Transcript
Page 1: Absolute light output determination of crystal scintillators

Absolute light output determination of crystal scintillators

Presented by Min Jeong Kim

Page 2: Absolute light output determination of crystal scintillators

Contents

Large Area Avalanche Photodiode Experimental Setup

APD Optimization Test

CsI(Tl) and newly developed crystal test

Conclusion

Page 3: Absolute light output determination of crystal scintillators

Large Area Avalanche photodiode

<Windowless LAAPD>

Model 630-70-73-510

Diameter 16mm

window Windowless

Enhancement UV

Gain 130 at 2600 V

Dark current 110 nA

Capacitance 110 pF

The quantum efficiency close to the 80% in the visible and near infra-red. (PMT ~20%)

Gain of up to several hundred in the total collected charge is possible.

(Photodiode doesn’t have internal gain)

Page 4: Absolute light output determination of crystal scintillators

CsI(Tl) & Experimental setup

slightHygroscopicity

550Peak Emission (nm)

~1050Decay Time (ns)

4.53Density (g/cm3)

40000~60000Light output (Photons/MeV)

valueproperty

<Properties of CsI(Tl) made by Bicron>

PreAmp Amplifier FADC 25MHz

PC

HV

(1800V)

APDcrystal PreAmpPreAmp AmplifierAmplifierFADC

25MHzFADC

25MHz

PCPCHV

(1800V)

HV

(1800V)

APDcrystalAPDcrystal

Page 5: Absolute light output determination of crystal scintillators

APD optimization test

Energy resolution from different gain by changing high voltage.

The best resolution is obtained between 1780V and 1820V.

Page 6: Absolute light output determination of crystal scintillators

APD optimization test

Energy resolution from different shaping time.

The best resolution is obtained with 3~4μs shaping time.

Page 7: Absolute light output determination of crystal scintillators

Energy resolution of CsI(Tl)

Energy resolution (FWHM)

:4.7%

If we use PMT, energy resolution is about 7%

<HV:1800, gain:20 and shaping time:4us in amplifier>

662 keV

Page 8: Absolute light output determination of crystal scintillators

Calibration

EE

E

P

PY

ion

rayX

rayX

peakhe

1

The number of e-h pairs : 37,000 e-h/MeV The absolute light output : 52,000 ph/MeV

<HV:1800, gain:100 and shaping time:4us in amplifier>

EQR

YY

PTFE

heAPDph .

1,

Page 9: Absolute light output determination of crystal scintillators

CsI(Tl) from Yangyang

CsI(Tl)_1

CsI(Tl)_2

47,000 ph/MeV73,000 ph/MeV

Page 10: Absolute light output determination of crystal scintillators

SrCl2 crystal test

Energy resolution (FWHM) : 9.6% The number of e-h pair : 14,000 e-h/MeV The absolute light output : 20,000 ph/MeV

662 keV

Page 11: Absolute light output determination of crystal scintillators

Ba0.20Sr0.80Cl2 crystal test

Energy resolution (FWHM) : 5.4% The number of e-h pair : 16,500 e-h/MeV The absolute light output : 23,000 ph/MeV

662 keV

Page 12: Absolute light output determination of crystal scintillators

Conclusion

The best resolution of CsI(Tl) is obtained with 3~4 μs shaping time, and with 1800V high voltage of LAAPD.

We can measure the number of e-h pairs and the absolute light yield of scintillation crystals with LAAPD.

The number of e-h pair of CsI(Tl) is obtained to be about 37,000 e-h/MeV and the absolute light output is obtained to be about 52,000 ph/MeV for 662 keV 137Cs γ-ray source.

We estimate the relative light output of newly developed SrCl2 crystal to be about 40% of CsI(Tl) and Ba0.20Sr0.80Cl2 crystal to be about 45% of that.

We measured the absolute light yield of ZnSe(O), CeBr3 and other scintillation crystals.


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