Micro PMT Assembly and Module

MICRO PMT ASSEMBLY
MICRO PMT MODULES
MICRO PMT PHOTON COUNTING HEAD
World's smallest and lightest photomultiplier tube*
Micro PMT
* By our research (as of December 2015)
Easy to
mass produce
Micro PMT can be produced in high
volume while still maintaining high
reliability and performance. What
makes this possible is overall integrated usage of our in-house advanced technologies for MEMS (micro-electro-mechanical systems),
semiconductor manufacturing, electron trajectory design, vacuum
sealed packaging, and vacuum processing.
High shock
resistance
Tiny dimensions
Micro PMT devices offer strong
shock resistance since anodic bonding by MEMS technology is utilized
to join the silicon substrate to the
glass substrates. This high cushioning or shock resistance makes
them ideal for developing high-performance, hand-held testing
and analysis devices.
Micro PMT has a three-layer
structure where a silicon substrate is sandwiched between
two glass substrates. Utilizing
only three components gives
tiny dimensions impossible up
until now.
Customizing
support
High sensitivity
and fast response
Feel free to consult with us on
customizing to match customer
usage conditions and environments.
Full-scale Micro PMT image!
Micro PMT utilizes the same high
precision structure for electrode
arrangement as conventional
PMTs and so provides the high
sensitivity and fast response needed from a PMT.
■ Micro PMT internal structure
CONNECTION TERMINAL
VACUUM TUBE
SECONDARY ELECTRON
GLASS
SILICON
FOCUSING
ELECTRODE
VACUUM
PHOTOCATHODE
ANODE
ANODE
Micro PMT works on the same vacuum tube
technology and principle as conventional PMTs
and so can deliver the same performance as
conventional PMT yet in a compact and lightweight unit.
DIRECTION
OF LIGHT
PHOTOCATHODE
LAST DYNODE
PHOTOELECTRON
ELECTRON MULTIPLIER (DYNODES)
GLASS
ELECTRON MULTIPLIER (DYNODES)
[TOP VIEW]
[SECTIONAL VIEW]
What is a PMT
(photomultiplier tube)?
The PMT is a photosensor delivering superb high sensitivity and response speed compared with other types of photosensors. The PMT makes use of the secondary emission
effect for electron multiplication and so achieves extremely high sensitivity and low noise
compared to other photosensors currently in use to measure UV light, visible light, and
near-infrared light. These features allow the PMT to be used in a broad range of applications including high-performance medical equipment and environmental monitors, etc.
Medical care
Measurement
Medical diagnosis in the home or at the bedside
Making environmental pollution measurements
on an individual or regional scale
Bringing high-tech closer to the patient
via compact and portable medical devices
Measurements under various environments
and any type of location
Tests and inspections normally held in examination
rooms or labs can now be made in emergency rooms
or small clinics by using the advantages offered by Micro PMT. Performing sophisticated exams in the home
could also allow detecting major diseases while still in
their early stage. This means the Micro PMT could
prove ideal not only for early stage disease diagnosis
but also daily health care management.
Micro PMT also proves ideal as a photosensor for environmental monitoring tasks. Environmental problems including abnormal weather phenomenon and wide-scale
natural disasters are recently occurring at places all
around the world. If compact measurement devices
were readily available, then environmental phenomena
could be quickly detected at diverse locations to keep
damage and losses to a be minimum.
PRODUCT CONFIGURATION
● MICRO PMT ASSEMBLY
Type No.
MICRO PMT
+
VOLTAGE DIVIDER CIRCUIT
Spectral response
H12400-00-01
300 nm to 650 nm
H12400-01-01
300 nm to 850 nm
compact type
* Suitable high voltage power supply is detailed in last page.
● MICRO PMT MODULES
Type No.
MICRO PMT
+
VOLTAGE DIVIDER CIRCUIT
+
HIGH-VOLTAGE
POWER SUPPLY CIRCUIT
Spectral response
H12402
300 nm to 650 nm
H12402-01
300 nm to 850 nm
flat type
Type No.
