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SiPM Workshop EU-FP7(HP3), Vienna, 16 Feb. 2013 F.G. H.O. Study of scintillator detectors time resolution with different SiPM readout on T10 test beam.

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Presentation on theme: "SiPM Workshop EU-FP7(HP3), Vienna, 16 Feb. 2013 F.G. H.O. Study of scintillator detectors time resolution with different SiPM readout on T10 test beam."— Presentation transcript:

1 SiPM Workshop EU-FP7(HP3), Vienna, 16 Feb. 2013 F.G. H.O. Study of scintillator detectors time resolution with different SiPM readout on T10 test beam at June 2012 - The goal of measurements. - Scintillator detectors with different SiPMs readout. - T10 test beam facility. - Results of measured time resolution for different SiPMs readout. - Conclusion F.Guber, A.Ivashkin,V.Marin, INR,Moscow H.Orth, GSI, Darmstadt

2 SiPM Workshop EU-FP7(HP3), Vienna, 16 Feb. 2013 F.G. H.O. Goal of the test To measure time resolution and amplitude spectra of scintillator detectors with SiPMs produced by HAMAMATSU, KETEK and ZECOTEK. Dimensions of scintillators are optimized for TOF systems of PANDA experiment at FAIR. Additional test have been done for scintillators optimized for central part of forward CBM TOF, HADES FW….

3 SiPM Workshop EU-FP7(HP3), Vienna, 16 Feb. 2013 F.G. H.O. Scintilators – BC-408 Two sample: -28 x 28 x 5 mm -30 x 30 x 10 mm Scintillators have been overlapped by TYVEK Used SiPMs – sensitive area 3 x 3 mm: - PM3350 (KETEK) - MPPC S10362-33-100C (HAMAMATSU) - MAPD-3N (Zecotek) Method of light readout: Scintillator 28 x 28 x 5 mm by two SiPMs from one surface. Scintillator 30 x 30 x 10 mm by two SiPMs from opposite rear surfaces. Scintillator detectors with different SiPMs readout

4 SiPM Workshop EU-FP7(HP3), Vienna, 16 Feb. 2013 F.G. H.O. Properties of used SiPMs Active Area 3 x 3 mm 2 Pixel Size 100 x 100 um Number of Pixels 3600 Peak Wavelength 440 nm Operating Voltage 70±10 V Gain 750 000 MPPC S10362-33-100C (HAMAMATSU) PM3350 (KETEK) Active Area 3 x 3 mm 2 Pixel Size 100 x 100 um Number of Pixels 3600 Peak Wavelength 420 nm Operating Voltage 28 - 41 V Gain ~2 000 000 Active Area 3 x 3 mm 2 Number of Pixels 135 000 Peak Wavelength 450 -500nm Operating Voltage ~90 V Gain 50 000 MAPD-3N (Zecotek)

5 SiPM Workshop EU-FP7(HP3), Vienna, 16 Feb. 2013 F.G. H.O. Amp PMT quartz beam Amp SiPM TDC Start Stop1 Stop2 LeCroy 2228A ADC LeCroy 2249A Hamamatsu R7525  t =60ps D DD Leading Edge DiscrimonatorC AEN Mod.84 Thresh=50 mV Experimental Setup

6 SiPM Workshop EU-FP7(HP3), Vienna, 16 Feb. 2013 F.G. H.O. Two different amplifiers were used Differential amplifier provided by H.Orth (positive overshoot is visible) Amplifier with Pole Zero Compensation The time and amplitude resolutions for PZC amplifier are slightly better and the measurements were done for second type.

