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Электронный компонент: R4330-02

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lnformation furnished by HA MAM ATS U is believed to be reliabIe. However, no responsibility 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.
1997 Hamamatsu Photonics K.K.
Subject to local technical requirements and regulations, availability of products included in this promotional material may var y. Please consult with our sales office.
PHOTOMULTlPLlER TUBES
R3310-02, R4330-02
InGaAs (Cs) Photocathode, Wide Spectral Response, 51mm (2") Dia., Head-on Type
For Photon Counting : Low Dark Counts, Excellent P.H.D.
GENERAL
FEATURES
Parameter
Description/Value
Unit
Spectral Response
Hamamatsu R3310-02 and R4330-02 are 51mm (2") diameter head-on type photomultiplier tubes having InGaAs (Cs) photocath-
odes, and linear focused CuBeO dynodes. The InGaAs (Cs) photocathode allows high sensitivity over a wide spectral range up to
1040nm.
The R3310-02 and the R4330-02 are selected for photon counting, and they feature low dark counts and excellent pulse height
distribution (PHD) of single photoelectrons.
Wavelength of Maximum Response
R3310-02
300 to 1040
nm
R4330-02
160 to 1040
nm
R3310-02
Borosilicate glass (K-free)
R4330-02
Synthetic silica glass
nm
Photocathode
MateriaI
400
Structure
Approx. 2
pF
Anode to Last Dynode
Approx. 3
pF
Anode to All Other Electrodes
Minimum Effective Area
InGaAs(Cs)
Secondary Emitting Surface
Cu-BeO
mm
Window Material
Weight
10 10
g
110
g
93
R3310-02
R4330-02
Dynode
Direct Interelectrode Capacitances
Base
Linear Focused
Number of Stages
10
21-pin Base
E67821D (Option)
Mode
Opaque
SuitabIe Socket
E67821C (Supplied)
Wide Spectral Response
High Quantum Efficiency in IR ...........
Fast Rise Time ......................................
Excellent Single Photoelectron
Pulse Height Distribution
........................... Peak to Valley Ratio 2.3 (at 20 )
Low Dark Counts ....................... 30cps Typ. (at 20 )
APPLICATIONS
Raman Spectroscopy
Fluorescent Spectroscopy
Astrophysical Measurement
Laser Detection
0.25% at 1 m
3.0ns at 1500V
Figure 1: Typical Spectral Response
R3310-02 ...........................................
R4330-02 ............................................
300 to 1040nm
160 to 1040nm
TPMHB0051EA
100
300
500
700
900
WAVELENGTH (nm)
10
2
CATHODE RADIANT SENSITIVITY (mA/W)
QUANTUM EFFICIENCY (%)
1100
10
1
10
0
10
1
10
2
QUANTUM
EFFICIENCY
R4330-02
R3310-02
R3310-02
R4330-02
CATHODE
RADIANT
SENSITIVITY
PHOTOMULTlPLlER TUBES R3310-02, R4330-02
CHARACTERISTlCS (at 25 )
Parameter
Min.
Typ.
Max.
Cathode Sensitivity
Anode Dark Current
Single Photoelectron PHD (Peak to Valley Ratio)
5
20
150
Radiant at 253.7nm (Hg-Line) R4330 Series
150
Red/White Ratio
0.4
at 852.1nm (Cs-Line)
at 852.1nm (Cs-Line)
at 1000nm
30
at 900nm
at 900nm
9.4
at 1000nm
at 1000nm
8.1
at 253.7nm (Hg-Line) R4330 Series
2
Anode Pulse Rise Time
3.0
Electron Transit Time
23
Time Response
Quantum Efficiency
80
1.1
0.13
0.25
15
Anode Sensitivity
Gain
Equivalent Anode Dark Current
Unit
Luminous
Radiant at 253.7nm (Hg-Line) R4330 Series
Luminous
50
15
1.0 10
4
3.1 10
3
2.7 10
3
6.6 10
2
3.3 10
5
30
2.3
nA
mA/W
mA/W
mA/W
mA/W
ns
ns
A/lm
%
%
A/lm
A/W
A/W
A/W
A/W
cps
E
F
F
G
H
H
J
K
H
L
M
MAXIMUM RATINGS (Absolute Maximum Values)
Parameter
Value
Supply Voltage
Between Anode and Cathode
Between Anode and Last Dynode
2200
250
1
80 to +50
Vdc
Vdc
A
Average Anode Current
Unit
Ambient Temperature
D
A
10
pA
Average Cathode Current
C
6 10
6
cps
Average Pulse Count Rate
B
NOTES
A
B
C
D
E
F
G
H
J
K
Averaged over any interval of 30 seconds maximum.