Spectral response
H12403
300 nm to 650 nm
H12403-01
300 nm to 850 nm
vertical type
● MICRO PMT PHOTON COUNTING HEAD
MICRO PMT
+
VOLTAGE DIVIDER CIRCUIT
+
HIGH-VOLTAGE
POWER SUPPLY CIRCUIT
+
PHOTON COUNTING CIRCUIT
Type No.
flat type
Spectral response
H12406
300 nm to 650 nm
H12406-01
300 nm to 850 nm
The H12400 series is a high sensitivity
photosensor that combines a Micro PMT
with a voltage divider circuit. The H12400
series can be installed even in narrow
spaces due to its small size.
MICRO PMT ASSEMBLY
H12400 SERIES
■ SPECIFICATIONS
(at +25 °C)
Parameter
Spectral response
Peak sensitivity wavelength
Material
Photocathode
Effective area
Window material
Dynode number of stages
Supply voltage Between anode and cathode
Maximum
Divider current
ratings
Average output signal current
Min.
Luminous sensitivity
Typ.
Cathode
Blue sensitivity index
Typ.
Red / White ratio
Typ.
Radiant sensitivity 1
Typ.
Min.
Luminous sensitivity
Typ.
Typ.
Radiant sensitivity 1
Anode 2
Typ.
Dark current 3
Max.
Typ.
Rise time
Typ.
Time response Transit time
Typ.
T.T.S. 4
Typ.
Gain 2
Operating ambient temperature
Storage temperature
Weight
H12400-00-01
300 to 650
H12400-01-01
300 to 850
Unit
nm
nm
—
mm
—
—
V
µA
µA
420
Multialkali
3(X) × 1(Y)
Borosilicate glass
12
-1150
126
5
100
50
200
80
—
8.0
0.2
—
62
80
15
30
70
160
2.1 × 104
1.6 × 105
0.3
3
1.2
8.0
1.3
2 × 106
3.5 × 105
+5 to +50
-20 to +50
11
Bialkali
µA/lm
—
—
mA/W
A/lm
A/W
nA
ns
—
°C
°C
g
1Measured at the peak sensitivity wavelength
2Supply Voltage: -900 V
3After 30 minutes storage in darkness
4T.T.S.=Transit Time Spread (FWHM)
■ SPECTRAL RESPONSE
107
MULTIALKALI
PHOTOCATHODE
TPMHB0885EA
A
BIALKALI
PHOTOCATHODE
106
10
105
1
GAIN
CATHODE RADIANT SENSITIVITY (mA/W)
QUANTUM EFFICIENCY (%)
100
■ GAIN
TPMHB0884EA
BIALKALI
PHOTOCATHODE
MULTIALKALI
PHOTOCATHODE
104
0.1
103
CATHODE RADIANT
SENSITIVITY
QUANTUM EFFICIENCY
0
200
300
400
500
600
700
800
WAVELENGTH (nm)
900
1000
102
0.5
-500
0.6
-600
0.7
-700
0.8
-800
0.9
1.0 1.1
-900 -1000 -1100
CONTROL VOLTAGE (V)*
SUPPLY VOLTAGE (V)
* Control voltage of a Micro PMT module.
The H12402/H12403 series are high
sensitivity photosensor modules that
contain a Micro PMT, a voltage divider
circuit, and a high-voltage power
supply circuit. These modules can be
easily operated with a low voltage
supply.
MICRO PMT MODULE
H12402/H12403
SERIES
▲Left: H12403 series
Right: H12402 series
■ PRODUCT VARIATIONS
Type No.
