PHOTONIC DEVICES 2020Electron Tube Devices and Applied Products

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Photonic Devices 2020Electron Tube Devices and Applied

Electron tube devices, developed by harnessing technologies accumulated over long periods of time and involved in cutting-edge scientific research, are key devices for measuring the unobservable and capturing the undetectable. Our electron tube devices are still evolving, via the use of new technologies, into more compact, lightweight, sophisticated and versatile products optimized for specific uses and environments, and their evolution expands the application fields of the equipment where they are installed.Hamamatsu Photonics provides a wide range of electron tube devices that play active roles in a diverse array of fields including medical care, spectroscopy and analysis, semiconductor industry, biotechnology, and academic and scientific research. This brochure introduces innovative electron tube devices that we have newly designed and manufactured to push their performance even further.

■Mass Spectrometry (MS) ..................................................●MCP Assembly MIGHTION® F14845-11●MCP Assembly F14844●Ceramic Channel Electron Multiplier CERARION® R14747-80●Dual Mode Ion Detector●Ionization-Assisting Substrates DIUTHAME® A13331-18-2B, A13331-5019-1B

■Printing .............................................................................. ●Low-Energy Electron Beam Source EB-ENGINE - Long Type●Linear Irradiation Type UV-LED Unit LIGHTNINGCURE® LC-L5G GH-103A●Linear Irradiation Type UV-LED Unit LIGHTNINGCURE® LC-L5G GC-113A●Linear Irradiation Type UV-LED Unit LIGHTNINGCURE® LC-L5G GD-390●Linear Irradiation Type UV-LED Unit LIGHTNINGCURE® LC-L5G GB-360●UV-LED Spot Light Source LIGHTNINGCURE® LC-L1V5

■High Energy Physics Research ....................................... ●Photomultiplier Tubes R14374, R14689●Photomultiplier Tube R15458

■Laser Microscopy ...............................................................●Photosensor Modules (GaAsP Photocathode) - Wide Dynamic Range Type●Photosensor Module (GaAsP Photocathode) H12056-40●Photosensor Module (GaAsP Photocathode) H15460-40●Compact Photosensor Modules (InP/InGaAsP Photocathode) H15620-25 / -45

■Micro PMT ...........................................................................●Surface-Mount Package Micro PMT R12900U Series●Micro PMT Module H14066 Series●Surface-Mount Package Micro PMT R15320U Series●Micro PMT Arrays H15690-014, H15691-018

■TO-8 Package Photomultiplier Tubes ................................●Metal Package Photomultiplier Tube R14755U-100●Metal Package Photomultiplier Tube R9880U-09

■Photomultiplier Tube Modules ................................................... ●Linear-Array Multianode Photomultiplier Tube Module H15441-20●Photosensor Modules H14447, H14990●Photosensor Modules H14601, H14950, H14953●Photosensor Module H14768●Photon Counting Head H14870●Wide Dynamic Range Photomultiplier Tube Module H13126-01

■Infrared (IR) Light Sources ......................................................... ●Supercontinuum Light Source L15077●IR Graphene Light Source

Broad Infrared Spectrum Xenon Flash Lamp

■Imaging Devices .............................................................................. ●180 kV Microfocus X-Ray Source L14351-02●Soft X-Ray Source L11754-01●Compact X-Ray CMOS Camera Digital X-CUBE●High-Count-Rate Neutron Detector Unit●High-Speed Gated Image Intensifier Unit C14245 Series

■Static Charge Removers ..............................................................●VUV Ionizers L12542, L15094●PhotoIonizers L14471, C14472, C14546

■High-Voltage Power Supply Modules ..................................... ●High-Voltage Power Supply Module C14051-55●High-Voltage Power Supply Module C14921-01

●NEW ●Devlp. ●Technology

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TOF-MS

MIGHTION is an ion detector using a combination of MCP (microchannel p la te ) and semiconducto r AD (avalanche diode). It features fast time response, high output linearity, and long life. MIGHTION also has a large effective area (27 mm dia.) ideal for TOF-MS (time-of-flight mass spectrometry).

MCP Assembly F14844

Miniature MS

The F14844 MCP assembly has a unique triode structure that suppresses ion feedback noise to ensure stable operation in high pressure (low vacuum) environments. The F14844 is an innovative ion detector that can be mounted in compact desktop mass spectrom-eters where installing large vacuum pumping systems is difficult or impractical.

Ceramic Channel Electron Multiplier CERARION® R14747-80

Q-MS (Quadrupole MS)

CERARION is a lead-free channel electron multiplier that employs a ceramic structure with high design flexibility and robustness. The shape and the number of channels can be customized to meet user equipment specifica-tions. When mounted with a conversion dynode, CERARION can measure ions of both polarities by changing the polarity of the voltage applied to the conversion dynode.

Ion detector capable of operating at high pressure (low vacuum) and high gain: 106 at 1 Pa

Mass Spectrometry (MS)Mass spectrometry (MS) can identify and quantify a substance by ionizing the atoms and molecules of the substance and measuring the mass and number of ions. It is a well-known and effective analytical technique and research tool.We contribute to progress in the mass spectrometry field by developing advanced ion detection devices in addition to supplying MCP and electron multipliers.

Ion detector with fast time response, high output linearity, and long service life

MCP Assembly MIGHTION® F14845-11 NEW

NEW

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MCP-in: -6 kVMCP: 600 VAD: -350 V

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MCP-in: -6 kVMCP: 600 VAD: -350 V

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VACUUM LEVEL (Pa)

F14844Conventional type

MCP gain: 105

Lead-free ion detector customizable to meet user equipment specifications

4

Output waveform (Typ.) Pulse linearity (Typ.)

