HAMAMATSU R7518

PHOTOMULTIPLIER TUBES
R7518
R7518P (For Photon Counting)
High Sensitivity with Low Noise Photocathode
FEATURES
●Spectral Response .................................. 185 nm to 730 nm
●High Cathode Sensitivity
Luminous ......................................................... 130 µA/lm
Radiant at 410 nm ............................................. 85 mA/W
●High Anode Sensitivity (at 1000 V)
Luminous ......................................................... 1560 A/lm
Radiant at 410 nm ..................................... 10.2 × 105 A/W
●Low Dark Current ....................................................... 0.2 nA
●Low Dark Counts (R7518P) ......................................... 10 s-1
APPLICATIONS
●Chemiluminescence Detection
●Bioluminescence Detection
●Fluorescence Spectrometer
●SO2 Monitor (UV Fluorescence)
SPECIFICATIONS
GENERAL
Parameter
Spectral Response
Wavelength of Maximum Response
MateriaI
Photocathode
Minimum Effective Area
Window Material
Secondary Emitting Surface
Structure
Dynode
Number of Stages
Anode to Last Dynode
Direct Interelectrode
Anode to All Other Electrode
Capacitances
Base
Weight
Operating Ambient Temperature
Storage Temperature
SuitabIe Socket
SuitabIe Socket Assembly
Description/Value
185 to 730
410
Low noise bialkali
8 × 24
UV glass
Low noise bialkali
Circular-cage
9
4
6
11-pin base JEDEC No. B11-88
45
-30 to +50
-30 to +50
E678–11A (Sold Separately)
E717–63 (Sold Separately)
Unit
nm
nm
—
mm
—
—
—
—
pF
pF
—
g
°C
°C
—
—
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. ©2005 Hamamatsu Photonics K.K.
PHOTOMULTIPLIER TUBES
R7518, R7518P (For Photon Counting)
MAXIMUM RATINGS (Absolute Maximum Values)
Parameter
Between Anode and Cathode
Supply Voltage
Between Anode and Last Dynode
Average Anode Current A
Value
1250
250
0.1
Unit
V
V
mA
CHARACTERISTlCS (at 25 °C)
R7518 for General Purpose R7518P for Photon Counting
Unit
Typ.
Max.
Min.
Min.
Typ.
Max.
—
%
Quantum Efficiency at 300 nm (Peak)
—
—
29
29
—
µA/lm
—
120
Luminous B
120
130
130
—
Cathode Sensitivity
—
mA/W
—
Radiant at 410 nm (Peak)
—
85
—
85
—
µA/lm-b
Blue Sensitivity Index (CS 5-58)
—
—
10
—
10
—
Luminous C
A/lm
1200
1200
1560
—
1560
Anode Sensitivity
—
A/W
Radiant at 400 nm
—
—
10.2 × 105
—
10.2 × 105
—
1.2 × 107
1.2 × 107
—
—
—
—
Gain D
2.0
Anode Dark Current E (After 30 min Storage in darkness)
0.2
0.2
nA
—
0.5
—
—
Anode Dark Counts E
—
10
s-1
—
50
—
—
ENI (Equivalent Noise Input) F
W
2.7 × 10-17
2.7 × 10-17
—
—
—
—
2.2
2.2
Anode Pulse Rise Time G
ns
—
—
—
—
Time Response D
Electron Transit Time
22
22
ns
—
—
—
—
Transit Time Spread (TTS) H
1.2
1.2
ns
—
—
—
—
Light Hysteresis
0.1
0.1
%
—
—
—
J
Anode Current Stability
—
Voltage Hysteresis
1.0
1.0
%
—
—
—
Parameter
NOTES
2q.ldb.G. f
(W)
S
where q = Electronic charge. (1.60 × 10-19 coulomb)
ldb = Anode dark current(after 30 minute storage) in amperes.
G = Gain.
f = Bandwidth of the system in hertz. (usually 1 hertz)
S = Anode radiant sensitivity in amperes per watt at the wavelength of peak response
ENI =
G: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.
H: 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.
J: Also called transit time jitter. This is the fluctuation in electron transit time
between individual pulses in the signal photoelectron mode, and may be
defined as the FWHM of the frequency distribution of electron transit times.
K: Hysteresis is temporary instability in anode current after light and voltage
are applied.
lmax.
Hysteresis =
lmin.
100 (%)
li
ANODE
CURRENT
A: Averaged over any interval of 30 seconds maximum.
B: The light source is a tungsten filament lamp operated at a distribution temperature of 2856 K. Supply voltage is 150 V between the cathode and all
other electrodes connected together as anode.
C: Measured with the same light source as Note B and with the anode-tocathode supply voltage and voltage distribution ratio shown in Table 1 below.
D: Measured with the same supply voltage and voltage distribution ratio as
Note E after removal of light.
E: Measured at the voltage producing the gain of 1 × 106.
F: ENI is an indication of the photon-limited signal-to-noise ratio. It refers to
the amount of light in watts to produce a signal-to-noise ratio of unity in the
output of a photomultiplier tube.
l max.
li
l min.
TIME
5
0
6
7 (minutes)
TPMSB0002EA
(1)Current Hysteresis
The tube is operated at 750 V with an anode current of 1 µA 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 V with an anode current of 0.1 µA for 5 minutes.
The light is then removed from the tube and the supply voltage is quickly
increased to 800 V. 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.