Measured at single photoelectron level. The discriminator level is set at valley
point.
In practical operation, the cathode current should be lower than 2pA to pre-
vent shortening the life of the photocathode.
For cooling operation, another ceramic socket, type number E678-21D is rec-
ommended, because the teflon socket type number E678-21C supplied with the
tube is not suitable for cooling operation due to its high thermal expansion coef-
ficient. Alternatively, it is recommended to solder a resistor, capacitor, etc. di-
rectly on stem pins using a socket contact (100-2520S) supplied by Winchester.
Supply voltage is 150 volts between the cathode and all other electrodes.
The light source is a tungsten filament lamp operated at a distribution tempera-
ture of 2856K.
The quotient of the cathode sensitivity measured with the light source is the
same as Note passing through a red filter (Toshiba R-68) divided by the
cathode luminous sensitivity without the red filter.
Measured with supply voltage and voltage distribution ratio in Table 1.
Measured with supply voltage to provide the anode luminous sensitivity of 40
(A/lm) and the voltage distribution ratio in Table 1 after 30 minutes storage in the
darkness.
Measured with supply voltage that gives 2 10
6
gain and with the voltage distri-
bution ratio shown in Table 1 after one hour storage in the cooler set at 20 .
The discriminator is set at 1/3 of a single photoelectron level.
The rise time is the time it takes 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.
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 when the output
pulse reaches the peak amplitude. In measurement the entire photocathode is
illuminated.
Electrodes
K
Dy1 Dy2 Dy3 Dy4 Dy5 Dy6 Dy7 Dy8
Distribution Ratio
3
1.5
1
1
1
1
1
1
1
SuppIy Voltage : 1500Vdc, K : Cathode, Dy : Dynode, P : Anode
1
1
Table 1:Voltage Distribution Ratio
WarningPersonal Safety Hazards
Electrical Shock Operating voltages
applied to this device present a shock hazard.
E
Dy9 Dy10
P
L
M
Figure 2: Typical Single Photoelectron
Pulse Height Distribution
Figure 3: Typical Gain
Figure 6: Typical Dark Counts vs. Temperature
Figure 4: Typical Time Response
Figure 5: Typical Temperature Coefficient of Quantum Efficiency
As Figure 6 shows, the dark counts of the R3310-02 and
R4330-02 decreases by cooling the tube. Therefore, when
performing photon counting, it is recommended that the tube be
cooled down to about 20 . The cooler C2761 which features
temperature control from 30 to 0 is available from
HAMAMATSU.