Output waveform (Typ.)

5

Dual Mode Ion Detector

Measurement example

●Measurement step

This is a new type of ion detector using a combination of electron multiplier and semiconductor AD (avalanche diode). Compared to the conventional type (R13733), this detector delivers a wider dy-namic range and longer service life achieved through improving the time response characteris-tics of counting signals.

Ionization-Assisting Substrates DIUTHAME®

A13331-18-2B, A13331-5019-1B

MALDI TOF-MS Imaging

DIUTHAME is an ionization-assisting tool that promotes ionization in place of the matrix used for MALDI. DIUTHAME works just by placing it on a sample before measurement. Since the A13331 series DIUTHAME is newly designed for use with the blotting technique, it can make imaging measurements that retain position infor-mation by transferring the components on the sample surface to the DIUTHAME substrate. There is no need to slice the samples, so DIUTHAME applications will now extend into fields where it could not be used up until now due to sample shapes and measurement methods.

A new type of ion detector that delivers a wide dynamic range and long service life

New measurement support tools optimized for blotting technique

2 3 41

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ICP-MS (Inductively Coupled Plasma MS)

Cut a fresh strawberry in half Start measurementPlace DIUTHAME for blotting Wait until dry

A13331-18-2B

Target

Laser pitch

Choline [M+H]+

Spectrum number 3 4 521

Hexose [M+K]+ Citric acid [M+K]+ Peralgonidin [M]+ Sucrose [M+K]+

300 μm 300 μm 300 μm 300 μm 300 μm

Mass spectrum

Ion image

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●Measurement data

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)Dual mode ion detector counting signalConventional type (R13733) counting signalDual mode ion detector analog signal

Output waveform (Typ.)

Technology

NEW

A13331-5019-1B

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Dual mode ion detector-HV: -1800 VAD: 4000 VGate: 300 VConventional type (R13733)-HV: -1800 V+HV: 1000 VGate: 230 V

FWHM: 9 ns

FWHM: 3.5 ns

Dynamic range (Typ.)

Low-Energy Electron Beam Source EB-ENGINE - Long Type

EB Printing

This EB-ENGINE is a low-energy electron beam source that is well-suited for high-speed paper transport requiring instant drying of radical polymerization ink such as EB ink. It has a wide effective processing span of 450 mm or 650 mm and emits high-density, low-energy electron beams that ensure streamlined, high-speed EB printing. The EB-ENGINE also offers advantages that help reduce equipment size and weight, simplifies shielding enclosures and cuts the total cost, making it easier to install and use.

Linear Irradiation Type UV-LED Unit LIGHTNINGCURE® LC-L5G

GH-103A

UV Printing

The LC-L5G series is a family of UV-LED light sources that instantly dry UV ink used for ink-jet printers, flexographic printers, and screen printers. To meet user needs, Hamamatsu offers a wide lineup of products that can be customized in size, output power, lighting method (partial lighting, etc.), cooling method, and communication method.

By taking advantage of our unique optical technology and cooling technology, we are developing UV-LED light sources that achieve even higher output power than ever before. This light source will prove ideal for printing ink and printer transport speeds that could not be handled until now.

PrintingFor the printing industry where there are ever-increasing demands for higher speed, higher quality, and higher added values, Hamamatsu Photonics offers products for EB and UV printing that were developed with photonics technology.

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Features

■Difference between low-energy and conventional

Low-energy electron beams Conventional electron beams(Medium- to high-energy electron beams)

Energy is applied only to the surfaceand thin film

Material may be damaged internally

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Accelerating voltage50 kV70 kV100 kV150 kV200 kV300 kV

Model with greatly improved processing capacity and compatible with high-speed paper transport

●Enhanced processing effect on surfaces and thin films (low accelerating voltage: 50 kV to 100 kV)

●High processing capability: 30 kGy at a rate of 100 m/min

●Wide effective processing span: 450 mm or 650 mm●Compact and lightweight●Easy maintenance

●High output power: 24 W/cm2

●Capable of segment lighting●RS-485 communication ●Supports multi-unit operation

High-end model with industry’s highest output power (air-cooled 24 W/cm2) in its class

Amount of imparted energy and penetration depth of electron beam

Features

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GC-113A

This UV-LED light source delivers high output power, enough to allow high-speed paper transport and effective pinning of white ink. Using the RS-485 communication also improves the versatility and ease of use.

GD-390

This light source is designed to have the same shape as a typical metal halide lamp and so serves as a direct replacement without needing any additional equipment.

GB-360

This UV-LED light source provides highly uniform irradiation patterns that prevent printing irregularities.

The LC-L1V5 is a UV-LED spot light source that emits deep UV light at a wavelength of 280 nm. Using deep UV light along with UV light improves the surface curability of ink. The LC-L1V5 can also be used for development (evaluation and testing) of inks. When an optical system such as a condenser lens is mounted, it will emit deep UV light in a wide variety of irradiation patterns. Please feel free to contact us for further information and requests.

Prin

ting

High-power pinning model capable of segment lighting

High-uniformity model design to minimize irradiation non-uniformities

Deep UV model expected to open new applications

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Devlp.UV-LED Spot Light Source LIGHTNINGCURE® LC-L1V5

Model name Light emitting window size

GH-103A

GC-113A

GD-390

GB-360

Forced-air cooling by fan

Forced-air cooling by fan

Forced-air cooling via suction ducts

Forced-air cooling by fan

NOTE:

103 mm × 24 mm

113 mm × 16 mm

390 mm × 20 mm

300 mm × 20 mm

Wavelength

395 nm

365 nm

385 nm

395 nm

385 nm

385 nm

UV irradiance Cooling method

24 W/cm2 1

8 W/cm2 1

10 W/cm2 1

18 W/cm2 1

7 W/cm2 2

1 Maximum UV irradiance within the area irradiated by the light source positioned at a distance of 0 mm from the irradiated area.2 Maximum UV irradiance within the area irradiated by the light source positioned at a distance of 5 mm from the irradiated area.

