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P. Sapienza, R. Coniglione and C. Distefano

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Presentation on theme: "P. Sapienza, R. Coniglione and C. Distefano"— Presentation transcript:

1 P. Sapienza, R. Coniglione and C. Distefano
Point source sensitivity and response to atmospheric muons for different orientation of the PMTs in a tower detector P. Sapienza, R. Coniglione and C. Distefano preliminary results

2 Outlook Angular acceptance for cosmic neutrino detection
Neutrino effective area and angular resolution vs PMT orientation Response to atmospheric muons and rejection Neutrino point source sensitivity To be done list

3 Mission of the session detector design Ch
Mission of the session detector design Ch. Spiering - vlvnt, Amsterdam october 2003

4 Detector geometry and simulation input
number of towers 169 (13x13) tower distance (m) 140 Floor lenght 20 PMT type & QE 10” - 23% number of OM/storey 4 number of PMT 12168 storey distance (m) 40 total PMT catode area (m2) 535 instr. volume (km3) 1.92 ANTARES code modified for km3 detectors neutrino and atm. muon generation water absorption and scattering optical background isotropic distributed around the event time window event trigger based on local coincidences and high charge Reconstruction based on maximum likelihood Detector paramiters NOT optimized! See Rosa talk’s

5 Neutrino effective areas
Quality cuts applied No quality cuts 0° - 30° 30° - 60° 60° - 90° 90° -120° 169 towers QE max 23%  169 towers QE max 35% 169 towers QE max 45% ▬ ref det with QE 33%

6 High energy neutrino detection
dh  ud  dd 100 TeV < E < 100 PeV qn-m Response to high energy neutrinos not sensitive to PMT orientation

7 Median and effective areas
dh ud dd dh dd ud dh dd ud qn-m qn-m dh/ud dd/ud

8 Angular resolution and effective areas 1 TeV<En<100 TeV
dh  ud  dd after quality cuts L qn-m up-down configuration exhibits a lower Aeff especially for horizontal events

9 Atmospheric muons Sensitivity to neutrino point sources imply rejection of atmospheric muons mis-reconstructed as up-going Detection of the moon shadowing for absolute pointing Evaluation of sensititivity to neutrino diffuse fluxes for several detector depths Code: Mupage v2r2 at 2400, 3400 and 5000 m depth

10 Atmospheric muon zenith angles
q reconstructed atmospheric muons (full line) q atmospheric muons mis-reconstructed as up-going in a 1° bin around a d=-60° source (dashed line (x 700)) qm

11 Atmospheric muons - Mupage v2r2
orientation ud atm. ric. atm. ric. up 155948 atm. ric. up after q. c. on L 2164 dd 220689 2341 dh 183761 1047 Energy threshold on muon bundle 3 TeV livetime 44 h (212 days in 1°around d=-60°) depth 3400 m

12 Signal and background source with d=-60° E-2 dN/dE = 10-9 cm-2 GeV sr-1 x 0.2 Source a = -2 Source a = -2.2 Source a = -1.8 Atmospheric n Number of expected n / year Atmospheric muons (Ebundle >3 TeV) Atmospheric n

13 Point source sensitivity d=-60°
dh  ud  dd a dh dd ud 2 2.2

14 Atmospheric muons vs detector depth
Energy threshold on muon bundle 3 TeV 212 day livetime around a point source with d=-60° and a=-2. lower curves represent atmospheric neutrino fluxes at three depths. 2400 m m m depth [m] sensitivity 2400 1.95x10-9 3400 1.96x10-9 5000 1.92x10-9 L

15 Summary detection efficiency for HE neutrinos DOES NOT depend on PMT orientation up-down configuration SEEMS to be sligtly disfavoured with respect to down-down and down-horizontal configurations for point source search

16 To do list improve optical background filtering and reconstruction
simulations with new Mupage version and improved statistics sensitivity for diffuse flux (at 2400, 3400 and 5000 m depths) sensitivity to Dark Matter Moon shadow detection


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