7 SiPM Workshop EU-FP7(HP3), Vienna, 16 Feb. 2013 F.G. H.O. Test results for scintillators with HAMAMATSU MPPC S10362-33-100C

8 SiPM Workshop EU-FP7(HP3), Vienna, 16 Feb. 2013 F.G. H.O. Amplitude spectra for one of MPPC at large side MPPC1 MPPC2 28 mm Time-amplitude walk At present analysis the time resolution was determined for narrow ADC bin to avoid T-A walk t= 5mm

9 SiPM Workshop EU-FP7(HP3), Vienna, 16 Feb. 2013 F.G. H.O. Time spectra for MPPCs from large side MPPC1 MPPC2 28 mm  t =173 ps for both MPPC  t =231 ps for single MPPC (T1+T2)/2 Time resolutions were calculated for narrow ADC bin= 40 ch Time resolution of start quartz detector (σ t =60ps) Is taken into account t= 5mm

10 SiPM Workshop EU-FP7(HP3), Vienna, 16 Feb. 2013 F.G. H.O. Amplitude spectrum for MPPC at small side Time resolution were calculated for narrow ADC bin ~ 40 ch to avoid T-A walk MPPC1 MPPC2 28 mm Amplitude at small side is ~1.5 times larger comparing to large side t= 5mm

11 SiPM Workshop EU-FP7(HP3), Vienna, 16 Feb. 2013 F.G. H.O. Time spectra for MPPCs at small opposite sides MPPC1 MPPC2 28 mm Calculation were done for narrow ADC bin= 40 ch (T1+T2)/2  t =148 ps for single MPPC  t =126 ps for both MPPC t= 5mm

12 SiPM Workshop EU-FP7(HP3), Vienna, 16 Feb. 2013 F.G. H.O. Spectra for MPPCs from scintillator 30 x 30 x10 mm t = 10 mm  t =170 ps for single MPPC  t =115 ps for both MPPC (T1+T2)/2 MPPC1 MPPC2 30 mm Calculation were done for narrow ADC bin= 40 ch

13 SiPM Workshop EU-FP7(HP3), Vienna, 16 Feb. 2013 F.G. H.O. Test results for scintillators with PM3350 (KETEK)

14 SiPM Workshop EU-FP7(HP3), Vienna, 16 Feb. 2013 F.G. H.O. Amplitude spectra for KETEK SiPMs at small side Time-amplitude walk Time resolution was calculated for narrow ADC bin to avoid T-A walk SiPM1 SiPM2 28 mm t= 5mm

15 SiPM Workshop EU-FP7(HP3), Vienna, 16 Feb. 2013 F.G. H.O. Time spectra for KETEK SiPMs at small sides Calculations were done for narrow ADC bin= 50 ch SiPM1 SiPM2 28 mm  t =120 ps for both SiPMs (T1+T2)/2  t =168 ps for single SiPM t= 5mm

16 SiPM Workshop EU-FP7(HP3), Vienna, 16 Feb. 2013 F.G. H.O. Time spectra for KETEK SiPMs at small sides for very narrow ADC bin=20 ch Measurement were done for very narrow ADC bin= 20 ch SiPM1 SiPM2 28 mm  t =96 ps for both SiPMs (T1+T2)/2  t =163 ps for single SiPM t= 5mm

17 SiPM Workshop EU-FP7(HP3), Vienna, 16 Feb. 2013 F.G. H.O. Test results for scintillators with MAPD-3N

18 SiPM Workshop EU-FP7(HP3), Vienna, 16 Feb. 2013 F.G. H.O. Spectra for Zecotek MAPD-3N (T1+T2)/2  t =240 ps for both MAPDs  t =360 ps for single MAPD SiPM1 SiPM2 28 mm t= 5mm

19 SiPM Workshop EU-FP7(HP3), Vienna, 16 Feb. 2013 F.G. H.O. Summary A measurements of 28x28x5 mm 3, 28x28x10 mm 3 and 30 x 30 x 10 mm 3 scintillator tiles were performed for a few types of SiPMs. The best time resolution is obtained in case of SiPM position at opposite small sides of the tile. Time resolutions for single Hamamatsu MPPC and KETEK SiPM are very similar and about 150-160 ps. Averaged time resolution with two SiPM readout is about 120 ps. For very narrow ADC bin widths the time resolution could achieve 100 ps. But it is worser probably for wide ADC range. The effect of time-amplitude walk should be account properly. Further optimization of the measurements is required. Namely, the discriminator threshold, signal amplification, SiPM voltage and noise affect the time resolution.


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