Performance of SiPM Ryuhei Nakamura (Kobe Univ.) GLC calorimeter group (KEK, Kobe, Konan, Niigata, Shinshu, Tsukuba) Contents ・ Introduction ・ Test results.

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Presentation transcript:

Performance of SiPM Ryuhei Nakamura (Kobe Univ.) GLC calorimeter group (KEK, Kobe, Konan, Niigata, Shinshu, Tsukuba) Contents ・ Introduction ・ Test results ・ Summary ・ To do

・ Particle Flow Algorithm  Fine segmentation  Large number of channels Introduction Particle  Direct attachment to Scinti. or WLS ・ Less expensive example is Scintillator (+WLS) & SiPM readout

SiPM (provided by JINR group) ・ Micro-APD cells operated in Geiger-mode ・ ~1000 pixels (~1mm × 1mm) ・ High Gain (~10 6 ) ・ Operational at low voltage (~65V) 8mm 2mm

Set up (for Gain mesurement) Fast Amp : ORTEC FTA820 (Gain 200) ADC : Phillips 7166 SiPM P.G.LED Bias G.G. FastAmp CAMAC ADC Thermostatic Chamber Gate width : 35nsec LED Pulse width : 10nsec height : 5.5V 50Ω 100kΩ 100 n F Bias 64.0V~67.5V SiPM Output Readout Circuit

Ped 1p.e. 2p.e. 3p.e. 4p.e. 2.00ns/div 100mV/div 1p.e. 2p.e. Ped Photon Counting at Room Temperature

Gain ・ Gain vs Bias voltage ( 6 SiPMs checked ) #Serial Number ① ――― ② ――― ③ ――― ④ ――― ⑤ ――― ⑥ ――― as  This #Serial ④ SiPM is used for the mesurement of Temp. dependence. (  Next page)

Temperature dependence ( for 1 SiPM ) 67.5V ――― 67.0V ――― 66.5V ――― 66.0V ――― 65.5V ――― 65.0V ――― 64.5V ――― 64.0V ――― 20 ℃ ――― 10 ℃ ――― 0 ℃ ――― ‐ 10 ℃ ――― ‐ 20 ℃ ―――

Thermal Noise ・ SiPM has a MHz order thermal noise. ---Some pixels discharge at random. -Set up 200ns/div 100mV/div SiPM Bias FastAmp Discriminater Scalar Thermostatic Chamber 1pixel

Thermal Noise vs Bias Voltage ( 6 SiPM checked )  This #Serial ④ SiPM is used for the measurement of Temp. dependence. (  Next page) (Same one was used in Gain vs Temp. mesurement) #Serial Number ① ――― ② ――― ③ ――― ④ ――― ⑤ ――― ⑥ ―――

Temperature dependence ( for 1 SiPM ) 67.5V ――― 67.0V ――― 66.5V ――― 66.0V ――― 65.5V ――― 65.0V ――― 64.5V ――― 64.0V ――― 24℃ ――― 10 ℃ ――― 0 ℃ ――― ‐ 10 ℃ ――― ‐ 20 ℃ ――― It was measured one day after (at room temperature)

Linearity ・ SiPM signal is saturated when two or more photons go into one pixel. SiPM P.G. LED Bias G.G. PMT CAMAC ADC GATE width : 100nsec LED Pulse width : 15nsec height : 4.0V to 8.0V WLS fiber N HIT = N pixels (1 - e - / Npixels )

Summary ・ We made a first measurements of Russian SiPMs (The result is very very preliminary) ・ Photo electron peak is observed ・ The gain of SiPM is ~10 6 ・ We measured -- Gain vs Bias V -- Gain vs Temp. -- Thermal Noise vs Bias V -- Thermal Noise vs Temp. -- Linearity ・・・ Saturation is observed

To do ・ Check reproducibility of the measurements ・ Check long term stability ・ Comparison with other photon sensors (MRS, AMPD, HPK’s…)