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・Multi-Pixel Photon Counter (MPPC)

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Presentation on theme: "・Multi-Pixel Photon Counter (MPPC)"— Presentation transcript:

1 ・Multi-Pixel Photon Counter (MPPC)
Newly Developed Semiconductor Detectors ・Multi-Pixel Photon Counter (MPPC)    ・Fully-Depleted Back-illuminated CCD HAMAMATSU PHOTONICS K.K. Koei Yamamoto                        June 27th PD07 Kobe CONFIDENTIAL

2 ■ Multi Pixel Photon Counter(MPPC)
What’s MPPC? Solid state photon counter having Multi pixelated Geiger-mode APDs with self-quenching resistance The MPPC (Multi-Pixel Photon Counter) is developed by HAMAMATSU PHOTONICS K. K. and it is one of the products of Si-PM (Silicon Photo multiplier) family which was originally developed in Russia. HAMAMATSU MPPC is designed as a photon counting device based on structures of a Si APD which was adopted by CERN (CMS). HAMAMATSU named this product MPPC which is a trademark.

3 The candidates of name in SiPM faimily
  SiPM (Silicon Photo Multiplier)        SiPMT (Silicon Photo Multiplier Tube) MRS-APD (Metal Resistive Semiconductor APD) SPM (Silicon Photo Multiplier) MPGM APD (Multi Pixel Geiger-mode APD) AMPD (Avalanche Micro-pixel Photo Diode) SSPM (Solid State Photo Multiplier) GM-APD (Geiger Mode APD) SPAD (Singe Photon Avalanche Diode) MPPC : Multi Pixel Photon Counter

4 What is the structure of MPPC to improve the performances

5 Photo Absorption coefficient of Silicon

6

7 electron electron holes holes

8 CMS(CERN) APD

9 Hamamatsu Reverse Structure APD for CMS
E field strength P+ P N N- N+ Hamamatsu Reverse Structure APD for CMS ・ APD structure used in the electromagnetic Calorimeter of CMS. ・ The p/n junction is formed in an epitaxial layer with 50μm thickness. ・ Bias 350 to 400V to get gain 50

10 Back illumination type
p--epi p++-subst. N/P-Reach through p+ n n--epi n++-subst. n+ p p- p+ P/N-Reach through N/P-Reach through Back illumination type p+ p--epi n++-subst. HPK Reverse structure

11 What are the characteristics of MPPC
1600 pixel

12 ■ Pixel number and application
PET HEP calorimeter Fluorescence meas. Neutrino detection 25um pitch 1600pixel 50um pitch 400pixel 100um pitch 100pixel Dynamic range wide               narrow The linearity is up to about 60% of the total pixels toward incident photons ; plural photons may enter one pixel beyond it Geo. efficiency low(10~40%)   high(~90%)

13 ■ Specification of 1mm□, MPPC
1600 400 100

14 ■ Bias vs. Gain S10362-11-025U/C S10362-11-050U/C, -100U/C
50μm 400pixels 25μm 1600pixels 100μm 100pixels S U/C S U/C, -100U/C

15 ■ Bias vs. Dark count S10362-11-025U/C S10362-11-050U/C, -100U/C
25μm 1600pixels 50μm 400pixels 100μm 100pixels S U/C S U/C, -100U/C

16 Photon Detection Efficiency (PDE)
100μm Pixel (100 pixel type) 50μm Pixel (400 pixel type) 25μm Pixel (1600 pixel type) ※including the cross-talk and after pulse

17 ■ Output signal of MPPC Photon counting by pulse height (liner Amp.)
Photon counting by output charge (charge Amp.)

18 Energy Resolution MPPC: 50mm pitch, 3mm square LSO: 3mm x 3mm x 20mm
13%

19 Gain uniformity (400 pixel, 100 samples)

20 PDE uniformity (400 pixel, 100samples)

21 1600 pixel Microscopic view
S U ( )

22 Laser Scan in One Pixel Pin-point scan :YAG laser (l = 532 nm) with spot size ~ 1 mm. Variation of photon sensitivity and gain in one pixel are evaluated. Observed variation is 2 ~ 5 % in a sensitive area for the 100 / 400 / 1600 pixel MPPCs. 1600 pixel Sensitivity 1600 pixel Gain Variation ~ 3 % Gain (x 105) y-point (1mm pitch) Sensitivity (arbitrary) y-point (2mm pitch) One pixel x-point (1mm pitch) x-point (2mm pitch)

