Measurement of light scattering in deep sea

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1 Hellenic Nuclear Physics Society HNPS-2016 June 3-4, 2016 Athens-Greece Measurement of light scattering in deep sea Konstantia Balasi Collaborators: N. Maragos, M. Maniatis, D. Lenis, T. Domvoglou, I. Kiskiras Head of research: G. Stavropoulos Institute of Nuclear and Particle Physics NCSR Demokritos

2 Outline 2/20 Outline Introduction --Motivation for performing the experiment --KM3NeT experiment Scattering model Experimental set up description --the light source sphere --the detector sphere Test of the electronics / laser sources Deployment - Results Summary-Conclusions

3 Introduction 3/20 Motivation Large volume deep sea observatory for the detection of cosmic point-like neutrino sources purpose: detect Cherenkov photons Charged-current reactions Neutral-current reactions optical properties of the sea water of great ineterest for deep underwater detectors

4 Introducton 4/20 KM3NeT experiment KM3NeT DOM: 31 PMTs each 3-inches Event simulation and reconstruction methods: o particles producing the light o PMT functional characteristics o optical photon processes in the sea water Optical processes in the sea water: o Absorption o Scattering: Rayleigh scattering from sea water molecules Mie scattering from macroscopic particles in sea water

5 Scattering model 5/20 Scattering Model Use combination of Rayleigh and Mie scattering scattering angle distr. p: Rayleigh contribution θs: scattering angle Rayleigh phase function Mie phase function HINPW3 2016, Athens-Greece

6 Site selection 15/20 Site Selection ---Close to the coast --- depth of 4500 m ---Good optical properties in water ---Low level of bioluminescence ---Low rate of sedimentation ---Low velocity bottom current HINPW3 2016, Athens-Greece HNPS 2016, Athens-Greece

7 Experimental set up description 6/20 Experimental set up Each OM will be attached in is own 5 m long metal girder The experimental setup will be deployed tree times inside the deep sea water, each time with different distance between the OMs. (10, 15, 20 m respectively) A metal disk attached at the other end of the Light Sources OM girder will be used as a field stop, stop to prevent blinding of the detectors from direct (un-scattered) light.

8 Experimental set up description 7/20 Light Source Diode lasers at 405,450,520 nm The pulse time distribution of the 450 nm diode laser as measured with an APD Pulse width ~ 10 ns Pulse energy ~ 2 pj Repetition rate ~ 1 MHz

9 Experimental set up description 8/20 Apparatus

10 Experimental set up description 9/20 Detector HAMAMATSU H PMT ultra bialkali QE=30% Pulse-pair resolution: 20 ns Effective area: ф8 mm Dark Count: 50 Hz

11 Experimental set up description 10/20 Apparatus

12 Simulation 10/20 Simulation

13 Simulation-Results 10/20 Results

14 Test of electronics 11/20 Test of the FPGA/electronics system Column 1 Column 2 Column Row 1 Row 2 Row 3 Row 4

15 Test of electronics 12/20 Delay of underwater connection cable under pressure

16 Test of electronics 13/20 Voltage drop under pressure

17 Scanning laser sources 14/20 Scanning the laser sources

18 Deployment 16/20 Deployment with the Aegeon ship of the HCMR

19 Deployment 17/20 Deployment with the Aegeon ship of the HCMR HINPW3 2016, Athens-Greece

20 Results 18/20

21 Conclusion 1)study the design of an experimental set up for in situ measurement of the scattering parameters in deep sea 2)deployed with success 3)processing data 4)almost ready for publication

22 Thank you for your attention Pylos, 2016 HNPS 2016, Athens-Greece

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