HAMAMATSU P9217-02

INFRARED DETECTOR
PbS photoconductive detector
P9217 series
Room-temperature detectors capable of detecting up to 2.9 µm
P9217 is a PbS photoconductive detector with greatly improved stability and resistance to high temperatures as compared with conventional types.
Features
Applications
l High reliability: high temperature resistant
l Radiation thermometers
l Flame monitors
l Water content analyzers
l Food ingredient analysis
l Spectrophotometers
Accessories (Optional)
l Preamplifier for PbS/PbSe photoconductive detector
C3757-02
■ Specification/Absolute maximum ratings
Type No.
P9217
P9217-02
P9217-03
P9217-04
Di m e nsional
O utline/
Package
Wi nd o w
m aterial * 1
➀/K
➀/K
➀/K
➁/K
TO-5
TO-8
Absolute maximum ratings
Cooling
Non-cooled
Active
area
(mm)
1×5
2×2
3×3
4×5
Supply voltage
Operating
temperature
Topr
Storage
temperature
Tstg
(V)
(°C)
(°C)
100
-30 to +65
-55 to +65
■ Electrical and optical characteristics (Typ. unless otherwise noted)
Type No.
Peak
Photo sensitivity *2
Cut-off
sensitivity
S
wavelength
wavelength
λ=λp
λc
Vs=15 V
λp
Min.
Typ.
(µm)
(µm)
(V/W)
(V/W)
D∗
(500, 600, 1)
D∗
(λp, 600, 1)
Min.
Typ.
(cm·Hz1/2/W) (cm·Hz1/2/W) (cm·Hz1/2/W)
P9217
4 × 104
1 × 105
P9217-02
5 × 104
5 × 108
1 × 109
1 × 1011
2.2
2.9
P9217-03
2 × 104
5 × 104
P9217-04
1 × 104
3 × 104
2 × 108
5 × 108
5 × 1010
*1: Window material K: Borosilicate glass
*2: Chopping frequency: 600 Hz, load resistance: nearly equal to detector element dark resistance.
Rise time
tr
0 to 63 %
Max.
(µs)
200
Dark
resistance
Rd
(MΩ)
0.05 to 1
0.25 to 2.5
0.2 to 2.0
1
P9217 series
PbS photoconductive detector
■ Spectral response
■ S/N vs. supply voltage
(Typ. T=25 ˚C)
100
(Typ. Ta=25 ˚C)
800
8
7
SIGNAL
80
60
40
6
5
400
4
NOISE
2
LIGHT SOURCE: BLACK BODY 500 K
INCIDENT ENERGY: 4.8 µW/cm2
1
CHOPPING FREQUENCY: 600 Hz
FREQUENCY BANDWIDTH: 60 Hz
0
20
40
50
60
30
200
20
0
1
2
3
4
0
5
10
0
3
NOISE (µV)
SIGNAL (µV)
RELATIVE VALUE (%)
600
WAVELENGTH (µm)
SUPPLY VOLTAGE (V)
KIRDB0301EA
KIRDB0046EA
If voltage of higher than 60 V is applied,
the noise increases exponentially, degrading the S/N. The device should be
operated at 60 V or less.
■ Photo sensitivity temperature characteristic
■ S/N vs. chopping frequency
(Typ. Ta=25 ˚C)
10
S
1
1
LIGHT SOURCE: BLACK BODY 500 K
INCIDENT ENERGY: 4.8 µW/cm2
CHOPPING FREQUENCY: 600 Hz
SUPPLY VOLTAGE: 15 V
N
0.1 1
10
102
(Typ.)
10
RELATIVE SENSITIVITY (%)
RELATIVE S/N
LIGHT SOURCE: BLACK BODY 500 K
INCIDENT ENERGY: 4.8 µW/cm2
SUPPLY VOLTAGE: 15 V
tr: 200 µs
S/N
0.1
-10
103
0
10
20
30
40
50
60
70
ELEMENT TEMPERATURE (˚C)
CHOPPING FREQUENCY (Hz)
KIRDB0047EC
KIRDB0302EB
Cooling the device enhances its sensitivity, but the sensitivity also depends
on the load resistance in the circuit.
