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Previous product |
S13360-3050CS |
---|---|
1 Mcps |
0.5 Mcps |
Type no. |
Built-in MPPC |
Photosensitive area |
Pixel pitch |
Noise equivalent power |
High-band cutoff frequency |
Temperature control |
Supply voltage |
---|---|---|---|---|---|---|---|
C13365-1350SA |
S13360-1350CS |
□1.3 mm |
50 μm |
0.7 fW/Hz1/2 |
7 MHz |
Temperature compensation (non-cooled) |
±5 V |
C13365-3050SA |
S13360-3050CS |
□3.0 mm |
1.6 fW/Hz1/2 |
||||
C13366-1350GA |
TE-cooled type (MPPC for precision measurement) |
□1.3 mm |
50 μm |
0.15 fW/Hz1/2 |
7 MHz |
TE-cooled |
±5 V |
C13366-3050GA |
□3.0 mm |
0.3 fW/Hz1/2 |
Type no. |
Built-in MPPC |
Photosensitive area |
Pixel pitch |
Dark count |
Maximum count rate |
Temperature control |
Supply voltage |
---|---|---|---|---|---|---|---|
C13366-1350GD |
TE-cooled type (MPPC for precision measurement) |
□1.3 mm |
50 μm |
2.5 kcps |
10 Mcps |
TE-cooled |
±5 V |
C13366-3050GD |
□3.0 mm |
15 kcps |
Type no. |
Temperature control |
Supply voltage |
Features |
---|---|---|---|
C12332 |
Temperature compensation (non-cooled) |
±5 V |
· Evaluates any non-cooled MPPC (sold separately) |
Type no. |
Effective photosensitive area |
Pixel pitch |
Package |
---|---|---|---|
S13360-1325CS |
□1.3 mm |
25 μm |
Ceramic |
S13360-1350CS |
50 μm |
||
S13360-1325PE |
25 μm |
Surface mount type |
|
S13360-1350PE |
50 μm |
||
S13360-3025CS |
□3.0 mm |
25 μm |
Ceramic |
S13360-3050CS |
50 μm |
||
S13360-3025PE |
25 μm |
Surface mount type |
|
S13360-3050PE |
50 μm |
||
S13360-6025CS |
□6.0 mm |
25 μm |
Ceramic |
S13360-6050CS |
50 μm |
||
S13360-6025PE |
25 μm |
Surface mount type |
|
S13360-6050PE |
50 μm |
Measurable light level range
MPPC modules include two output types according to the incident light level (number of photons): analog output type and digital output type.
Selecting the digital output type or analog output type
The output type (digital or analog) should be selected according to the light level incident on the MPPC module. The following output waveforms (a) (b) and (c) show MPPC output waveforms measured at different incident light levels and observed on an oscilloscope. The incident light level was increased in the order of (a), (b), and (c), starting from (a) at very low light levels. The output signal of (a) consists of discrete pulses. In this state, selecting the digital output type allows measuring at a higher S/N, where the signals are binarized and the number of pulses is digitally counted. Since the digital output type can easily subtract the dark count from the signal, the detection limit is determined by dark count fluctuations.