Duct-suction forced-air cooling model designed for improved compatibility with metal halide lamps

Specifications

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Features●High output power: 10 W/cm2

●Capable of segment lighting●RS-485 communication ●Supports multi-unit operation

Features●High compatibility with metal halide lamps●Forced-air cooling via suction ducts●High output power: 18 W/cm2

●Capable of segment lighting●RS-485 communication

Features●High output power: 7 W/cm2

●Highly uniform irradiation: Within ±4 %●Capable of segment lighting

Photomultiplier Tubes R14374, R14689

The R14374 and R14689 are small-diameter hemispherical photomultiplier tubes with high gain designed for use with the next generation neutrino telescope KM3NeT. Compared to the conventional hemispherical photomultiplier tube (R12199), the R14374 and R14689 exhibit higher time resolution that gives more accurate neutrino observa-tion. Despite their small diameter, they offer a large field-of-view angle and also minimize the so-called dead space when installed.

High Energy Physics ResearchHamamatsu photomultiplier tubes are widely used for cutting-edge high energy physics research being con-ducted by scientists around the world such as at SuperKamiokande in Japan. We are pursuing the ulti-mate in photomultiplier tube performance by working to develop new technologies to optimize our products to serve as ideal matches for various experiments.

3-inch and 3.5-inch diameter hemispherical photomultiplier tubes with high gain and high time resolution

500 1000600 800 1200700 900 1500

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Transit time spread (FWHM) (Typ.)

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Features●High gain: 1.0 × 107 (typ.)●High time resolution: Transit time spread (FWHM) R14374: 1.3 ns (typ.)

R14689: 1.5 ns (typ.)

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Supply voltage: 1250 V

Courtesy of Edward Berbee / Nikhef Courtesy of the KM3NeT Collaboration

Next generation neutrino telescope KM3NeT

DOM (Digital Optical Module)

In the depths of the Mediterranean Sea, a total of 6210 DOMs (Digital Optical Modules) will be installed, each of which incorporates photomultiplier tubes, operating circuits, and readout circuits. These modules are for use in ORCA (Oscillation Research with Cosmics in the Abyss) that will be conducted off the coast of Marseille, France for observation of low-energy neutrinos and are also for use in ARCA (Astroparticle Research with Cosmics in the Abyss) that will be conducted off the coast of Sicily, Italy for observation of high-energy neutrinos.

Gain (Typ.)

115 mm108 mm

R15458 Conventional type(R12199)

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Photomultiplier Tube R15458

The R15458 is a small-diameter hemispherical photomultiplier tube with high gain designed for use with the 12-country collaboration project IceCube Neutrino Observatory. Compared to the conventional hemispherical photomultiplier tube (R12199), the R15458 is designed with a shorter overall length that helps reduce the size of the detection unit called the mDOM (multi-PMT Digital Optical Module).

3-inch diameter, low-profile hemispherical photomultiplier tube with high gain

NEW

Features●High gain: 1.0 × 107 (typ.)●Low profile

IceCube neutrino observatory

mDOM (multi-PMT Digital Optical Module)

At a depth of 1500 to 2500 meters in the Antarctic ice, a total of 5160 DOMs (Digital Optical Modules) were installed, each of which incorporates photomultiplier tubes, operating circuits, and readout circuits. One cubic kilometer of Antarctic ice is used for neutrino detection. At present, an upgrade plan for the IceCube experiment is underway to add new 700 photodetectors to the currently used 5160 DOMs. More than half of those new photodetectors will be mDOM equipped with R15458.

Courtesy of the IceCube Collaboration Courtesy of IKP, U Münster / A. Kappes

Bedrock

Top View

IceCubeDeepCoreUpgrade

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Gain (Typ.)

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Multialkali photocathode (suffix: -20)GaAsP photocathode (suffix: -40)Extended red GaAsP photocathode (suffix: -42)GaAs photocathode (suffix: -50)InGaAs photocathode (suffix: -61)

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Photosensor Modules (GaAsP Photocathode) - Wide Dynamic Range Type

These photosensor modules use a GaAsP photo-cathode photomultiplier tube. These achieve a wide dynamic range with a maximum output current of 40 µA providing clear images with sharp contrast and also ensuring stable operation without needing a protection circuit.

Laser MicroscopyIn confocal laser microscopes and multiphoton exci-tation microscopes for laser microscopy, our photo-sensor modules that incorporate a photomultiplier tube or HPD (hybrid photo-detector) are becoming more and more widely used as detectors for captur-ing fluorescence and scattered light from the sample.

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Easy-to-use photomultiplier tube modules with a wide dynamic range

Spectral response (Typ.)

For Better Image Contrast Without Protection Circuit

800 1000 1200 1400900 1100 1300 1500 16000.01

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InP/InGaAsP photocathode (suffix: -25)InP/InGaAsP photocathode (suffix: -45)

400 500 600 700 800 900 10000

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InGaAs photocathode (suffix: -61)InGaAs photocathode (target specification)

To keep up with increasing demands for single-molecule fluorescence imaging, we are continuing to improve our compound-semiconductor photocathode technology to further boost photomultiplier tube sensitivity.Besides developing GaAsP photocathodes useful for measurement in the visible light region such as for GFP (green fluorescence protein), we are also developing photomultiplier tubes with an extended red GaAsP pho-tocathode, GaAs photocathode, InGaAs photocathode, and InP/InGaAsP photocathode that have high sensitiv-ity in longer wavelength regions.

