HAMAMATSU R2693_07

PHOTOMULTIPLIER TUBES
R2693, R2693P
Transmission Mode Low Noise Bialkali Photocathode
28 mm (1-1/8 inch) Diameter, Side-on Type
FEATURES
●Low Dark Current
●Low Dark Counts (R2693P)
●Wide Photocathode
●Excellent Spatial Uniformity
●Fast Time Response
APPLICATIONS
●Fluorescence Detector
●Chemiluminescence Detector
●Light Scattering Detector
SPECIFICATIONS
Figure 1: Electron Trajectories
GENERAL
Parameter
Description/Value
185 to 650
Spectral Response
375
Wavelength of Maximum Response
MateriaI
Low noise bialkali
Photocathode
Minimum Effective Area
16 (H) × 18 (W)
UV glass
Window Material
Structure
Circular-cage
Dynode
Number of Stages
9
1.2
Direct Interelectrode Anode to Last Dynode
Anode to All Other Electrodes
3.4
Capacitances
Base
11-pin base JEDEC No. B11-88
Operating Ambient Temperature
-30 to +50
Storage Temperature
-30 to +50
SuitabIe Socket
E678–11A (Sold Separately)
E717–63 (Sold Separately)
SuitabIe Socket Assembly
E717–74 (Sold Separately)
Unit
nm
nm
—
mm
—
—
—
pF
pF
—
°C
°C
—
—
—
3rd DYNODE
1st DYNODE
FOCUSING
ELECTRODES
2nd DYNODE
GLASS
BULB
PHOTOELECTRONS
PHOTOCATHODE
LIGHT
TPMSC0003EC
Figure 2: Typical Spatial Uniformity
X
●Y-Axis
100
100
90
90
80
80
RELATIVE OUTPUT (%)
Y
RELATIVE OUTPUT (%)
●X-Axis
70
60
50
40
30
20
SPOTSIZE: 1 mm
SUPPLY VOLTAGE: 1000 V
WAVELENGTH: 400 nm
60
50
40
30
20
10
0
-15
70
10
-10
CATHODE
ANODE
5
0
POSITION (mm)
5
10
15
0
-15
-10
CATHODE
ANODE
5
0
5
10
15
POSITION (mm)
TPMSB0066EB
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. ©2007 Hamamatsu Photonics K.K.
PHOTOMULTIPLIER TUBES R2693, R2693P
MAXIMUM RATINGS (Absolute Maximum Values)
Parameter
Between Anode and Cathode
Supply Voltage
Between Anode and Last Dynode
Average Anode Current A
Unit
V
V
mA
Value
1250
250
0.1
CHARACTERISTlCS (at 25 °C)
Parameter
Quantum Efficiency at 375 nm
Luminous B
Radiant at 375 nm (Peak)
Blue Sensitivity Index C
Luminous D
Radiant at 375 nm (Peak)
Cathode Sensitivity
Anode Sensitivity
Gain D
Anode Dark Current E (After 30 min Storage in Darkness)
Pulse Hight Distribution F
Anode Dark Counts
at Plateau Voltage G
ENI (Equivalent Noise Input) H
Anode Pulse Rise Time J
D
Time Response
Electron Transit Time K
Transit Time Spread (FWHM) L
M Current Hysteresis
Anode Current Stability
Voltage Hysteresis
R2693
for General Purpose
Min.
Typ.
Max.
—
—
20.5
—
30
50
—
—
62
—
—
7.0
—
100
300
—
—
3.7 × 105
—
—
6 × 106
5.0
—
0.5
—
—
—
—
—
—
—
—
8.6 × 10-17
—
—
1.2
—
—
18
—
—
1.0
—
—
0.5
—
—
1.0
R2693P
for Photon Counting
Min.
Typ.
Max.
