absolute light output determination of crystal scintillators

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Absolute light output determinati on of crystal scintillators Presented by Min Jeong Kim

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Absolute light output determination of crystal scintillators. Presented by Min Jeong Kim. Contents. Large Area Avalanche Photodiode Experimental Setup APD Optimization Test CsI(Tl) and newly developed crystal test Conclusion. Large Area Avalanche photodiode. - PowerPoint PPT Presentation

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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.