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R2693 查看數據表(PDF) - Hamamatsu Photonics

零件编号
产品描述 (功能)
比赛名单
R2693
Hamamatsu
Hamamatsu Photonics Hamamatsu
R2693 Datasheet PDF : 4 Pages
1 2 3 4
PHOTOMULTIPLIER TUBES R2693, R2693P
MAXIMUM RATINGS (Absolute Maximum Values)
Parameter
Value
Unit
Supply Voltage
Between Anode and Cathode
Between Anode and Last Dynode
1250
250
V
V
Average Anode Current A
0.1
mA
CHARACTERISTlCS (at 25 °C)
Parameter
Cathode Sensitivity
Anode Sensitivity
Gain D
Quantum Efficiency at 375 nm
Luminous B
Radiant at 375 nm (Peak)
Blue Sensitivity Index C
Luminous D
Radiant at 375 nm (Peak)
Anode Dark Current E (After 30 min Storage in Darkness)
Anode Dark Counts
Pulse Hight Distribution F
at Plateau Voltage G
ENI (Equivalent Noise Input) H
Anode Pulse Rise Time J
Time Response D
Electron Transit Time K
Transit Time Spread (FWHM) L
Anode Current Stability M Current Hysteresis
Voltage Hysteresis
R2693
for General Purpose
Min. Typ. Max.
20.5
30
50
62
7.0
100
300
3.7 × 105
6 × 106
0.5
5.0
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
0.1
2.0
20
50
10
50
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 • • • • Dy7 Dy8 Dy9 P
Ratio
1
1
1
1 •••••
1
1
1
SuppIy Voltage: 1000 V, K: Cathode, Dy: Dynode, P: Anode
Pulse Height Distribution
Electrodes K Dy1 Dy2 Dy3 • • • • Dy7 Dy8 Dy9 P
Ratio
1
1
1
1 •••••
1
1
1
SuppIy Voltage: Note F, K: Cathode, Dy: Dynode, P: Anode
Plateau
Electrodes K Dy1 Dy2 Dy3 • • • • Dy7 Dy8 Dy9 P
Ratio
1
1
1
1 •••••
1
2
1
SuppIy Voltage: Plateau Voltage, K: Cathode, Dy: Dynode, P: Anode
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 = 2q.ldb.G.f
S
where 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.
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.
Hysteresis =
lmax. lmin. × 100 (%)
li
li
l max.
l min.
TIME
0
5
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.

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