H12402 / H12403
H12402-01 / H12403-01
Spectral response
Photocathode material
Features
300 nm to 650 nm
300 nm to 850 nm
Bialkali
Multialkali
for visible range
for visible to near IR range
■ SPECIFICATIONS
(at +25 °C)
Parameter
Input voltage
Maximum input voltage
Maximum input current 1
Maximum average output signal current 2
Maximum control voltage
Recommended control voltage adjustment range
Control voltage input impedance
Effective area
Peak sensitivity wavelength
Min.
Typ.
Typ.
Typ.
Typ.
Min.
Typ.
Typ.
Typ.
Max.
Typ.
Typ.
Max.
Max.
Luminous sensitivity
Cathode
Blue sensitivity index
Red / White ratio
Radiant sensitivity 3
Luminous sensitivity
Anode 2
Radiant sensitivity 3
Dark current 4
Time response Rise time
Gain 2
Ripple noise 25 (peak to peak)
Settling time 6
Operating ambient temperature 7
Storage temperature 7
Weight
Typ.
H12402 / H12403
H12402-01 / H12403-01
+4.5 to +5.5
+5.5
20
5
+1.15
+0.5 to +1.1
+0.5 to +1.0
1
3(X) × 1(Y)
420
100
50
200
80
—
8.0
0.2
—
62
80
15
30
70
160
2.1 × 104
1.6 × 105
0.3
3
1.2
2.0 × 106
3.5 × 105
0.3
10
+5 to +50
-20 to +50
42 (H12402 series), 52 (H12403 series)
Unit
V
V
mA
µA
V
V
MΩ
mm
nm
µA/lm
—
—
mA/W
A/lm
A/W
nA
ns
—
mV
s
°C
°C
g
1At +5 V input voltage, +0.9 V control voltage, and output current equal to dark current
2+0.9 V control voltage
3Measured at the peak sensitivity wavelength
4After 30 minutes storage in darkness.
5Cable RG-174/U, Cable length 450 mm, Load resistance=1 MΩ, Load capacitance=22 pF
6The time required for the output to reach a stable level following a change in the control voltage from +1.0 V to + 0.5 V.
7No condensation
■ SENSITIVITY ADJUSTMENT METHOD
VOLTAGE PROGRAMMING
SIGNAL OUTPUT
LOW VOLTAGE INPUT (RED)
GND (BLACK)
Vref OUTPUT (BLUE)
Vcont INPUT (WHITE)
• Adjust the control voltage to adjust
the sensitivity.
• Electrically insulate the reference
voltage output.
POWER SUPPLY
+5 V
GND
+0.5 V to
+1.0 V *1
(No suffix)
GND
*1 Suffix -01: +1.1 V
POWER SUPPLY
MICRO PMT MODULE
SIGNAL OUTPUT
LOW VOLTAGE INPUT (RED)
GND (BLACK)
Vref OUTPUT (BLUE)
Vcont INPUT (WHITE)
+5 V
GND
CW
MICRO PMT MODULE
RESISTANCE PROGRAMMING
MONITOR
POTENTIOMETER (10 KΩ)
• When using a potentiometer, adjust sensitivity while monitoring
the control voltage so it does not exceed +1.15 V.
TPMOC0256EA
Characteristics
■ Dark current
ANODE DARK CURRENT (A)
A small amount of current is output from a photomultiplier
tube even when operated in a completely dark state. This
output current is called the anode dark current, and the
resulting noise is a critical factor in determining the lower
detection limit of photomultiplier tubes. The graph on the
right shows typical dark current of a Micro PMT versus
the supply voltage.
10-8
TPMHB0901EB
10-9
10-10
10-11
10-12
10-13
-400
-500
-600
-800
-1000
-1200
SUPPLY VOLTAGE (V)
■ Output waveform
OUTPUT VOLTAGE (2 mV/div.)
Photomultiplier tubes are photosensors with extremely
high speeds. The figure on the right shows an output waveform example of a Micro PMT operating at an anode-tocathode voltage of -900 V, measured with pulsed light
(pulse width: 70 ps) that is sufficiently shorter than the response time of the PMT. This anode output pulse has a
rise time of 1.2 ns and a fall time of 1.7 ns.
