Subject to local technical requirements and regulations, availability of products included in this promotional material may vary. Please consult with our sales office. 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. ? 1998 Hamamatsu Photonics K.K.
Figure 1: Typical Spectral Response
PHOTOMULTIPLIER TUBES R1463, R1463P
CHARACTERISTICS (at 25°C)
Parameter
Min.Unit Cathode Sensitivity
Anode Sensitivity D
Gain D
Anode Dark Current D (After 30 minute storage in the darkness)
Anode Dark Count D (After 3 hour storage in the darkness) (for R1463P)
Time Response
μA/lm mA/W mA/W %—A/lm A/W A/W —nA cps ns ns
80———0.1530———————
————————201000——
Max.Typ.1205119190.21205.1 × 1041.9 × 1041 × 106
49002.524
Luminous B
Radiant at 420nm at 633nm
Quantum Efficiency at 290nm Red/White Ratio C Luminous E
Radiant at 420nm at 633nm
Anode Pulse Rise Time D, F
Electron Transit Time D,G
NOTES
A:Averaged over any interval of 30 seconds maximum.
B:The light source is a tungsten filament lamp operated at a distribution temperature of 2856K. The light input is 10-3 lumen. Supply voltage is 150 volts
between the cathode and all other electrodes connected together as anode.
C:Red/White Ratio is the quotient of the cathode current measured using a 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.
D: Measured with the anode-to-cathode supply voltage and voltage distribution ratio shown in Table 1.E: The light input is 10-8 lumens with the same light source as Note B.
F: 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.
G: The electron transit time is the interval between the arrival of a delta function light pulse at the entrance window of the tube and the time the output pulse
reaches the peak amplitude. In measurement the entire photocathode is illuminated.
Supply Voltage: 1000Vdc, K: Cathode, Dy: Dynode, P: Anode
Table 1: VOLTAGE DISTRIBUTION RATIO
Electrodes Distribution Ratio K Dy11Dy21Dy31Dy41Dy51Dy61Dy71Dy81Dy91
11Dy10P
100
10
1
0.1
0.01
WAVELENGTH (nm)C A T H O D E R A D I A N T S E N S I T I V I T Y (m A /W )Q U A N T U M E F F I C I E N C Y (%)
Figure 2: Anode Sensitivity and Gain Characteristics
104
103102
10110010-110-2
108
107
106
105
104
103
102SUPPLY VOLTAGE (V)
A N O D E L U M I N O U S S E N S I T I V I T Y (A /l m )
G A I N
Figure 3: Typical Time Response
TPMHB0532EA
Figure 4: Typical Temperature Coefficient of Anode Sensitivity
TPMHB0533EA
200
100806040
20
10864
2
1
SUPPLY VOLTAGE (V)
T I M E (n s )
+1.5
+1.0
+0.5
-1.0
-0.5
-1.5
200400600800
WAVELENGTH (nm)
T E M P E R A T U R E C O E F F I C I E N T (%/°C )
Figure 5: Typical Temperature Characteristic of Dark Current and Dark Counts (R1463P)
TPMHB0534EA
Figure 6: Typical Single Photoelectron Pulse Height Distribution (R1463P)
TPMHB0535EA
100
1010.1
0.01
10000
1000
100
10
1
TEMPERATURE (°C)
A N O D E D A R K C U R R E N T (n A )
A N O D E D A R K C O U N T (c p s )
0.3m m 2m 3m
PULSE HEIGHT
C O U N T R A T E (C o u n t s /C h a n n e l )
INCIDENT LIGHT : 600nm TEMPERATURE : 25°C SUPPLY VOLTAGE: 1500V
SIGNAL + NOISE = Σ = 8100cps NOISE = Σ = 900cps
Σ (Count) = Σ (Count)M is defined to satisfy the
following equation
m 0.3m
0.3m
3m 3m
m
3m
0.3m
TPMH1216E01AUG. 1998
HAMAMATSU PHOTONICS K.K., Electoron Tube Center
314-5, Shimokanzo, Toyooka-village, Iwata-gun, Shizuoka-ken, 438-0193, Japan, Telephone: (81)539/62-5248, Fax: (81)539/62-2205
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)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: Hamamatsu Photonics UK Limited: Lough Point, 2 Gladbeck Way, Windmill Hill, Enfield, Middlesex EN2 7JA, United Kingdom, Telephone: (44)181-367-3560, Fax: (44)181-367-6384North Europe: Hamamatsu Photonics Norden AB: F?r?gatan 7, S-164-40 Kista Sweden, Telephone: (46)8-703-29-50, Fax: (46)8-750-58-95
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
TACCA0005EA
TPMHA0014EA
TACCA0022EA
TACCA0021EA
TPMHA0435EA
Figure 7: Dimensional Outline and Basing Diagram (Unit: mm)
Figure 8: Optional Socket Assembly E849-34 and E849-35 (Unit: mm)
PHOTOMULTIPLIER TUBES R1463, R1463P
Socket (E678-13A)
DY4SHORT PIN
R1463
R1463P
E849-34
E849-35
The E849-34 and E849-35 are socket assemblies specifically designed for 1/2 inch diameter, 10 stage, head-on type photomultiplier tubes having a 13-pin glass base. It contains a voltage-divider network potted with silicone rubber, thus eliminating troublesome soldering for making up the divider network.
330k ?
R1 to R11 :SOCKET
: 330k ?: 0.01μF
Warning - Personal Safety Hazards Electrical Shock — Operating voltage applied to this device presents shock hazard.