Conventional type(H7422 / H10770A series, etc.)

Maximum averageanode output current

Development

40 µA

2 µA

20 times

Photosensor Module (GaAsP Photocathode) H12056-40

The H12056-40 is a photosensor module using a GaAsP photocathode photomultiplier tube. It includes a gate function of 1 ms to DC which is ideal for laser microscopes and protects the photomultiplier tube electronically from excessive light such as fluctuating background light that might enter the unit when changing the sample.

Photosensor Module (GaAsP Photocathode) H15460-40

The H15460-40 photosensor module employs a GaAsP photocathode photomultiplier tube. The photosensitive area is 14 mm square making it ideal for multiphoton excitation microscopes. The H15460-40 also includes an amplifier with a fre-quency band of 30 MHz and a current-to-voltage conversion factor of 0.02 V/µA.

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Gate timing chart (Typ.)

Miniature size photomultiplier tube module with gate function from 1 ms to DC

Photomultiplier tube module with a large photosensitive area and built-in high-frequency band amplifier

Compact Photosensor Modules (InP/InGaAsP Photocathode) H15620-25 / -45

The H15620-25 and H15620-45 photosen-sor modules employ an InP/InGaAsP pho-tocathode photomultiplier tube. Compared to the conventional type (H10330C series), these photosensor modules are designed to be compact making them easier to in-stall in laser microscopes.

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Compact, easy-to-install photomultiplier tube modules

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Gate signal input

OUTPUT

OFF

(+2 V to +5 V at 10 kΩ)

ON

1 ms to DC

Delay time: 0.6 ms

90 %

50 %

10 %

Delay time: 0.1 ms

Rise time: 0.3 msFall time: 0.1 ms

Output 100 % / 10 %: 0.7 ms

Output 100 % / 0 %: 1 ms

Output 0 % / 90 %: 1 ms

Output 0 % / 100 %: 3 ms

H15460-40 Conventional type

Effective area

14 mm Effective area 5 mm

Gate Function for Optogenetics

10× Larger Area for 2-Photon Microscopy

For NIR Detection

H15620-25 / -45 Conventional type(H10330C series)

Main unit: (W) 100 mm × (H) 198 mm × (D) 150 mmController unit: (W) 102 mm × (H) 143 mm × (D) 279.5 mm

(W) 120 mm × (H) 60 mm × (D) 60 mm(except for heatsink and fan)

-500 -1150-1000-900-800-700-6000.5 1.151.00.90.80.70.6

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* Control voltage of a micro PMT module.

Bialkali photocathodeMultialkali photocathodeExtended redmultialkali photocathode

200 3000.01

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400 500 600

WAVELENGTH (nm)

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Cathode radiant sensitivityQuantum efficiency

Bialkali photocathodeMultialkali photocathodeExtended redmultialkali photocathode

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Micro PMT

Surface-Mount Package Micro PMT R12900U Series

The world’s smallest photomultiplier tubes sealed in a subminiature package that increases design flexibility

Micro PMT is the world’ s smallest, thinnest and lightest photomultiplier tube developed by taking advantage of our unique advanced technologies in MEMS (Micro-Electro-Mechanical Systems), semiconductor manufacturing, electron trajectory design, vacuum-sealed packaging and vacuum process-ing. Micro PMT is a promising device with a highly diverse range of applica-tions since it provides high sensitivity and fast time response and allows reducing the equipment size while maintaining good performance.

The R12900U series is a micro PMT encapsulated in a plastic package designed for easy mounting by the user onto electronic circuit boards. To meet increasing demands for more portable equipment, the R12900U series offers great features including a smaller size, thinner profile, lighter weight and easier installation. These features allow creating a free and flexible design during equipment development.

Gain (Typ.)

Micro PMT sealed in a small, thin and light package for easy mounting on circuit boards

Spectral response (Typ.)

14 mm

14 mm

NEW

Micro PMT Module H14066 Series

The H14066 series is the world’s smallest micro PMT module that integrates a micro PMT with a voltage-divider circuit and a high-voltage power supply circuit. The H14066 series incorporates an R12900U series surface-mount package micro PMT. Com-pared with our currently available micro PMT module (H12402), the H14066 series is down-sized about 50% in volume, helping the design of more portable equipment. It also easily operates from a low voltage supply that makes it quick and easy to start using.

The world’s smallest photomultiplier tube module that easily operates from a simple low voltage supply

NEW

ncreases design flexibility

and lightest photomultiplier tube que advanced technologies in

semiconductor manufacturing,ackaging and vacuum process-highly diverse range of applica-ast time response and allows g good performance.

signed for easy mounting by the userable equipment, the R12900U series and easier installation. These features

easy mounting on circuit

NEW

easily operates from a

NEW

H14066Conventional type(H12402)

50 % volume reduction

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Array devices enabling multi-channel measurement

15 mm

8.6 mm

Micro PMT Arrays H15690-014, H15691-018

The H15690-014 and H15691-018 are 4-channel and 8-channel micro PMT arrays using the R15320U series surface-mount package micro PMTs, which are arrayed in parallel at a center-to-center spacing of 9 mm. These micro PMT arrays allow multi-channel s imul taneous measurement and mult i -wavelength measurement with no crosstalk since each channel is fully separated. The number of channels and other specs can be customized to match user needs. We are also developing micro PMT arrays with an optical system so please consult us if interested.