TPMHB0902EA
LOAD RESISTANCE: 50 Ω
SUPPLY VOLTAGE: -900 V
RISE TIME: 1.2 ns
FALL TIME: 1.7 ns
TIME (2 ns/div.)
■ T.T.S. (transit time spread)
SUPPLY VOLTAGE: -900 V
FWHM: 1.3 ns
1000
RELATIVE COUNT
The time interval between the arrival of light at the photocathode and the instant when the anode output pulse
reaches its peak amplitude is called the electron transit
time.
The T.T.S. (transit time spread) indicates the fluctuations
of the electron transit time measured when the photocathode is fully illuminated with single photons, and is defined as the FWHM of the histogram of the fluctuations. A
typical T.T.S. of Micro PMT is 1.3 ns.
TPMHB0903EA
10000
100
10
1
TIME (2 ns/div.)
■ Pulse linearity
TPMHB0906EA
0
DEVIATION (%)
When an intense light pulse enters the photocathode of a
photomultiplier tube, a large current flows in the latter dynode stages and increases the space charge density,
causing current saturation. This causes the anode output
to deviate from the ideal linearity. The figure below is a typical linearity of a Micro PMT versus light pulse, showing a
deviation of approximately 5 % at an anode peak current
of 1 mA.
10
-10
-20
-30
-40
-50
0.01
SUPPLY VOLTAGE: -900 V
PULSE WIDTH: 50 ns
REPETITION: 1 kHz
0.1
1
ANODE PEAK CURRENT (mA)
10
■ Ripple noise
TPMHB0945EA
1 (mV/div.)
The oscillator circuit used in high-voltage power supplies
in photomultiplier tube modules induces noise into the signal input due to oscillation. This induction noise is referred
to as ripple. The ripple can be observed on an oscilloscope along the baseline in a low voltage range by feeding the output signal to the oscilloscope input while no
light is incident on the modules. For example, under conditions where the load resistance is 1 MΩ and the load capacitance is 22 pF, you will see a signal with an output
near 200 µV and a frequency of approximately 220 kHz.
4 (µs/div.)
■ Uniformity
RELATIVE OUTPUT (%)
WAVELENGTH : 400 nm
SUPPLY
: -900 V
VOLTAGE
SPOT DIA.
: 1 mm
80
60
20
0
-2.5
BOTTOM
TOP
LEFT
RIGHT
BOTTOM
(TOP VIEW)
■ Temperature characteristics
TEMPERATURE COEFFICIENT (%/°C)
The anode sensitivity of photomultiplier tubes is affected
by the ambient temperature. Temperature characteristics
for anode sensitivity are wavelength-dependent, and the
temperature coefficient generally fluctuates from a negative value to a positive value near the long wavelength
limit. The figure on the right shows temperature coefficient
data of micro PMT with a bialkali photocathode and multialkali photocathode as a function of wavelength. The temperature coefficient for both photocathodes is approximately -0.3 %/°C at a wavelength around 500 nm.
2.5
ANODE
40
-1.5
-0.5
0.5
1.5
2.5
TOP
POSITION (mm)
X-AXIS
100
RELATIVE OUTPUT (%)
This uniformity is the variation of sensitivity with respect to the incident
light position on the photocathode.
The figure on the right shows an example of anode output measured by
scanning a light spot of 1 mm diameter at 400 nm wavelength over the
photocathode surface of a Micro
PMT at a pitch of 0.1 mm in the X-axis and Y-axis directions. The output indicates relatively good uniformity.
