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Optical Time Projection Chamber

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Presentation on theme: "Optical Time Projection Chamber"— Presentation transcript:

1 Optical Time Projection Chamber
for radon and thoron detection Wojciech Dominik Zenon Janas Krzysztof Miernik Marek Pfützner Institute of Experimental Physics Warsaw University

2 Optical Time Projection Chamber
PMT CCD visible light 1 ms/cm Gate 1 atm. gas: 49 % He 49 % Ar 1 % N2 1 % CH4 M. Ćwiok et al., IEEE TNS, 52 (2005) 2895

3 OTPC at Warsaw Materials used: Chamber active volume: 20 x 20 x 15 cm3
Stesalit fibreglass PCB plates Pyrex optical window

4 Registration of a particle
CCD PMT

5 Principle of 3D track reconstruction
z a vdt2 vdt1 Lxy Total track length: Inclination angle: vd– electron drift velocity  10 mm/ms

6 What one can measure with OTPC ?
length and position on XY plane (from camera picture) length of projection on Z axis (from the length of the PMT signal) no Z coordinate energy (from the total track length) charge of the particle (from the energy loss) time and position correlation between succesive a-decays - no sensitivity for electrons

7 Example: 214Po a-decay CCD Dt= 5 ms PMT Lxy=115 mm

8 Example: energy loss along the particle track
projection of CCD picture fit of Bethe-Bloch formula

9 Example: correlation between succesive a-decays
T= 0 min a 222Rn T= 3 min a 218Po - tracks originate from the same XY position - track lengths compatible with the 222Rn and 218Po a energies

10 14 tracks starting from the center
OTPC background measurement - 5 hours measurement - circles mark the beginning of the tracks Total of 260 tracks - most of them start from the walls 14 tracks starting from the center Y - position X - position

11 Tracks starting from the central region (16 x 16 x 15 cm3 gas volume ?)
Background activity estimate

12 Search for 220Rn - a - 216Po - a decay
- two triggers within 300 ms gate 2161 155 ms 216Po 9 cm 220Rn 5 ms

13 Range of a particles in Ar(50%) + He (50%) gas
1 atm 216Po 220Rn

14 Decays in the center (thoron gate)

15 Decays from the walls (thoron gate)

16 Time correlation between two a particles

17 Background thoron activity estimate

18 Super-Kamiokande radon detector
16x16 mm2 S = 2 (counts/day)/(1 mBq/m3) Background – 2.4 ± 1.3 counts/day Y. Takeuchi et al.. NIM A 421 (1999) 334

19 OTPC for radon detection
100 cm 50 cm 20 cm 15 cm 20 cm V = 6·10-3 m3 S = 6·10-3 m3 1 mBq/m3  24 h = 0.5 (counts/day) / (1 mBq/m3) V = 0.25 m3 S = 0.25 m3 1 mBq/m3  24 h = 21.6 (counts/day) / (1 mBq/m3) Background: 200 mBq/m3 radon 20 mBq/m3 thoron

20 220Rn decay products 220Rn 56 s 216Po 145 ms 212Po 300 ns 212Bi 61 m
212Pb 10.6 h 208Pb stable 212Bi 61 m 212Po 300 ns 208Tl 3 m 6.29 6.78 8.78 6.1

21 222Rn decay products 222Rn 3.8 d 218Po 3.1 m 214Po 164 ms 210Po 138 d
214Pb 27 m 210Pb 22.3 y 214Bi 20 m 214Po 164 ms 210Tl 1.3 m 5.49 7.69 5.45 6.00 206Pb stable 210Po 138 d 210Bi 5 d 206Tl 4.2 m 5.30 4.65

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