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MPPC Radiation Hardness (gamma-ray & neutron)

MPPC Radiation Hardness (gamma-ray & neutron). Satoru Uozumi , Kobe University for Toshinori Ikuno, Hideki Yamazaki, and all the ScECAL group. Knowing radiation resistivity is important to estimate the life time of the calorimeter under the environment at the ILC.

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MPPC Radiation Hardness (gamma-ray & neutron)

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  1. MPPC Radiation Hardness(gamma-ray & neutron) Satoru Uozumi, Kobe University for Toshinori Ikuno, Hideki Yamazaki,and all the ScECAL group Knowing radiation resistivity is important to estimate the life time of the calorimeter under the environment at the ILC. In last year we have some chances to have radiation test with gamma-ray and neutrons.

  2. Multi Pixel Photon Counter (MPPC) ~ 1 mm photon A pixelated photon detector manufactured by Hamamatsu Photonics • MPPC consists of 2D array of Geiger-mode APD pixels. • Each pixel can count a photon at same time. • MPPC outputs signal from all pixels as a summation. • (Properties) • High Gain (>105) • Good Photon Detection • Efficiency (~15% with 1600 pixel) • Compact (package size ~ a few mm) • Low Cost • Insensitive to magnetic field • Dark count exists • (because of thermal electrons) • Secondary photons from avalanche • make crosstalk. • Input vs output is non-linear 2

  3. Gamma-ray Radiation 60Co Source MPPC 60 cm Radiation source ~15TBq 60Co Source Dose amount 10 Gy/h for 3 hours →30 Gy 10 Gy/h for 6 hours 　→60 Gy 10 Gy/h for 12 hours →120 Gy Prospective damage Charge accumulation on the oxidized layer. Radiated MPPC Sample Type : ILC-11-0125M 　 Size : 1mm×1mm 1600 pixel (25μmpitch) (Gy=100 rad=J/kg) Oxidized layer Al Quenching resister p+ p- n++ 3

  4. Gain measurement d PED 1 p.e. 2 p.e. An example of ADC distribution PED 1 p.e. 2 p.e. p.e. : photo-electron S: ADC resolution Q: charges gained by geiger-mode e: elementary charge Vbias: Bias Voltage C: pixel capacitance V0: Breakdown Voltage(Threshold of geiger-mode) 4

  5. Gamma-ray(Gain) before after radiated　before　after 30 Gy ● ● 60 Gy ■■ 120 Gy ▲ ▲ before after ● 30 Gyradiated ● 60 Gy radiated ● 120 Gy radiated There seem no significant changes on the gain by gamma-ray radiation. 5

  6. Gamma-ray(current : during radiation) ● 30 Gy radiated sample ●60 Gy radiated sample ●120 Gy radiated sample Ammeter Over-range 3 hrs radiation 6 hrs radiation 12 hours radiation The current was measured by an ammeter. The current has increased drastically. (about 90 Gy) 6

  7. Gamma-ray(leakage current : afterradiation) ●120 Gy radiated sample The leakage current has decreased by time. Start operating bias 　　　　　before　after 30 Gy ● ● 60 Gy ■■ 120 Gy ▲ ▲ (at 40hour) 120 Gy radiated sample 1 p.e. height The leakage current have increased by gamma-ray radiation. 7

  8. Gamma-ray(Noiserate / Crosstalk Probability) 1 MHz (goal of ScECAL) The noiserate have increased by gamma-ray radiation. For almost all points, there seem no significant changes on the crosstalk probability by radiation. radiated　before　after 30 Gy ● ● 60 Gy ■■ 8

  9. Gamma-ray(Hot spot pictures) We took infrared pictures to see the hot spots. (Hot spot : The spot which always let out noise.) 30 Gy radiated 60 Gy radiated 120 Gy radiated 120 Gy radiated (zoomed) There seem hot spots have increased by gamma-ray radiation, The black squares are the sensitive areas. The white lines are the oxidized layer with bias lines. The hot spots only appeared on the oxidized layer. 9

  10. Gamma-ray(Response Curve) ● not radiated ● 30 Gyradiated ● 60 Gy radiated ● 120 Gy radiated The response curves have not changed by gamma-ray radiation. 10

  11. Neutron Radiation Flux 3.1×108 neutron/cm2 3.1×109 neutron/cm2 3.1×1010 neutron/cm2 3.1×1011 neutron/cm2 Prospective damage Increasing lattice defect in silicon bulk Radiated MPPC Sample Type : S10362-11-025MK Size : 1mm×1mm 1600 pixel (25μmpitch) Radiation test location The reactor YAYOI (Fast neutron source reactor of the University of Tokyo) 11

  12. Neutron(Gain) before after radiated　before　after 108 /cm2● ● 109 /cm2■■ 1010 /cm2▲ ▲ before after ● 108 /cm2 radiated ● 109 /cm2 radiated ● 1010 /cm2 radiated There seem no significant changes on the gain by neutron radiation. 12

  13. Neutron(Leakage Current) radiated　before　after 108/cm2● ● 109 /cm2■■ 1010 /cm2▲ ▲ 1011 /cm2▼▼ The leakage current have increased by neutron radiation. 13

  14. Neutron(Noise Rate / Crosstalk Probability) The noiserate have increased by neutron radiation. There seem no significant changes on the crosstalk probability by radiation. 1MHz (goal of ScECAL) radiated　before　after 108/cm2● ● 109 /cm2■■ 14

  15. Neutron(Hot spot pictures) 108 /cm2 radiated 109 /cm2 radiated 1010 /cm2 radiated 1011 /cm2 radiated 1011 /cm2 radiated (zoomed) There seem hot spots have increased by neutron radiation. The hot spots only appeared on the sensitive area. 15

  16. Neutron(Response Curve) ● not radiated ● 108 /cm2 radiated ● 109 /cm2 radiated ● 1010 /cm2 radiated ● 1011 /cm2 radiated Theresponse curves have not changed by neutron radiation. 16

  17. Summary MPPC Radiation Resistivity Study (Gamma-ray & Neutron radiation) ・The leakage current and the noise rate are significantly increased. ・There seem no significant changes on the gain and the crosstalk probability. ・The response curves have not changed by radiation. Even though the dark noise increased by radiation, the MPPC still working as photon-counting device. Plan ・The estimation of dose at ScECAL (Need simulation tools!). ・More radiation tests with estimateddose. 17

  18. Back Up

  19. ADC distribution Some ADC distributions of radiated samples are too noisy to evaluate the gain. Ex.) The ADC distributions of gamma-ray 120 Gy radiated sample ΔV = 2.8V ΔV= 1.9V O.K. N.G.

  20. Response Curve measurement Ped Timing Sig Timing 20

  21. NoiseRate measurement(Crosstalk Probability measurement) 1 photo-electron 2 photo-electron An example of Threshold curve Scaler count 0.5 p.e. 1.5 p.e. 21

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