Y-AXIS
100
80
60
ANODE
40
20
0
-2.5
LEFT
-1.5
-0.5
0.5
1.5
2.5
RIGHT
TPMHB0904EB
POSITION (mm)
TPMHB0943EA
SUPPLY VOLTAGE: -900 V
2
1.5
BIALKALI
PHOTOCATHODE
1
0.5
0
-0.5
MULTIALKALI
PHOTOCATHODE
-1
-1.5
300
400
500
600
700
800
900
WAVELENGTH (nm)
■ Magnetic characteristics
TPMHB0905EA
SUPPLY VOLTAGE: -900 V
1.4
RELATIVE OUTPUT (%)
An external magnetic field deviates the photoelectrons
traveling in a photomultiplier tube from their normal trajectories, causing a loss of gain. The extent of the loss of
gain depends on the direction of the magnetic field. The
figure on the right shows how magnetic fields affect the
output of a Micro PMT. It is seen that the magnetic field in
the Z direction most affects the output. Terrestrial magnetism which is less than 0.1 mT will have almost no effect
on the output.
1.6
1.2
X
1
0.8
0.6
0.4
0.2
Y
Z
0
-20
-15
-10
-5
0
5
10
MAGNETIC FLUX DENSITY (mT)
15
20
MICRO PMT
PHOTON COUNTING HEAD
H12406 SERIES
The H12406 series is a photon counting
head that contain a Micro PMT, a highvoltage power supply circuit and a photon
counting circuit.
This photon counting head can be easily
operated with a low voltage supply.
■ SPECIFICATIONS
(at +25 °C)
Parameter
H12406
+4.75 to +5.25
+6
40
3×1
Input voltage
Max. Input voltage
Max. Input current
Effective area
Spectral response
Peak sensitivity wave length
300 to 650
300 to 850
420
1.7 × 105
3.6 × 105
2.6 × 105
4.3 × 104
1.4 × 102
—
300 nm
400 nm
500 nm
600 nm
700 nm
800 nm
Typ.
Count sensitivity
H12406-01
5.0 × 106
Count linearity 1
10
50
Typ.
Max.
Dark count 2
Pulse-pair resolution
Output pulse width
Output pulse height
(at load resistance 50 Ω)
Recommended load resistance
Signal output logic
Excessive light incident
Excessive light
detection output 3 Normally
Operating ambient temperature 4
Storage temperature 4
Weight
2.1 × 105
2.7 × 105
2.3 × 105
1.7 × 105
9.6 × 104
2.1 × 104
Unit
V
V
mA
mm
nm
nm
s-1·pW-1
s-1
100
500
s-1
20
10
+2.0
+2.2
50
Positive logic
+3.5
+0.5
+5 to +50
-20 to +50
46
Min.
Typ.
Min.
Max.
ns
ns
V
Ω
—
V
V
°C
°C
g
1Random pulse, at 10% count loss
2After 30 minute storage in darkness
3Load resistance 10 kΩ
4No condensation
■ COUNT SENSITIVITY
■ BLOCK DIAGRAM
A
106
PMT
COUNT SENSITIVITY (s-1·pW-1)
H12406-01
AMPLIFIER
PULSE
COMPARATOR SHAPER
L.L.D.
HIGH VOLTAGE
POWER SUPPLY CIRCUIT
OUTPUT
POSITIVE
LOGIC
TO
PULSE
COUNTER
RL 50 Ω
105
H12406
GND +5 V
POWER INPUT
OVER LIGHT
DETECTION
OUTPUT
+4.0 V at the over light condition
0 V at the normal condition
104
TPMOC0226EB
103
200
300
400
500
600
700
800
WAVELENGTH (nm)
900
1000
Characteristics
■ Dark count
10000
1000
DARK COUNT (s-1)
Some dark current pulses are generated in a photomultiplier tube during operation even if no light is incident on it.
These dark current pulses are amplified by an amplifier
and then only those dark pulses with a height exceeding a
certain discriminator threshold are output through a pulse
shaper. This output, expressed in counts per second (s-1),
is the dark count and indicates the lower limit of signal detection.