—
20.5
—
30
50
—
—
62
—
—
7.0
—
100
300
—
—
3.7 × 105
—
—
—
6 × 106
—
2.0
0.1
—
50
20
—
50
10
—
—
3.9 × 10-17
—
—
1.2
—
—
18
—
—
1.0
—
—
0.5
—
—
1.0
Unit
%
µA/lm
mA/W
µA/lm-b
A/lm
A/W
—
nA
s-1
s-1
W
ns
ns
ns
%
%
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 2856 K. Supply voltage is 100 V
between the cathode and all other electrodes connected together
as anode.
C: The value is cathode output current when a blue filter (Corning
CS 5-58 polished to 1/2 stock thickness) is interposed between
the light source and the tube under the same condition as Note B.
D: Measured with the same light source as Note B and with the
voltage distribution ratio shown in Table 1 below.
Table 1: Voltage Distribution Ratio
Electrodes K Dy1 Dy2 Dy3
Ratio
1
1
1
1
• • • •
Dy7 Dy8 Dy9 P
1
1
1
J: 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.
K: 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 amplitube. In
measurement, the whole photocathode is illuminated.
L: Also called transit time jitter. This is the fluctuation in electron
transit time between individual pulses in the single photoelectron
mode, and may be defined as the FWHM of the frequency
distribution of electron transit times.
M: Hysteresis is temporary instability in anode current after light and
voltage are applied.
• • • • •
SuppIy Voltage: 1000 V, K: Cathode, Dy: Dynode, P: Anode
• • • •
• • • •
K
Dy1 Dy2 Dy3
1
1
1
1
• • • •
Dy7 Dy8 Dy9 P
1
2
1
SuppIy Voltage: Plateau Voltage, K: Cathode, Dy: Dynode, P: Anode
where
× 100 (%)
l max.
li
l min.
TIME
0
5
6
7 (minutes)
TPMSB0002EA
• • • • •
E: Measured with the same supply voltage and voltage distribution
ratio as Note D after removal of light.
F: Measured at the voltage producing the gain of 1 × 106
G: Plateau voltage at the test up in HPK
H: 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.
ENI =
lmin.
li
Dy7 Dy8 Dy9 P
•
1
1
1
SuppIy Voltage: Note F, K: Cathode, Dy: Dynode, P: Anode
Plateau
Electrodes
Ratio
lmax.
Hysteresis =
ANODE
CURRENT
Pulse Height Distribution
Electrodes K Dy1 Dy2 Dy3
Ratio
1
1
1
1
2q.ldb.G.∆f
S
q = Electronic charge (1.60 × 10-19 coulomb).
ldb = Anode dark current (after 30 minutes 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
wavelength of peak response.
(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.
Figure 3: Typical Spectral Response
Figure 4: Typical Time Response
TPMSB0060EA
200
CATHODE
RADIANT
SENSITIVITY
TPMSB0061EA
100
80
60
10
40
QUANTUM
EFFICIENCY
TRAN
TIME (ns)
CATHODE RADIANT SENSITIVITY (mA/W)
QUANTUM EFFICIENCY (%)
100
1
SIT TIM
E
20
10
8
6
4
0.1
2
RISE
1
0.01
200
400
300
800
600
500
Figure 5: Typical Gain and Anode Dark Current (R2693)
TPMSB0062EA
1.0
10-7
G
N
EN
T
GAIN
10-8
10-9
AR
K
C
U
R
R
104