Table 1:Voltage Distribution Ratio
Electrodes
Distribution
Ratio
K
Dy1 Dy2 Dy3 Dy4 Dy5 Dy6 Dy7 Dy8 Dy9
1
1
1
1
1
1
1
1
1
P
1
SuppIy Voltage : 1000 V, K: Cathode, Dy: Dynode, P: Anode
Figure 1: Typical Spectral Response
10-5
CATHODE
RADIANT
SENSITIVITY
TPMSB0011EA
108
10-6
107
10-7
106
GAIN
105
10-9
CU
RR
EN
T
1
10-8
DA
RK
QUANTUM
EFFICIENCY
10-10
0.1
10-11
0.01
100
200
300
400
500
600
700
400
500
600
800
101
1500
1000
SUPPLY VOLTAGE (V)
WAVELENGTH (nm)
Figure 3: Typical Time Response
100
103
102
10-12
300
800
104
AN
O
DE
10
G
AI
N
100
ANODE DARK CURRENT (A)
CATHODE RADIANT SENSITIVITY (mA/W)
QUANTUM EFFICIENCY (%)
1000
Figure 2: Typical Gain and Anode Dark Current
TPMSB0177EA
Figure 4: Typical ENI vs. Wavelength
TPMSB0004EB
10-13
TPMSB0178EA
EQUIVALENT NOISE INPUT (W)
80
60
40
TRAN
SIT T
IME
TIME (ns)
20
10
8
6
10-14
10-15
10-16
4
RISE
10-17
100
TIME
200
300
400
500
600
700
800
2
WAVELENGTH (nm)
1
500
300
700
1000
1500
SUPPLY VOLTAGE (V)
Figure 5: Typical Single Photon Pulse Height
Distribution for R7518P
TPMSB0179EB
0.8
0.6
104
WAVELENGTH OF INCIDENT LIGHT: 450 (nm)
: 722 (V)
SUPPLY VOLTAGE
: 67 (ch)
LOWER LEVEL DISCRI.
PHOTON + DARK COUNT : 6021 (s-1)
: 10 (s-1)
DARK COUNT
AMBIENT TEMPERATURE : 25 (°C)
0.4
PHOTON+DARK
0.2
TPMSB0015EB
103
DARK COUNT (s-1)
LOWER LEVEL DISCRI.
COUNT PER CHANNEL
FULL SCALE 104 (PHOTON+DARK)
FULL SCALE 103 (DARK)
1.0
Figure 6: Typical Temperature Characteristics
of Dark Count for R7518P
102
101
100
DARK
0
200
400
600
800
CHANNEL NUMBER (CH)
1000
10-1
-20
0
+20
TEMPERATURE (°C)
+40
+50
PHOTOMULTIPLIER TUBES
R7518, R7518P (For Photon Counting)
Figure 7: Dimensional Outline and Basing Diagram (Unit: mm)
Figure 8: Socket E678-11A (Sold Separately)
28.5 ± 1.5
49
8 MIN.
38
PHOTOCATHODE
5
DY6
6
7
80 MAX.
94 MAX.
49.0 ± 2.5
DY7
8 DY8
DY3 3
DY2
33
24 MIN.
DY4 4
3.5
DY5
9 DY9
2
5
10 P
1
11
K
DY1
DIRECTION OF LIGHT
29
18
4
Bottom View
(Basing Diagram)
32.2 ± 0.5
11 PIN BASE
JEDEC No. B11-88
TACCA0064EA
TPMSA0001EB
Figure 9: D Type Socket Assembly E717-63 (Sold Separately)
PMT
3.5
33.0 ± 0.3
5
SOCKET
PIN No.
10
P
38.0 ± 0.3
49.0 ± 0.3
DY9
9
DY8
8
DY7
7
DY6
6
DY5
5
DY4
4
DY3
3
DY2
2
DY1
K
1
R9
C2
R8
C1
4
R6
R1 to R10 : 330 kΩ
C1 to C3 : 10 nF
R5
0.7
30.0 +0
-1
C3
R7
29.0 ± 0.3
450 ± 10
R10
SIGNAL GND
SIGNAL OUTPUT
RG-174/U(BLACK)
POWER SUPPLY GND
AWG22 (BLACK)
31.0 ± 0.5
R4
HOUSING
(INSULATOR)
POTTING
COMPOUND
R3
R2
R1
11
-HV
AWG22 (VIOLET)
TACCA0002EH
* 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.
Warning–Personal Safety Hazards
Electrical Shock–Operating voltages applied to this
device present a shock hazard.
WEB SITE http://www.hamamatsu.com
HAMAMATSU PHOTONICS K.K., Electron Tube Division
314-5, Shimokanzo, Iwata City, Shizuoka Pref., 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 E-mail: [email protected]
Germany: Hamamatsu Photonics Deutschland GmbH: Arzbergerstr. 10, D-82211 Herrsching am Ammersee, Germany, Telephone: (49)8152-375-0, Fax: (49)8152-2658 E-mail: [email protected]
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 E-mail: [email protected]
United Kingdom: Hamamatsu Photonics UK Limited: 2 Howard Court, 10 Tewin Road Welwyn Garden City Hertfordshire AL7 1BW, United Kingdom, Telephone: 44-(0)1707-294888, Fax: 44(0)1707-325777 E-mail: [email protected]
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 E-mail: [email protected]
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 E-mail: [email protected]
TPMS1060E02
APR. 2005. IP