TPHOB0063EA
H12406-01
100
10
H12406
1
0.1
5
10
15
20
25
30
35
40
45
50
TEMPERATURE (°C)
■ Output waveform
Output waveforms are positive logic signals. The figure on
the right shows output waveforms measured with and
without a load resistance of 50 Ω. Since photon counting
head handles high-speed signals, a 50 Ω impedance cable is usually connected between a photon counting head
and external device, and the input impedance of the external device should also preferably be 50 Ω.
OUTPUT PULSE HEIGHT (1 V/div.)
TPHOB0064EA
NO LOAD
10 ns
LOAD
RESISTANCE
50 Ω
10 ns
TIME (4 ns/div.)
■ Count linearity and excessive
light detection characteristics
109
OUTPUT COUNT
COUNT RATE (s-1)
In a random light input event, when the light level increases and exceeds a certain level, the output pulses begin to
overlap each other and the count value is no longer proportional to the light level. As the light level further increases causing more pulses to overlap, the number of
output pulses gradually saturates and then begins to decrease and eventually reaches 0. Count linearity is specified as the count value at which a 10 % loss occurs in the
counted value compared to the theoretical value.
If the incident light level largely exceeds the count linearity,
a signal (4.0 V) is output to indicate an excessive light input.
TPMOB0217EA
1010
107
106
EXCESSIVE LIGHT
DETECTION OUTPUT
105
+4 V
0V
104
103
103
104
105
106
107
108
109
1010
1011
1012
RELATIVE INPUT LIGHT
■ Count rate correction
TPMOB0218EA
20
10
CORRECTED
0
DEVIATION (%)
When the number of pulses measured by photon counting
exceeds 106 s-1, counting errors begin to occur due to
pulse overlap. One method for improving the count linearity utilizes a correction formula to find the approximate values. The graph on the right shows improved count linearity characteristics obtained by using a correction formula
to find the approximate values.
108
-10
-20
MEASURED
-30
-40
-50
-60
Linearity correction formula
N : real count rate (s-1)
M
N=
M : measured count rate (s-1)
1-Mt
t : pulse pair-resolution (s)
* Micro PMT photon counting head H12406 series do not have the function to
automaticlly output a correction value.
-70
-80
103
104
105
106
COUNT RATE (s-1)
107
108
■ DIMENSIONAL OUTLINES (Unit: mm)
MICRO PMT ASSEMBLY
■ H12400 Series
19 ± 0.25
2.2 ± 0.2
4 ± 0.25
DEDICATED ADAPTOR FOR OPTICAL BLOCK
TO MICRO PMT ASSEMBLY *
4 × M2 DEPTH 4
THREADED HOLE
FLEXIBLE
PRINTED
CIRCUIT
14 ± 0.1
8.0
22 ± 0.5
ABS CASE
12
VOLTAGE
DIVIDER
CIRCUIT
15 ± 0.5
10.2
34 ± 0.5
36 ± 2
GND
C1: 1 nF
FLEXIBLE
C2, C3, C4: 22 nF
PRINTED CIRCUIT
R1, R12: 1 MΩ
R2, R11: 680 kΩ
R1 R2 R3 R4 R5 R6 R7 R8 R9 R10 R11 R12 R13
R3 to R10: 470 kΩ
R13: 2 MΩ
-HV
GND
INPUT
WINDOW
SMA
CONNECTOR
GND
C2 C3 C4
GND
18.6 ± 0.1
4.3 ± 0.2
13 ± 0.1
P
SIGNAL OUTPUT
: SMA CONNECTOR
C1
A
COAXIAL CABLE
180 ± 10
8 ± 0.5
Dy1 Dy2 Dy3 Dy4 Dy5 Dy6 Dy7 Dy8 Dy9 Dy10 Dy11 Dy12
K
7.2 ± 0.25
17 ± 0.25
5.5 ± 0.2
21 ± 0.25
4 × M1.4 DEPTH 1.5
MOUNTED
THREADED HOLE
6 ± 0.5
-HV AWG26 PURPLE 500 ± 10
14 ± 0.1
3 ± 0.2
22 ± 0.5
4.8 ± 0.2
MICRO PMT ASSEMBLY
GND 0.2SQ BLACK 500 ± 10
* Dedicated Adaptor for optical block is supplied.
