Radiant at 400nm .....................................
Low Drift and Hysteresis
The R928 and R955 feature extremely high quantum efficiency,
high current amplification, good S/N ratio and wide spectral response from UV to near infrared. The R928 employs a UV glass
envelope and the R955 has a fused silica envelope for UV sensitivity extension.
The R928 and R955 are well suited for use in broad-band spectrophotometers, atomic absorption spectrophotometers, emission spectrophotometers and other precision photometric instruments.
185 to 900 nm
160 to 900 nm
250 A/lm
74mA/W
2500A/lm
7.4 10
5
A/W
PHOTOMULTlPLlER TUBES
R928, R955
GENERAL
ParameterDescription/Value Unit
Spectral Response
R928
R955
Wavelength of Maximum Response
Photocathode
MateriaI
Minimum Effective Area
Window Material
R928
R955
Dynode
Secondary Emitting Surface
Structure
Number of Stages
Direct Interelectrode Capacitances
Anode to Last Dynode
Anode to All Other Electrodes
Base
Weight
SuitabIe Socket
SuitabIe Socket Assembly
185 to 900nm
160 to 900nm
400
Multialkali
8 24
UV glass
Fused silica
Multialkali
Circular-cage
9
Approx. 4pF
Approx. 6pF
11-pin base
JEDEC No. B11-88
Approx. 45
E678–11A (option)
E717–21 (option)
nm
mm
g
Figure 1: Typical Spectral Response
TPMSB0001EB
100
R955
10
1
QUANTUM EFFICIENCY (%)
0.1
CATHODE RADIANT SENSITIVITY (mA/W)
0.01
100 200 300
R928
QUANTUM EFFICIENCY
400 500 600 700
WAVELENGTH (nm)
CATHODE
RADIANT
SENSITIVITY
900
800
1000
Subject to local technical requirements and regulat ions, availability of products included in this promotional material may va r y. Please consult with our sales office.
lnformation furnished by HAMA M ATSU is believed to be reliabIe. However, no respon sibility is assumed for possibIe inaccuracies or ommissions. Specifications are
subject to change without notice. No patent right are granted to any of the circuits described herein.
Between Anode and Last Dynode
Average Anode Current
Ambient Temperature
–80 to +50
CHARACTERISTlCS (at 25 )
Parameter
Cathode Sensitivity
Quantum Efficiency at Peak Wavelength
Luminous
Radiant at 194nm18
Red/White Ratio
Blue
Anode Sensitivity
Luminous
Radiant at 194nm1.8 10
Gain
Anode Dark Current
After 30 minute Storage in the darkness350
B
254nm52
400nm74
633nm41
852nm3.5
C
D
E
254nm
400nm
633nm
852nm
E
F
1250
250
0.1
Min.Max.
Unit
Vdc
Vdc
mA
R928
Typ.
25.4
(at 260nm)
140250
0.2
0.3
8
2500400
5.2 10
7.4 10
4.1 10
3.5 10
1.0 10
5
5
5
5
4
7
R955
Min.Max.
Typ.
29.0
Unit
%
(at 220nm)
140250 A/lm
43mA/W
56mA/W
74mA/W
41mA/W
3.5mA/W
0.2
0.3
8 A/lm-b
2500A/lm400
4.3 10
5.6 10
7.4 10
4.1 10
3.5 10
1.0 10
5
5
5
5
4
7
A/W
A/W
A/W
A/W
A/W
350nA
ENI(Equivalent Noise Input)
Time Response
E
Anode Pulse Rise Time
Electron Transit Time
Transit Time Spread (TTS)
Anode Current Stability
H
I
J
K
L
Current Hysteresis
Voltage Hysteresis
NOTES
Averaged over any interval of 30 seconds maximum.
A:
The light source is a tungsten filament lamp operated at a distribution tem-
B:
perature of 2856K. Supply voltage is 100 volts between the cathode and
all other electrodes connected together as anode.
Red/White ratio is the quotient of the cathode current measured using a
C:
red filter(Toshiba R-68) interposed between the light source and the tube
by the cathode current measured with the filter removed under the same
conditions as Note B.
The value is cathode output current when a blue filter(Corning CS-5-58
D:
polished to 1/2 stock thickness) is interposed between the light source and
the tube under the same condition as Note B.
Measured with the same light source as Note B and with the voltage distri-
SuppIy Voltage : 1000Vdc
K : Cathode, Dy : Dynode, P : Anode
1111111111
1.3 10
2.2
22
1.2
0.1
1.0
-16
F:
Measured with the same supply voltage and voltage distribution ratio as
Note E after removal of light.
G:
Measured at a supply voltage adjusted to provide an anode sensitivity of
100 A/lm.
ENI is an indication of the photon-limited signal-to-noise ratio. It refers to
H:
the amount of light in watts to produce a signal-to-noise ratio of unity in the
output of a photomultiplier tube.
ENI =
where q = Electronic charge (1.60 10
ldb = Anode dark current(after 30 minute storage) in amperes.
G = Gain.
f = Bandwidth of the system in hertz. 1 hertz is used.
S = Anode radiant sensitivity in amperes per watt at the wave length of peak response.
I:
The rise time is the time for the output pulse to rise from 10% to 90% of the
peak amplitude when the entire photocathode is illuminated by a delta
function light pulse.
