Argon scintillation light triplet component decay time in presence - - PowerPoint PPT Presentation

argon scintillation light triplet component decay time in
SMART_READER_LITE
LIVE PREVIEW

Argon scintillation light triplet component decay time in presence - - PowerPoint PPT Presentation

Argon scintillation light triplet component decay time in presence of contaminant(s) and the Air hypothesis Flavio Cavanna Dante Totani 1 Average waveform normalized from channel 270 Red= run 9004 Blue= run 8562 2 Single photon


slide-1
SLIDE 1

Argon scintillation light triplet component decay time in presence of contaminant(s) and the Air hypothesis

  • 1

Flavio Cavanna Dante Totani

slide-2
SLIDE 2

Red= run 9004 Blue= run 8562

Average waveform normalized from channel 270

2

slide-3
SLIDE 3

Max amplitude [ADU]

Single photon response:

The single photon response comes from calibrations runs. A pulsed LED lightened the PD modules giving a signal which is totally dependent from the MPPS response to the single photon (or more photons “contemporary”) Since after pulses and cross talks, a single photon detected can give more than one

  • avalanche. This means that a single

photon detected can populate the peaks beyond the first. Through the Poisson statistic we can get the average response to a single photon detected

λ = − ln ( N0 NTot)

3

slide-4
SLIDE 4

Single photon response normalized from channel 270

In these considerations we are assuming that the LED light pulse is a delta function.

4

slide-5
SLIDE 5

Comparing the Single photon response we can see how the scintillation light from ionizing events differs from the single photons response All the differences should be due to the LAr scintillation light structure in time

5

slide-6
SLIDE 6

The average waveforms are then deconvoluted for these single photon response and fitted with the function:

f(t) = A + B ⋅ exp(−t/τ)

Tick [1=6.67 ns] Run 8562 ch270

6

slide-7
SLIDE 7

7

Tick [1=6.67 ns] Run 9004 ch270

slide-8
SLIDE 8

Run 9004

<Tau> Arapuca1 : 765 ns <Tau> Arapuca2 : 762 ns

Run 8562

<Tau> Arapuca1 : 1263 ns <Tau> Arapuca2 : 1297 ns

An average of the values obtained for each Arapuca channel gives the following values

Arapuca 1 means Arapuca PD module in APA 3 (beam side) Arapuca 2 means Arapuca PD module in APA 6 (no-beam side)

8

slide-9
SLIDE 9

Run 9004

DAQch: 1 Tau t= 874.876 ns DAQch: 2 Tau t= 890.906 ns DAQch: 3 Tau t= 882.734 ns DAQch: 4 Tau t= 671.433 ns DAQch: 5 Tau t= 748.434 ns DAQch: 6 Tau t= 640.75 ns DAQch: 7 Tau t= 651.294 ns DAQch: 8 Tau t= 713.695 ns DAQch: 9 Tau t= 767.622 ns DAQch: 10 Tau t= 772.635 ns DAQch: 11 Tau t= 799.018 ns DAQch: 12 Tau t= 771.664 ns DAQch: 13 Tau t= 727.221 ns DAQch: 14 Tau t= 746.412 ns DAQch: 15 Tau t= 738.458 ns DAQch: 16 Tau t= 725.76 ns DAQch: 17 Tau t= 848.436 ns DAQch: 18 Tau t= 789.197 ns DAQch: 19 Tau t= 835.554 ns DAQch: 20 Tau t= 700.478 ns DAQch: 21 Tau t= 792.706 ns DAQch: 22 Tau t= 702.004 ns DAQch: 23 Tau t= 788.414 ns DAQch: 24 Tau t= 749.985 ns

<Tau> Arapuca1 : 765 ns <Tau> Arapuca2 : 762 ns

Run 8562

DAQch: 1 Tau t= 1281.68 ns DAQch: 2 Tau t= 1397.07 ns DAQch: 3 Tau t= 1309.93 ns DAQch: 4 Tau t= 1166.01 ns DAQch: 5 Tau t= 1149.52 ns DAQch: 6 Tau t= 1123.27 ns DAQch: 7 Tau t= 1165.98 ns DAQch: 8 Tau t= 1284.1 ns DAQch: 9 Tau t= 1346.99 ns DAQch: 10 Tau t= 1317.68 ns DAQch: 11 Tau t= 1298.19 ns DAQch: 12 Tau t= 1324.72 ns DAQch: 13 Tau t= 1238.85 ns DAQch: 14 Tau t= 1193.46 ns DAQch: 15 Tau t= 1285.95 ns DAQch: 16 Tau t= 1230.48 ns DAQch: 17 Tau t= 1363.56 ns DAQch: 18 Tau t= 1388.69 ns DAQch: 19 Tau t= 1419.86 ns DAQch: 20 Tau t= 1272.79 ns DAQch: 21 Tau t= 1315.56 ns DAQch: 22 Tau t= 1222.39 ns DAQch: 23 Tau t= 1302.91 ns DAQch: 24 Tau t= 1334.82 ns

<Tau> Arapuca1 : 1263 ns <Tau> Arapuca2 : 1297 ns

9

slide-10
SLIDE 10

10

The scintillation of liquid argon

2010 EPL 91 62002

  • T. Heindl, T. Dandl, M. Hofmann, R. Krucken, L. Oberauer, W. Potzel, J. Wieser, A. Ulrich

τT

0 = 1300 ± 60 ns

slide-11
SLIDE 11

11 Effects of Nitrogen contamination in liquid Argon

R Acciarri et al 2010 JINST 5 P06003

Oxygen contamination in liquid Argon

R Acciarri et al 2010 JINST 5 P05003

Light Quenching

slide-12
SLIDE 12

12

1 τT = 1 τT + kN2 fN2 [Air] + kO2 fO2 [Air]

𝝊0T

1.300 μs

kN2

0.11 ppm-1 μs-1

fN2

0.7809

kO2

0.54 ppm-1 μs-1

fN2

0.2095

1.300 0.10 1 10 100 Concentration(ppm) 0.10 0.50 1 tau_T (mus) 0.765 2.7

2.7 ppm (Air) = 0.56 ppm (O2) + 2.11 ppm (N2)

Light Quenching

slide-13
SLIDE 13

Light Absorption

R Acciarri et al 2010 JINST 5 P05003

ℓA = 1 kA [O2] = 52.5 cm

For tracks at the cathode (x=d=360 cm) the Transmittance is very low:

TA(x = d) = 0.1 %

slide-14
SLIDE 14

14

Backup slides

slide-15
SLIDE 15

15

slide-16
SLIDE 16

16

slide-17
SLIDE 17

17

slide-18
SLIDE 18

Run 8562 Run 9004