23 Time resolution at center in different pixel
MPPC: MPPC:1mm2 50μm pitch

24 Time resolution in one pixel
MPPC:1mm2 50μm pitch

25 Package Developments

26 Plastic PKG(1mm□ × 1ch.) 4.2 3.2 1.3

27 SMD PKG(1mm□ × 1ch.) 1.0 2.4 1.9 [mm]

28 SMD PKG(3mm□ × 1ch.) 1.0 4.4 3.9 [mm]

29 CERAMIC PKG(3mm□ × 1ch.) 2.0 7.2 5.9

30 CERAMIC PKG(3mm□ × 4ch.) 8.1 2.0 8.95

31 ■ MPPC’s future plan ・Increase reproducibility and uniformity ・ Large sensitive area , Array and Matrix ・Enhance PDE ・Suppress after pulse and cross talk ・Quenching resistance optimization ・Package development (small, cheap, rugged) ・Custom design ( pitch, package, array)

32 Al optical separation and Trench etching

33 MPPC Module Features -Employs a Geiger-mode multi-pixel APD(MPPC)
-Integrates a signal readout circuit ideal for MPPC -Built-in high-voltage circuit and temperature-compensated circuit -Three types of output: analog, comparator, pulse calculation value -USB interface for easy handling: driven by USB bus power -Compact and light weight

34 MPPC Module block diagram
Power ( Use USB bus power ) Output-3 ( pulse calculation value) BUS line Output-1 ( analog out ) Output-2 ( comparator out )

35 Characteristics(analog output)
PC USB Measurement C U C U

36 Characteristics(temperature stability of Gain)

37 Fully-depleted thick back-illuminated CCD

38 Subaru Telescope 山頂観測所 山麓オフィス

39 Target Collaboration with National Astronomical Observatory of Japan for a next generation instrument for Subaru Telescope:a very wide-field CCD camera which named Hyper Suprime Camera(HSC). The CCD format: 4 side buttable, 2k×4k 15um square pixels with 4 low noise output amplifiers. QE Require 400nm 60% 700nm 85% 1000nm 60% 900nm 95% 10e- rms at 1MHz -

40 UV-NIR, X-ray Absorption Efficiency
Absorption Length [mm] 1000 UV-IR Light X-ray 100 10 1 0.1 0.01 Wavelength [nm] Energy [keV]

41 CCD fabrication Technology
Standard front processing through about 10 masking steps 6inch process line Conventional CCD fabrication technology except N-type high-resistivity silicon 3 layer polysilicon After front process, wafers are sent out for backgrinding and backpolishing The wafer are thinned 600um to um. Active accumulation and deposition of antireflection coating Front metallization process Dicing and Assembly

42 CCD Structure and Format

43 Specification and evaluation results
CCD Structure FFT or FT Pixel size 15um square Number of active pixels 2048(H)x4096(V) or 2048(V) Vertical clock phase 3phases Horizontal clock phase 2phases or 4phases Output One stage MOSFET SF 4ch Package Aluminum Nitride CTE > Full well capacity >150ke- Dark <5e-/pixel/hour CCE 5uV/e- Readout noise <5e- at 130kHz Quantum efficiency 40% at 400nm 90% at 650nm 40% at 1000nm

44 2k4k BICCD assembly technology
The 2k x 4k pixels 4 side buttable CCD The size is 31.54mm x mm 66Pins On-PKG Pre-Amplifier , Thermistor

45 4 side buttabletechnology(3x3 chips)

46 Good surface flatness

47 Improvement of cosmetics & dark image
1st trial Small format CCD 24umx512x512 300e-/pixel/s at -20oC Prototype Small format CCD 24umx51512 300e-/pixel/s at -20oC Large format CCD 15umx2kx4k 2-4e-/pixel/hour at -100oC

48 Quantum efficiency at -100oC

49 Evaluation results   ・Good Charge Transfer efficiency  >   ・Large full-well capacity >150Ke   ・High charge conversion efficiency 5uV/e   ・Low dark <5e/pixel/hour at -100℃   ・Low noise <5e at 130kHz readout,-100℃   ・High near-infrared QE  40% at 1000nm     ・Good surface flatness um Due to the new process factory of Hamamatsu, the CCD has the good cosmetics. These results are promising for HSC which requires more than 100 CCDs.

50 10 Billion Pixels CCD Camera
800mm  Hyper Suprime Camera Suprime-Camera

51 Hyper Suprime Camera / Subaru NAOJ
Courtesy to NAOJ

52


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