Photomultiplier tube modules capable of multi-channel measurement and multi-wavelength detection

Surface-Mount Package Micro PMT R15320U Series

The R15320U series is a micro PMT encapsulated in a plastic package designed for easy mounting by the user onto electronic circuit boards. The package size is further reduced to 8.6 mm × 15 mm. Two or more micro PMTs can be arrayed in parallel to allow equipment downsizing and also to meet demands for multi-functional use such as simultaneous analysis of multiple samples with just a single piece of equipment.

Photomultiplier tube designed even smaller to allow a parallel array configuration

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A photocathode with the spectral response characteristics you need can be selected for each channel.The gain of each channel can be adjusted independently (wide gain adjustment range).

Back: H15690-014, Front: H15691-018

Applications●Environmental analysis●Specimen test (POCT: point-of-care testing)●Various portable devices

Example of micro PMT array with optical system (3-wavelength detector)

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Micro PMT Arrays H15690-014, H15691-018

The H15690-014 and H15691-018 are

Photomultiplier tube modules capable of multi-channel measurement and multi-wavelength detection

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Example of micro PMT array with optical system

Array devices en

15 mm

8.6 mm

Surface-Mount Package Micro PMT R15320U Series

The R15320U series is a micro PMT encapsulated in a plastic package designed for easy mounting by the useronto electronic circuit boards. The package size is further reduced to 8.6 mm × 15 mm. Two or more micro PMTs can be arrayed in parallel to allow equipment downsizing and also to meet demands for multi-functional use such as simultaneous analysis of multiple samples with just a single piece of equipment.

Photomultiplier tube designed even smaller to allow a parallel array configuration

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nabling multi-channel measurement

S f M t P k Mi PMT R15320U S i

Light

Micro PMT array

Dichroic mirror

Band-pass filter

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TO-8 Package Photomultiplier Tubes

Metal Package Photomultiplier Tube R14755U-100

Hamamatsu Photonics also provides TO (transistor outline) package photo-multiplier tubes that incorporate metal channel dynodes created by taking advantage of our advanced microfabrication technology. These photomulti-plier tubes feature compact size, light weight and fast time response, making them useful across a wide range of fields and applications including radiation measurement, semiconductor wafer inspection, and specimen tests.

The R14755U-100 is a metal package photomultiplier tube with a fast response of 800 MHz, developed for high-speed optical measurement such as underwater optical communication and electron beam detection. Compared to the conventional type (R9880), the time response is now twice as fast due to modification of the internal structure.

Photomultiplier tube with fast time response ideal for high-speed optical measurement

NEW

Metal Package Photomultiplier Tube R9880U-09

The R9880U series photomultiplier tubes deliver higher gain (approx. 5 times) and higher quantum efficiency (approx. 1.6 times*) when compared to the conven-tional (R9875). The R9880U-09, which is newly added to the lineup of the R9880U series, has a Cs-Te photo-cathode with excellent solar blind characteristics (spectral response range: 160 to 320 nm). The R9880U-09 can in this way detect low level light in the vacuum ultraviolet region for atomic absorption spec-troscopy, optical emission spectroscopy, and other photometric applications.* Quantum efficiency at 254 nm

Devlp.

Time response (Typ.)

Photomultiplier tube with excellent solar blind spectral response

TIME (1 ns/div.)

OU

TP

UT

VO

LTA

GE

(5

mV

/div

.)

FWHM: 680 ps1091 ps

R14755Conventional type (R9880)

FALL: 420 ps785 ps

RISE: 400 ps549 ps

Spectral response (Typ.)

14

(approx. 1.6 times*) when compared to the conven-tional (R9875) The R9880U-09 which is newly addedtional (R9875). The R9880U 09, which is newly added to the lineup of the R9880U series, has a Cs-Te photo-cathode with excellent solar blind characteristics (spectral rR9880U-09 vacuum ultrtroscopy, ophotometric* Quantum e

response range: 160 to 320 nm). The can in this way detect low level light in the

raviolet region for atomic absorption spec-optical emission spectroscopy, and other c applications.efficiency at 254 nm

100 200 300 400 500 600 700 8000.01

0.1

1

10

100

1000

WAVELENGTH (nm)

CA

TH

OD

E R

AD

IAN

T S

EN

SIT

IVIT

Y (

mA

/W)

QU

AN

TU

M E

FF

ICIE

NC

Y (

%)

R9880U-09R9880U-110R9880U-116

Cathode radiant sensitivityQuantum efficiency

TO-8 Package Photom

ultiplier TubesPhotom

ultiplier Tube Modules

Devlp.

Photomultiplier Tube ModulesWe are continually designing and developing various types of photomulti-plier tube modules to meet requirements in a diverse range of measurement applications. Our product lineup includes a wide array of versatile photomul-tiplier tube modules that vary in shape, characteristics, output configuration, and functions to let users choose the optimal product that best matches their needs and applications.

Linear-Array Multianode Photomultiplier Tube Module H15441-20

The H15441-20 is designed to function as a 6-channel spectrum detector. Compared to the conventional type (H13457-20) mainly designed for optical fibers with an effective fiber core diameter of 400 µm, the H15441-20 supports optical fibers with larger core diameters up to 1000 µm.

Photomultiplier tube module capable of simultaneous multi-wavelength measurement with high accuracy

Spectral efficiency of filter optics (Typ.)