Increasing the chopping frequency reduces the 1/f noise and results in an S/N
improvement. The S/N can also be improved by narrowing the noise bandwidth
using a lock-in amplifier.
■ Dark resistance, rise time temperature characteristics
■ Photo sensitivity linearity
(Typ.)
10
RISE TIME
101
RELATIVE OUTPUT
RELATIVE VALUE (%)
(Typ. Ta=25 ˚C, FULLY ILLUMINATED)
102
1 DARK
RESISTANCE
100
10-1
10-2
DEPENDENT ON NEP
0.1
-10
0
10
20
30
40
50
60
70
ELEMENT TEMPERATURE (˚C)
10-3 -9
10
10-8
10-7
10-6
10-5
10-4
INCIDENT ENERGY (W/cm2)
KIRDB0303EB
KIRDB0050EA
By making the incident light spot smaller
than the active area, the upper limit of
the linearity becomes lower.
2
PbS photoconductive detector
P9217 series
■ Dimensional outline (unit: mm)
➁ P9217-04
9.1 ± 0.3
13.9 ± 0.2
8.1 ± 0.1
WINDOW
5.9 ± 0.1
12.35 ± 0.1
CASE
4.9 ± 0.2
4.3 ± 0.2
0.45
LEAD
7.5 ± 0.2
2.3 ± 0.2
0.5 MAX.
0.45
LEAD
PHOTOSENSITIVE
SURFACE
18 MIN.
0.7 ± 0.1
2.3 ± 0.2
0.4 MAX.
PHOTOSENSITIVE
SURFACE
WINDOW
10.5 ± 0.1
15 ± 1
➀ P9217/-02/-03
1 MAX.
5.1 ± 0.2
1.5 MAX.
CASE
45˚
8
0.
±
0.
8
±
0.
1
1
0.
KIRDA0166EB
KIRDA0181EA
Information furnished by HAMAMATSU is believed to be reliable. However, no responsibility is assumed for possible inaccuracies or omissions.
Specifications are subject to change without notice. No patent rights are granted to any of the circuits described herein. ©2007 Hamamatsu Photonics K.K.
HAMAMATSU PHOTONICS K.K., Solid State Division
1126-1 Ichino-cho, Higashi-ku, Hamamatsu City, 435-8558 Japan, Telephone: (81) 53-434-3311, Fax: (81) 53-434-5184, www.hamamatsu.com
U.S.A.: Hamamatsu Corporation: 360 Foothill Road, P.O.Box 6910, Bridgewater, N.J. 08807-0910, U.S.A., Telephone: (1) 908-231-0960, Fax: (1) 908-231-1218
Germany: Hamamatsu Photonics Deutschland GmbH: Arzbergerstr. 10, D-82211 Herrsching am Ammersee, Germany, Telephone: (49) 08152-3750, Fax: (49) 08152-2658
France: Hamamatsu Photonics France S.A.R.L.: 19, Rue du Saule Trapu, Parc du Moulin de Massy, 91882 Massy Cedex, France, Telephone: 33-(1) 69 53 71 00, Fax: 33-(1) 69 53 71 10
United Kingdom: Hamamatsu Photonics UK Limited: 2 Howard Court, 10 Tewin Road, Welwyn Garden City, Hertfordshire AL7 1BW, United Kingdom, Telephone: (44) 1707-294888, Fax: (44) 1707-325777
North Europe: Hamamatsu Photonics Norden AB: Smidesvägen 12, SE-171 41 Solna, Sweden, Telephone: (46) 8-509-031-00, Fax: (46) 8-509-031-01
Italy: Hamamatsu Photonics Italia S.R.L.: Strada della Moia, 1/E, 20020 Arese, (Milano), Italy, Telephone: (39) 02-935-81-733, Fax: (39) 02-935-81-741
Cat. No. KIRD1065E03
Mar. 2007 DN