10-10
1500
TPMSB0063EA
0.8
SIGNAL+DARK
0.6
WAVELENGTH OF INCIDENT LIGHT
: 400 nm
: 1000 V
SUPPLY VOLTAGE
SIGNAL+DARK COUNTS : 5364 s-1
: 15 s-1
DARK COUNTS
AMBIENT TEMPERATURE : +25
0.4
0.2
AN
O
D
E
D
103
COUNTS PER CHANNEL
106
FULL SCALE (SIGNAL+DARK): 1 × 104
FULL SCALE (DARK)
: 1 × 103
10-6
ANODE DARK CURRENT (A)
107
105
1000
Figure 6: Typical Single Photoelectron Pulse Height
Distribution (R2693P)
10-5
AI
700
SUPPLY VOLTAGE (V)
WAVELENGTH (nm)
108
TIME
DARK
102
0
10-11
101
300
400
500
600
800
1000
0
200
400
600
800
1000
CHANNEL NUMBER (ch)
10-12
1300
DISCRIMINATION LEVEL
SUPPLY VOLTAGE (V)
Figure 7: Typical Temperature Coefficient
of Anode Sensitivity
TPMSB0064EA
100
TPMSB0065EB
+0.8
ANODE DARK CURRENT (nA)
TEMPERATURE COEFFICIENT (%/°C)
+1.2
Figure 8: Typical Temperature Characteristics
of Dark Current (R2693)
(at 1000 V, after 30 min storage)
+0.4
0
-0.4
10
1
0.1
-0.8
-1.2
200
0.01
300
400
500
WAVELENGTH (nm)
600
700
0
20
40
60
TEMPERATURE (°C)
80
100
PHOTOMULTIPLIER TUBES R2693, R2693P
Figure 9: Dimensional Outline and Basing Diagram (Unit: mm)
Figure 10: Socket (Unit: mm) Sold Separately
29.0 ± 1.7
E678-11A
18 MIN.
49
38
PHOTOCATHODE
5
DY6
6
7
8 DY8
DY2
33
76 MAX.
DY7
DY3 3
90 MAX.
49.0 ± 2.5
DY4 4
9 DY9
2
10
1
3.5
16 MIN.
DY5
5
P
11
K
DY1
DIRECTION OF LIGHT
18
4
29
32.2 ± 0.5
11 PIN BASE
JEDEC No. B11-88
HA COATING
TPMSA0007ED
Figure 11: D Type Socket Assembly (Unit: mm)
TACCA0064EA
Sold Separately
E717-63
E717-74
HOUSING
(INSULATOR)
10
P
R10
49.0 ± 0.3
DY8
8
DY7
7
26.0±0.2
TOP VIEW
5
4
R1 to R10 : 330 kΩ
C1 to C3 : 10 nF
31.0 ± 0.5
DY4
4
DY3
3
DY2
2
DY1
K
1
A
G
2.7
R5
R4
HOUSING
(INSULATOR)
POTTING
COMPOUND
22.4±0.2
K
°
10
R2
30°
8
-HV
AWG22 (VIOLET)
C2
DY7
7
R8
C1
DY6
6
DY5
5
DY4
4
DY3
3
DY2
2
DY1
K
1
R6
R5
R1 to R10 : 330 kΩ
C1 to C3 : 10 nF
R3
0.7
R1
11
DY8
R4
SIDE VIEW
R3
C3
R9
R7
2
6
DY5
R10
9
32.0±0.5
C1
7
DY6
R6
0.7
30.0 +0
-1
450 ± 10
C2
R7
29.0 ± 0.3
SIGNAL
OUTPUT (A)
GND (G)
10
DY9
R8
SOCKET
PIN No.
P
9
R9
38.0 ± 0.3
C3
PMT
14.0±0.5
DY9
SIGNAL GND
SIGNAL OUTPUT
RG-174/U(BLACK)
POWER SUPPLY GND
AWG22 (BLACK)
26.0±0.2
SOCKET
PIN No.
32.0±0.5
PMT
3.5
33.0 ± 0.3
5
R2
R1
11
-HV (K)
4- 2.8
R13
* "Wiring diagram applies when -HV is supplied."
To supply +HV,connect the pin "G" to +HV, and the pin
"K" to the GND.
BOTTOM VIEW
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.
TACCA0277EA
Warning–Personal Safety Hazards
Electrical Shock–Operating voltages applied to this
device present a shock hazard.
WEB SITE 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.: 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 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]
TPMS1014E02
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]
JAN. 2007. IP