EF

FIC

IEN

CY

(%

)

1 ch40

50

60

70

80

90

100

6 ch5 ch4 ch3 ch

Fiber core diameter (NA=0.2)

●Conventional type (H13457-20)

400 µm

2 ch

1000 µm

EF

FIC

IEN

CY

(%

)

1 ch40

50

60

70

80

90

100

6 ch5 ch4 ch3 ch

Fiber core diameter (NA=0.2)

●H15441-20

400 µm

2 ch

1000 µm

15

Applications

Internal structure

●Biomedical fluorescence detection●Flow cytometry

Photomultiplier tubeDichroic mirror

High-reflectivity mirror

Light

Band-pass filter

16

Photosensor Modules H14447, H14990

The H14447 and H14990 are photosensor modules having fast responses of 1 GHz and 0.7 GHz, respectively. Compared to the conventional type (H13661), the H14447 and H14990 offer improved ringing and fewer pulse height fluctuations in the output while also ensuring a wide opening in the eye pattern, making them more ideal for optical communication and laser radar (LiDAR).

NEWDevlp.

Devlp.

Photomultiplier tube modules capable of 1 Gbps communication

Photosensor Modules H14601, H14950, H14953

These are miniaturized photosensor modules integrating a TO-8 package photomultiplier tube and a high-voltage power supply circuit. Compared to our currently available products (H10721, H11900 and H11903 series), the cubic volume is reduced by about 50% to help users design more portable equipment. The H14601 is a cable type with +5 V input and current output (same as our currently available H10721). The H14950 is a pin type with +15 V input and current output (same as our currently available H11900). The H14953 is a cable type with +15 V input and voltage output (same as our currently available H11903).

Miniaturized photomultiplier tube modules that help the design of more portable equipment

Photosensor Module H14768

The H14768 is a photosensor module incorporating a side-on photomultiplier tube with a high-sensitivity multialkali photo-cathode along with a high-voltage power supply circuit and a thermoelectric cooler. Compared to the conventional type (H7844), the maximum cooling temperature is improved to reduce noise on low-light-level detection in the near-infrared region.

Photomultiplier tube module ideal for low-light-level detection in the near-infrared region

NEW

Left: H14447, Right: H14990

Left: H14950, Center: H14601, Right: H14953

0 500 1000 1500-5

0

5

10

15

20

25

30

COOLING TIME (s)

TE

MP

ER

ATU

RE

(°C

)

2000

Ambient temperature: 25 °CPeltier input current: 1.3 A

TIME (1 ns/div.)

OU

TP

UT

VO

LTA

GE

(10

mV

/div

.)

FALL: 250 psRISE: 350 ps

FWHM: 440 ps

Applications●Optical communication●Laser radar (LiDAR)

Applications●Environmental measurement●Specimen test (POCT: point-of-care testing)

Applications●NOx gas detection●Fluorescence detection●Chemiluminescence detection●Near-infrared spectroscopy

Time response (Typ., H14447) Eye pattern (1 Gbps) (Typ., H14447)

Photocathode temperature vs. cooling time (Typ.)

17

Mic

ro P

MT

Photon Counting Head H14870

The H14870 photomultiplier tube module is designed specifically for MTP readers (microplate readers). It has the light input openings arranged at intervals equal to the well-to-well spacing for 96-well microplates and allows 16-channel simultaneous measurement with low crosstalk. This will significantly improve the throughput of MTP readers.

Photomultiplier tube module capable of 16-channel photon counting

NEW

Wide Dynamic Range Photomultiplier Tube Module H13126-01

The H13126-01 is a compact photomultiplier tube module that allows continuous measurement each time with no time lag over a 10-log dynamic range and with just one unit. The H13126-01 provides a digital output for detecting low-level light counting signal and an analog output for detecting high-level visible light, both of which can be measured simultaneously.

Photomultiplier tube module that ensures a wide dynamic range up to 10 log units in one measurement

NEW

Photomultiplier Tube M

odules

In laser radar (LiDAR) systems for obtaining information on overhead clouds and aerosols by capturing scattered light of a laser beam transmitted into the atmosphere, the H13126-01 is used to make simultaneous measure-ments of three output signals: two analog signals and one counting signal.The graph on the right shows the count rate versus distance data with a wide dynamic range, plotted by converting the analog signals to the count rate.

0 1 2 3 4 5 6 7 8 9 1010-1

100

101

102

103

104

105

DISTANCE (km)

CO

UN

T R

ATE

(M

s-1 )

Analog signal (Converted to count rate)

Analog signal (Converted to count rate)

Counting signal

Applications●MTP readers (microplate readers)

Applications

Measurement example

●Laser radar (LiDAR)●Fluorescence measurement●Chemiluminescence measurement

18

Infrared (IR) Light SourcesOur product lineup includes advanced infrared light sources that have out-standing features compared to thermal type light sources such as halogen lamps. Our infrared light sources will help users achieve their objective and meet requirements in a wide range of applications including gas measure-ment, gas analysis, product inspection, and infrared spectroscopy.

NEW

900 1100 1300 1500 1700 1900 2100 23000

20

40

60

80

100

WAVELENGTH (nm)

RE

LAT

IVE

OU

TP

UT

(%

)

0 1 2 395

97

99

101

103

105

96

98

100

102

104

TIME (min)

RE

LAT

IVE

OU

TP

UT

(%

)Our supercontinuum light sourceCompetitor’s supercontinuum light source

Supercontinuum Light Source L15077

The L15077 is a compact laser light source that uses broadband laser light generated by a nonlinear optical phe-nomenon utilizing an ultra-short pulsed laser. It provides high directivity and high brightness like that of a laser and a broadband spectrum like that of a lamp light source.

