storeys each, PMTs tilted 45° Towards a cubic kilometre detector in water scale up – too expensive – too complicated – not easily scalable (readout bandwidth, power, ...) new design dilute absorption in water limits possible sensor spacing sensitivity loss effective area 2 - 3 x IceCube muon angular resolution: 0.2° at 10 TeV – expected sensitivity after 1 year of data taking: 2.4 x 10 -12 TeV -1 cm -2 s -1 for generic E -2 sources – event rates for known TeV gamma sources (5 years): test performance for various sets of geometry parameters Expected fluxes require a detector volume of at least 1 km 3 But: current sub-km 3 designs cannot just be scaled up ! Perform Monte-Carlo design study to establish optimised geometry New design optimised for: – sensitivity / cost fast and easy installation – lifetime and stability S ource N am e D etection R econstruction R XJ1713.7-3946 3.4 /17.3 1.4 /8.1 R XJ0852.0-4622 3.5 /43.3 1.4 /19.6 N /N atm w ith E > 1 TeV Design Study with the “NESSY” tools – simulation and reconstruction/analysis chain detailed semi-analytic simulation of light generation and propagation – originally developed in Mathematica (1) framework Fast and flexible approach to test a range of physics parameters (absorption, scattering) detector geometries DAQ systems (thresholds, timing, etc) Distance between lines reconstruc tion detector simulation physics simulation water parameters ( abs , scattering ) background ( 40 K, biolum.) detector geometry front-end hardware photomultiplier tubes PMT configuration in the storey (number, distance, tilt) effective area and angular resolution optimal string distance = 100 m (balance between total volume and density) optimum PMT configuration (for constant number of OMs): PMTs tilted by 45° (“standard”) N strings =cons t. (1) Wolfram Mathematica™ (www.wolfram.com) exemplary results for hexagonal test geometry 1 distance of PMT from string axis (standard=0.5 m) (1)

Detector Design Studies for a Cubic Kilometre Deep Sea Neutrino Telescope – KM3NeT

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Distance between lines. Detector Design Studies for a Cubic Kilometre Deep Sea Neutrino Telescope – KM3NeT. J. Carr 1 , F. Cohen 2 , D. Dornic 1 , F. Jouvenot 3 , G. Maurin 4 and C. Naumann 4 for the KM3NeT consortium - PowerPoint PPT Presentation

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Page 1: Detector Design Studies for a Cubic Kilometre Deep Sea Neutrino Telescope – KM3NeT

XXIII International Conference on Neutrino Physics and Astrophysics 2008

Christchurch, New Zealand

Contacts: [email protected] [email protected]

Detector Design Studies for a Cubic Kilometre Detector Design Studies for a Cubic Kilometre Deep Sea Neutrino Telescope – KM3NeTDeep Sea Neutrino Telescope – KM3NeT

Detector Design Studies for a Cubic Kilometre Detector Design Studies for a Cubic Kilometre Deep Sea Neutrino Telescope – KM3NeTDeep Sea Neutrino Telescope – KM3NeT

J. Carr1, F. Cohen2, D. Dornic1, F. Jouvenot3, G. Maurin4 and C. Naumann4

for the KM3NeT consortium

1 CPPM – Centre de Physique des Particules de Marseille, CNRS/IN2P3, France2 IReS - Institut de Recherches Subatomiques, Strasbourg, France3 previously University of Liverpool, Oliver Lodge Laboratory – United Kingdom4 CEA Saclay – DSM/IRFU – Service de Physique des Particules, France

The case for a km3 neutrino telescopeThe case for a km3 neutrino telescopeMany known astrophysical objects such as AGNs, GRBs and SNRs, are expected to also produce TeV – PeV neutrinos by means of hadronic acceleration.Dark matter, accumulated in gravitational wells, is also expected to create neutrino signatures.In both cases, a detector volume of the order of cubic kilometres will be necessary.

To achieve this goal, the European KM3NeT consortium is currently in the preparatory phase for the construction of a cubic-kilometre neutrino telescope in the Mediterranean Sea. Similar to its South Pole counterpart IceCube, it will be able to survey a large part of the galactic plane and the extragalactic sky, while its location on the northern hemisphere will also allow it to directly view the galactic centre.

fixed: 127 strings

variable: string spacing

3 optical modules

= 10’’ PMTs

variable tilt

(9525 in total)

25 storeys,

variable spacing

Example: Hexagonal GeometryExample: Hexagonal Geometry

(m)

(m)

X X

Expected Performance (for NESSY Result)Expected Performance (for NESSY Result)

Hexagonal Configuration with

- 225 strings spaced by 100 m

- 25 storeys each, PMTs tilted 45°

Hexagonal Configuration with

- 225 strings spaced by 100 m

- 25 storeys each, PMTs tilted 45°

Towards a cubic kilometre detector in waterTowards a cubic kilometre detector in water

scale up – too expensive– too complicated– not easily scalable(readout bandwidth, power, ...)

new designdilute

absorption in water limits possible sensor spacing

sensitivity loss

– effective area 2 - 3 x IceCube

– muon angular resolution: 0.2° at 10 TeV

– expected sensitivity after 1 year of data taking:2.4 x 10-12 TeV-1 cm-2 s-1 for generic E-2 sources

– event rates for known TeV gamma sources (5 years):

test performance for various sets of geometry parameters

Expected fluxes require a detector volume of at least 1 km3…But: current sub-km3 designs cannot just be scaled up !

Perform Monte-Carlo design study to establish optimised geometry

New design optimised for:– sensitivity / cost– fast and easy installation– lifetime and stability

Source Name Detection ReconstructionRXJ1713.7-3946 3.4 / 17.3 1.4 / 8.1RXJ0852.0-4622 3.5 / 43.3 1.4 / 19.6

N / Natm with E > 1 TeV

Design Study with the “NESSY” toolsDesign Study with the “NESSY” tools

– simulation and reconstruction/analysis chain– detailed semi-analytic simulation of light generation and propagation– originally developed in Mathematica(1) framework

Fast and flexible approach to test a range of– physics parameters (absorption, scattering)– detector geometries– DAQ systems (thresholds, timing, etc)

Fast and flexible approach to test a range of– physics parameters (absorption, scattering)– detector geometries– DAQ systems (thresholds, timing, etc)

Distance between linesreconstruction

detector simulation

physics simulation

water parameters (abs, scattering)background (40K, biolum.)

detector geometry

front-end hardware

photomultiplier tubes

PMT configuration in the storey(number, distance, tilt)

effective area and angular resolution

optimal string distance = 100 m(balance between total volume and density)

optimum PMT configuration(for constant number of OMs): PMTs tilted by 45° (“standard”)

Nstrings=const.

(1)Wolfram Mathematica™ (www.wolfram.com)

exemplary results for hexagonal test geometry

exemplary results for hexagonal test geometry

1distance of PMT from string axis (standard=0.5 m)

(1)