2q.ldb.G
S
1.3 10
2.2
22
1.2
0.1
1.0
.
f
-16
-19
coulomb).
W
ns
ns
ns
%
%
J:
The electron transit time is the interval between the arrival of delta function
light pulse at the entrance window of the tube and the time when the anode
output reaches the peak amplitude. In measurement, the whole photocathode is illuminated.
Also called transit time jitter. This is the fluctuation in electron transit time
K:
between individual pulses in the signal photoelectron mode, and may be
defined as the FWHM of the frequency distribution of electron transit times.
Hysteresis is temporary instability in anode current after light and voltage
L:
are applied.
l
max.
l
min.
TIME
TPMSB0002EA
ANODE
CURRENT
567 (minutes)
0
l
i
l
l
max.
Hysteresis =100(%)
min.
l
i
(1)Current Hysteresis
The tube is operated at 750 volts with an anode current of 1 micro-ampere for
5 minutes. The light is then removed from the tube for a minute. The tube is
then re-illuminated by the previous light level for a minute to measure the
variation.
(2)Voltage Hysteresis
The tube is operated at 300 volts with an anode current of 0.1 micro-ampere
for 5 minutes. The light is then removed from the tube and the supply voltage
is quickly increased to 800 volts. After a minute, the supply voltage is then
reduced to the previous value and the tube is re-illuminated for a minute to
measure the variation.
Figure 2: Anode Luminous Sensitivity and Gain
Characteristics
TPMSB0003EB
4
10
3
10
2
10
1
10
TYPICAL ANODE SENSITIVITY
8
10
7
10
6
10
5
10
GAIN
TYPICAL GAIN
0
10
–1
10
ANODE LUMINOUS SENSITIVITY (A/lm)
–2
10
200300
MINIMUM ANODE SENSITIVITY
500700
1000
1500
4
10
3
10
2
10
SUPPLY VOLTAGE (V)
Figure 4: Typical Temperature Coefficient of Anode
Sensitivity
TPMSB0005EA
160
140
800nm
600nm
Figure 3: Typical Time Response
TPMSB0004EB
100
80
60
40
20
10
8
TIME (ns)
6
4
2
1
300
TRANSIT TIME
RISE TIME
500700
10001500
SUPPLY VOLTAGE (V)
Figure 5: Typical Temperature Characteristic of Dark
Current (at 1000V, after 30minute storage)
TPMSB0006EA
100
120
100
80
60
ANODE SENSITIVITY (%)
40
20
0
400nm
–
40
–
200+20
TEMPERATURE (°C)
+40
10
1
ANODE DARK CURRENT (nA)
0.1
0.01
–
40
–
200+20
TEMPERATURE (°C)
+40
PHOTOMULTlPLlER TUBES R928, R955
Figure 6: Dimensional Outline and Basing Diagram (Unit : mm)
28.5 1.5
T9
BULB
PHOTOCATHODE
24MIN.
11 PIN BASE
JEDEC No. B11-88
32.2 0.5
8MIN.
49.0 2.5
80MAX.
94MAX.
DY6
DY7
6
7
8
9
10
11
K
DY4
DY3
DY2
DY5
3
DY1
5
4
2
1
DIRECTION OF LIGHT
BOTTOM VIEW
(BASING DIAGRAM)
TPMSA0008EA
DY8
DY9
P
Hybrid Assembly of R928
H957-08
The H957-08 integrates on R928, a voltage-divider circuit, and a high
voltage power supply into a compact magnetic shield case. It can be
readily operated by input of 15Vdc.
Figure 7: Optional Accessories (Unit : mm)
Socket
(E678 – 11A)
49
38
33
3.5
5
29
418
TACCA0064EA
Hamamatsu also provides C4900 series compact high voltage power supplies and C6270 series DP type socket assemblies which incorporate a
DC to DC converter type high voltage power supply.
D Type Socket Assembly E717-21
SOCKET
PMT
3.5
33.0 0.3
4.8
41.0 0.5
450 10
5
38.0 0.3
49.0 0.3
29
31.0 0.5
HOUSING
(INSULATOR)
POTTING
COMPOUND
PIN No.
10
P
DY9
9
DY8
8
DY7
7
DY6
6
DY5
5
DY4
4
DY3
3
DY2
2
DY1
1
K
11
R10
R9
R8
R7
R6
R5
R4
R3
R2
R1
C3
C2
C1
R to R10
C1 to C3
SIGNAL GND
SIGNAL OUTPUT RG-174/U
(BLACK)
POWER SUPPLY GND
AWG22 (BLACK)
: 330k
: 0.01 F
–HV
AWG22 (VIOLET)
TACCA0002ED
Warning–Personal Safety Hazards
Electrical Shock–Operating voltages applied to this
Hamamatsu Photonics Deutschland GmbH: Arzbergerstr. 10, D-82211 Herrsching am Ammersee, Germany, Telephone: (49)8152-375-0, Fax: (49)8152-2658
France:
Hamamatsu Photonics France S.A.R.L.: 8, 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:
North Europe:
Italy:
Hamamatsu Photonics UK Limted: Lough Point, 2 Gladbeck Way, Windmill Hill, Enfield, Middlesex EN2 7JA, United Kingdom, Telephone: (44)181-367-3560, Fax: (44)181-367-6384