Near-infrared laser light source with a broad spectrum and high stability

Features●High stability: 0.1 % or less (typ.)●Broad spectrum: 1300 nm to 2000 nm●High brightness: Approx. 20,000 times (compared to halogen lamps)

Applications●Fourier transform near-infrared spectrophotometry (FT-NIR)●Optical coherence tomography (OCT)●Gas measurement and analysis●Semiconductor wafer inspection●Near-infrared spectroscopy

Spectral distribution (Typ.) Output stability (Typ. at 1500 nm)

18

Applications●Fourier transform near-infrared spectrophotometry (FT-NIR)●Optical coherence tomography (OCT)●Gas measurement and analysis

100 105

●Semiconductor wafer inspection●Near-infrared spectroscopy

Spectral distribution (Typ.) Output stability (Typ. at 1500 nm)

900 1100 1300 1500 1700 1900 2100 23000

20

40

60

80

100

WAVELENGTH (nm)

RE

LAT

IVE

OU

TP

UT

(%

)

0 1 2 395

97

99

101

103

105

96

98

100

102

104

TIME (min)

RE

LAT

IVE

OU

TP

UT

(%

)Our supercontinuum light sourceCompetitor’s supercontinuum light source

19

Infra

red

(IR) L

igh

t So

urc

es

Devlp.

0 100.01

0.1

1

10

100

20

TIME (µs)

RE

LAT

IVE

IRR

AD

IAN

CE

30

20 W XENON FLASH LAMP (MgF2)24 W GLOBAR LIGHT SOURCE150 W HALOGEN LAMP0.44 W MEMS INFRARED LIGHT SOURCE

1.5

10

2

WAVELENGTH (µm)

RE

LAT

IVE

IRR

AD

IAN

CE

2.5

20 W XENON FLASH LAMP2 W XENON FLASH LAMP MODULE7.2 W HALOGEN LAMP

2 3 4 5 6 7 8 9 10 11 120

2

4

6

8

10

12

14

WAVELENGTH (µm)

RE

LAT

IVE

IRR

AD

IAN

CE

H2O

H2O CO2

Instrument: Fourier transform infrared spectrophotometer (FTIR)

Detector: MCTEmission point temperature: 1000 °CAtmosphere: Atmospheric air

* Spectral distribution depends on the atmospheric components.

IR Graphene Light Source

The IR graphene light source is a thermal mid-infrared light source that operates at high temperatures to emit black body radiation. Besides high temperature operation, the IR graphene light source offers excellent features such as faster time response and lower power consumption compared to conventional thermal light sources, making it a promising tool for a wide range of applications.

Thermal mid-infrared light source with high brightness and fast time response

Broad Infrared Spectrum Xenon Flash Lamp

This xenon flash lamp is an infrared light source that emits a broad spectrum spanning from 0.16 µm to 7.5 µm. Compared to other types of infrared light sources, this xenon flash lamp features low heat generation, stable operation and momentarily high optical output. It also delivers a long service life and ensures high reliability.

NEW

Pulsed light source that emits a broad infrared spectrum

Spectral distribution (Typ.) Time response (Typ.)

Features●High temperature operation: Emission point temperature approx. 1000 °C●Fast time response: 3000 Hz (max.)●Low power consumption: 1000 mW (typ.)●Broad emission spectrum: 1 µm to 7.5 µm●Emission point size: 100 µm × 2000 µm

Features●Broad spectrum: 160 nm to 7500 nm●Momentarily high optical output: Approx. 1000 times (compared to halogen lamps)●Low heat generation●High stability●Long life

Applications●Non-dispersive infrared (NDIR) gas sensor●Fourier transform infrared spectrophotometer (FTIR)●Breath monitor (CO2, etc.)

Applications●Food analysis, foreign matter inspection, food sorting●Gas measurement and analysis●Infrared spectroscopy

0 500 1000 1500 2000 2500

RE

LAT

IVE

IRR

AD

IAN

CE

(%

)

TIME (µs)

120

100

80

60

40

20

0

FALL TIME: 20 µsRISE TIME: 80 µs

Detector: Spectrometer NIRQuest512-2.5 made by Ocean Optics (slit width: 25 µm, integration time: 1 ms)Optical fiber: MF11L1 made by Thorlabs (core diameter: 100 µm, InF3 transmission wavelength range: 0.3 µm to 5.5 µm)

* Light output depends on detector sensitivity.Use this data as a reference for comparison with other infrared light sources.

* Light output of halogen lamp is corrected to peak irradiance of xenon flash lamp (flash duration: approx. 6 µs)

Emission pulse waveform (Typ.)Spectral distribution (Typ.)10

RE

LAT

IVE

IRR

AD

IAN

CE

2 3 40

2

H2O C

* Spectral distribution d

Broad Infrare

This xenon flash laCompared to otheoperation and mom

Pulsed light s

Features●Broad spectrum: ●Momentarily high Approx. 1000 time●Low heat generat●High stability●Long life

Detector: Spectrometer NIR(slit width: 25 µm, integratioOptical fiber: MF11L1 madeInF3 transmission waveleng

* Light output depends on dUse this data as a referenc

* Light output of halogen lam(flash duration: approx. 6 µ

Spectral distributio

Tube voltageTube current

180 kV300 µA

Sample

Imaged region

Void

2 mm

Sample

Imaging example●Tablets in aluminum foil pouch

20

Imaging DevicesImaging technology, which enables high-precision inspection, measurement and analysis, is now used across a vast range of fields. We at Hamamatsu Photonics are continuing to develop sophisticated yet easy-to-use imaging devices such as for transmission imaging utilizing X-rays and neutrons, and low-light-level imaging in the UV to the near-infrared regions.

180 kV Microfocus X-Ray Source L14351-02

X-Ray Imaging

The L14351-02 is a sealed type micro-focus X-ray source that achieves the world’ s highest tube voltage (maximum tube voltage 180 kV) and high output (maximum output 90 W). In addition to high resolution (up to 10 µm), it handles samples that are normally difficult to view in X-ray non-destructive inspec-tions and X-ray CT using sealed type X-ray sources. It also improves the imaging speed.