TPMHA0590EB
MICRO PMT MODULE
MICRO PMT MODULE
■ H12402 Series
■ H12403 Series
38 ± 0.35
15 ± 0.25
38 ± 0.35
A
13 ± 0.1
26 ± 0.1
450 ± 20
13 ± 0.1
A
INPUT
WINDOW
30 ± 0.25
34 ± 0.35
11 ± 0.1
2 × M1.4
DEPTH 1.5
2
12.5 ± 0.25
450 ± 20
34 ± 0.1
34 ± 0.1
2
PHOTOCATHODE
(3 × 1 MIN.)
CABLE
INPUT
WINDOW
CABLE
4 × M2 DEPTH 4
MOUNTED
THREADED HOLE
4 × M2 DEPTH 4
MOUNTED THREADED HOLE
12 ± 0.25
PHOTOCATHODE (3 × 1 MIN.)
●CABLE
LOW VOLTAGE INPUT (+5 V) : AWG26 (RED)
: AWG26 (BLACK)
GND
: AWG26 (BLUE)
Vref OUTPUT (+1.2 V)
: AWG26 (WHITE)
Vcont INPUT
: RG-174/U
SIGNAL OUTPUT
●CABLE
LOW VOLTAGE INPUT (+5 V) : AWG26 (RED)
: AWG26 (BLACK)
GND
: AWG26 (BLUE)
Vref OUTPUT (+1.2 V)
: AWG26 (WHITE)
Vcont INPUT
: RG-174/U
SIGNAL OUTPUT
Weight: 52 g
TPMOA0084EC
Weight: 42 g
TPMOA0083EC
MICRO PMT PHOTON COUNTING HEAD
■ DETAILS OF INPUT WINDOW
■ H12406 Series
34 ± 0.1
2
2 × M1.4
DEPTH 1.5
4
EFFECTIVE AREA
3 × 1 MIN.
INPUT
WINDOW
A
13 ± 0.1
26 ± 0.1
12.5 ± 0.25
30 ± 0.25
450 ± 20
1.4
38 ± 0.35
■ A CROSS SECTION
MICRO PMT
CABLE
4 × M2 DEPTH 4
MOUNTED
THREADED HOLE
PHOTOCATHODE
C0.3
15 ± 0.25
PHOTOCATHODE (3 × 1 MIN.)
INPUT
WINDOW
RESIN
PACKAGE
●CABLE
: AWG26 (RED)
LOW VOLTAGE INPUT (+5 V)
: AWG26 (BLACK)
GND
OVER LIGHT DETECTION OUTPUT: AWG26 (BLUE)
: RG-174/U
SIGNAL OUTPUT
0.5
0.5
Weight: 46 g
TPMHA0590EB
TPMOA0091EB
■ OPTION (sold separately)
GASKET
4 × 2.2
(FOR M2 SCREW FIXING *)
30
* Supplied with M2 screws (4 pcs)
for fixing to model.
5.0 - 0.5
+0
1.5
GASKET
4 × 2.2
(FOR M2 SCREW FIXING *)
* Supplied with M2 screws (4 pcs)
for fixing to model.
12.5 ± 0.1
12.5 ± 0.1
34 ± 0.1
+0
4.9 - 0.5
TACCA0339EA
2.6
2
10.7
4 × 2.2
(FOR M2 SCREW FIXING *)
* Supplied with M2 screws (4 pcs)
for fixing to model.