COOLING
TPMHB0280EA
0
1024
512
CHANNEL NUMBER (CH)
0
0.2
0.4
0.6
0.8
1.0
COUNTS PER CHANNEL
FULL SCALE
(SIGNAL
+
DARK)
: 1 10
4
FULL
SCALE
(DARK)
:
1 10
3
WAVELENGTH OF INCIDENT LIGHT : 800 (nm)
LOWER LEVEL DISCRI. : 87 (CH)
SIGNAL
+
DARK COUNTS : 5526 (cps)
DARK COUNTS
: 30 (cps)
TEMPERATURE
:
20 ( )
SIGNAL
+
DARK
DARK
TPMHB0044EA
500
1000
1500
2000
2500
10
2
10
3
10
4
10
5
10
6
10
7
10
8
SUPPLY VOLTAGE (V)
GAIN
TPMHB0045EA
500
1000
1500
2000
3000
10
1
TIME (ns)
SUPPLY VOLTAGE (Vdc)
TRANSIT TIME
10
0
10
2
RISE TIME
TPMHB0046EB
2
400
500
600
700
800
900
1000
1.5
1
0.5
0.5
1.5
2
1
0
TEMPERATURE COEFFICIENT (%/ )
WAVELENGTH (nm)
300
TEMPERATURE RANGE:
10 to
+
40 ( )
TPMHB0047EA
40
30
20
10
0
10
20
10
0
10
1
10
2
10
3
10
4
10
5
TEMPERATURE ( )
DARK COUNTS (cps)
TPMH1021E04
SEP. 1997
PHOTOMULTlPLlER TUBES R3310-02, R4330-02
Figure 7: Dimensional Outline and Basing Diagram (Unit : mm)
a) TUBE
b) PHOTOCATHODE
Orientation of Photocathode
with Respect to Base pin
X Axis Cross Section
Y Axis Cross Section
c) SOCKET(Refer to NOTES )
E67821C (SUPPLIED)
REMARKS
H A c o a t i n g
T h e R 3 3 1 0 - 0 2 a n d R 4 3 3 0 - 0 2 a r e c o a t e d w i t h t h e c o n d u c t i v e p a i n t c o n -
n e c t e d t o t h e c a t h o d e , w h i c h i s c o v e r e d w i t h a n i n s u l a t i n g m a t e r i a l ( H A c o a t -
i n g ) . T h i s m e t h o d d e c r e a s e s n o i s e . C a r e s h o u l d b e t a k e n n o t t o d a m a g e t h e
i n s u l a t i n g c o v e r w r a p p i n g a r o u n d t h e b u l b .
CAUTIONS
U s e t h e H A M A M A T S U S O C K E T E 6 7 8 - 2 1 C o r E 6 7 8 - 2 1 D .
W h e n s o l d e r i n g t h e v o l t a g e d i v i d e r s t o t h e s o c k e t , t h e P M T s h o u l d b e i n -
s e r t e d i n t h e s o c k e t .
E67821D (OPTION)
TPMHA0286EA
X
Y
51
1
10
6.6
3.4
1.6
PHOTOCATHODE
CENTER
19
88 2
14MAX.
HA-COATING
(Conductive
paint connected
to the cathode)
LIGHT SHIELD
(SILICONE)
15
PHOTOCATHODE
PHOTOCATHODE
(10 10)
D
TPMHA0022EB
Bottom View
Top View
Dy
K
P
IC
: Dynode
: Photocathode
: Anode
: Internal Connection
(should not be used)
SHORT PIN
1
2
3
4
5
6
7
9
8
11 12
13
14
15
16
17
18
19
20
21
K
DY2
DY4
DY1
P
DY8
DY10
IC
IC
IC IC DY9
DY7
DY5
DY3
DY6
IC
IC
IC
IC
IC
10
33
2
PIN 3
PIN 1
PIN 14
90
2.5
TPMHA0023EB
22.0
15
20 1
PHOTOCATHODE
22.0
17.5 1.0
PHOTOCATHODE CENTER
19
15
1
TUBE CENTER
1.6
PHOTOCATHODE
7.5 1.0
17.5 1.0
10.5
20 1
INPUT WINDOW
INPUT WINDOW
11.5
10
TACCA0066EC
R5
56.8
19
51
5
4
13
6.5
TACCA0054EB
48
7.5
3.0
18.5
4.2
23.5
44.5
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, 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 Limted: Lough Point, 2 Gladbeck Way, Windmill Hill, Enfield, Middlesex EN2 7JA, United Kingdom, Telephone: (44)181-367-3560, Fax: (44)181-367-6384
North Europe: Hamamatsu Photonics Norden AB: Frgatan 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.: Via Della Moia, 1/E, 20020 Arese, (Milano), Italy, Telephone: (39)2-935 81 733, Fax: (39)2-935 81 741