GASKET
Weight: 12 g
+0
5.0 - 0.5
13.0 ± 0.1
3.5
11.0 ± 0.1
38
13.0 ± 0.1
● E13564 (SMA type)
15
34.0 ± 0.1
38
GASKET
34.0 ± 0.1
1.5
2
5.5
Weight: 15 g
38
TACCA0338EA
● E13563 (FC type)
3.5
34 ± 0.1
2
Weight: 17 g
38
1.5
2
3.5
10.7
2.6
3.5
1.5
26 ± 0.1
5.5
+0
4.9 - 0.5
● E13562 (SMA type)
26 ± 0.1
30
3.5
3.5
● E13561 (FC type)
15
11.0 ± 0.1
4 × 2.2
(FOR M2 SCREW FIXING *)
* Supplied with M2 screws (4 pcs)
for fixing to model.
Weight: 10 g
* E13561 and E13562 are the exclusive options for H12402/H12406 series. E13563 and E13564 are the exclusive options for H12403 series.
Related
Products
■ HIGH VOLTAGE POWER SUPPLY C10940 SERIES 0.7 W output 1200 V / 0.6 mA
The C10940 series is a high voltage power supply module developed for compact size and high performance.
This is designed to mount on a printed circuit making them ideal for use with a H12400 series Micro PMT assembly. Besides high performance and low power consumption, a variety of protective functions are also included.
Protective Functions: Units protected against reversed power input, reversed / excessive controlling voltage input,
continuous over loading / short circuit output
Parameter
Input Voltage
Typ.
Input Current 1
Output Voltage
Max.
Output Current
Ripple / Noise (p-p) 12
Typ.
Operating Ambient Temperature 12 / Humidity 3
Storage Temperature / Humidity 3
Weight
Typ.
Dimensions (W × H × D)
1: At maximum output voltage
* -R2 type: RS-485 control
2: At maximum output current
C10940-03
C10940-03-R2*
C10940-53
C10940-53-R2*
+5 ± 0.5
60 (no load), 230 (full load)
-10 to -1200
+10 to +1200
0.6
50
0 °C to +50 °C / Below 80 %
-20 °C to +60 °C / Below 80 %
8.5
15 × 18 × 15
Unit
V
mA
V
mA
mV
—
—
g
mm
3: No condensation
■ POWER SUPPLY FOR PMT MODULE C10709
The C10709 is a power supply unit designed to operate a PMT module. This unit supplies both drive
voltage and control voltage, making it ideal for operating the H12402 series and H12403 series Micro
PMT modules.
▲C10709
■ AMPLIFIER UNITS
These amplifier units convert the signal current input from a photomultiplier tube into a voltage output.
Please select the desired type with a frequency range and current-to-voltage conversion factor that
match your applications.
▲ (Rear) C7319, C9663, C6438
(Front) C11184, C5594-44
■ PHOTON COUNTING CONFIGURATION EXAMPLE
▲Micro PMT assembly
H12400 series
USB
▲Photon Counting Unit C9744
▲Counting Unit C8855-01
▲Micro PMT modules
H12402, H12403 series
PC
▲Micro PMT photon counting head
H12406 series
*
is the registered trademark of Hamamatsu Photonics K.K. in Japan, U.S.A., and EU.
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. ©2016 Hamamatsu Photonics K.K.
HAMAMATSU PHOTONICS K.K.
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, 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)1707-294888, Fax: (44)1707-325777 E-mail: [email protected]
North Europe: Hamamatsu Photonics Norden AB: Torshamnsgatan 35 SE-164 40 Kista, Sweden, Telephone: (46)8-509-031-00, Fax: (46)8-509-031-01 E-mail: [email protected]
TPMZ1019E02
Italy: Hamamatsu Photonics Italia S.r.l.: Strada della Moia, 1 int. 6, 20020 Arese (Milano), Italy, Telephone: (39)02-93581733, Fax: (39)02-93581741 E-mail: [email protected]
China: Hamamatsu Photonics (China) Co., Ltd.: B1201 Jiaming Center, No.27 Dongsanhuan Beilu, Chaoyang District, Beijing 100020, China, Telephone: (86)10-6586-6006, Fax: (86)10-6586-2866 E-mail: [email protected]
JAN. 2016 IP