The L11754-01 is a soft X-ray source that operates at low energy (tube voltage: 15 kV, tube current: 1 mA) to allow find-ing foreign objects made of light elements that were difficult to detect up to now. The L11754-01 features compact size, light weight, easy shielding, and wide X-ray emission angle, making it optimal for inspection applications such as finding poor package sealing of foodstuffs and medicines or detect-ing misalignment of rechargeable battery separators.

Sealed type X-ray source with the world’s highest tube voltage of 180 kV maximum

NEW

Soft X-Ray Source L11754-01

Soft X-ray source that operates at low energy for detecting foreign objects made of light elements

Compact X-Ray CMOS Camera Digital X-CUBE

Digital X-CUBE is a compact X-ray CMOS camera using a CMOS image sensor chip optically coupled to a high-sensitivity CsI scintillator. It gives high-sensitivity, high-quality X-ray images in the same easy way as when using ordinary CMOS cameras.

High-sensitivity X-ray camera designed to smoothly and effortlessly capture high-quality X-ray images

Devlp.

Devlp.

Features●High contrast imaging for

light elements●Compact, lightweight

●Easy shielding●Wide emission angle

Imaging example●Automotive engine die casting

21

Ima

gin

g D

ev

ice

s

The graphs show analysis data when pulsed neutrons were detected and in te-grated 100 times.The gray area of the integra-tion map is displayed by ex-tracting data from noise-free regions of the TOF distribu-tion and pulse height distri-bution graphs.

C14245 series

Relay lens

Camera

Connection example Imaging example●Observation of discharges on PC board

Ordinary visible imageImage captured with C14245

Poor insulation (discharge)

TOF distribution

0 5000

50

100

150

200

250

300

TIME (µs)

TOF

CO

UN

T

1000 1500 2000

Pulse height distribution

100 2001

10

100

1000

10000

OUTPUT (mV)C

OU

NT

400

Integration map Measurement block diagram

High-count-rateneutrondetector

Trigger signal

Pulsed neutron

Neutronshielding

Pulsedneutron

generator

High-Count-Rate Neutron Detector Unit

Neutron Imaging

This high-count-rate neutron detector unit uses a multianode photomultiplier tube combined with a scintillator and readout circuit. To detect neutrons in a particular energy region, the detector unit comes with analysis software that can be customized to meet user needs. This detector unit is ideal for small-angle or backscatter imaging and supports imaging up to 256 channels.

Neutron detector with built-in multi-channel readout circuit

High-Speed Gated Image Intensifier Unit C14245 Series

Low-Light-Level Imaging

The C14245 consists of an image intensifier (or I.I.), a high-voltage power supply circuit and a gate drive circuit enclosed in a cubic housing. The cubic housing easily connects to the body of most large-sized, high-performance cameras, which has been difficult for the conventional type (C9546 series) that has an L-shape configuration. The standard lens mount of the C14245 is a C-mount but can be easily changed to an F-mount if needed.

Compact image intensifier unit with gate function of 3 ns to DC

C-mount type

F-mount type

NEW

Technology

Measurement example●Measurement data

Neutralization performance (Typ., L12542)

22

Static Charge RemoversHamamatsu Photonics provides a variety of static charge removers that neutralize static electricity by utilizing photoionization known as a clean ion-ization method. Photoionization proves a powerful tool for solving problems with static charges that have recently arisen in production processes and other tasks and in this way improves both the throughput and yield.

VUV Ionizers L12542, L15094

The L12542 and L15094 eliminate static charges in a vacuum by utilizing vacuum UV light. Due to their greatly improved neutralization performance over larger areas, they can handle a variety of objects with large surface areas, with heavy electrical charges, or moving on high-speed conveyors and in this way help shorten the neutral-ization time.

Static charge removers that neutralize static charges across large areas with greater efficiency

L15094

NEW

PhotoIonizers L14471, C14472, C14546

These photoionizers use soft X-rays to neutralize static charges in the atmosphere and are designed to drive 2 or 4 ionizer heads to boost neutralization performance to the maximum level. They can handle a variety of objects with large surface areas, with heavy electrical charges, or moving on high-speed conveyors and in this way shorten the neutralization time.

Static charge removers designed to drive multiple ionizer heads for extracting maximum neutralization performance

L14471, C14472

NEW

Applications●Electrostatic dechucking●Semiconductor manufacturing●Liquid crystal and organic EL display manufacturing●Film manufacturing●Equipment using electron beams (SEM, etc.)

●Neutralization time vs. distance ●Neutralization time vs. vacuum level

0.00010

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.001 0.01

VACUUM LEVEL (Pa)

NE

UT

RA

LIZ

AT

ION

TIM

E (

s)

0.1 1 10

Charge plate: 25 mmCharge voltage: 1 kV / 100 VOutput window to charge plate distance: 300 mm

Positive chargeNegative charge

0 200 400 600 800 1000 1200 14000

1

2

3

4

5

OUTPUT WINDOW TO CHARGE PLATE DISTANCE (mm)

NE

UT

RA

LIZ

AT

ION

TIM

E (

s)

Positive chargeNegative charge

Charge plate: 25 mmCharge voltage: 1 kV / 100 VVacuum level: 1 × 10-2 Pa

Applications●Semiconductor manufacturing●Component mounting in chip mounter●Liquid crystal and organic EL display manufacturing●Film manufacturing●Lithium ion rechargeable battery manufacturing●Printing, painting

23

High-Voltage Pow

er Supply M

odulesS

tatic Charge R

emovers

100200 10 20 30 40 50 60 70

TIME (min)

OU

TP

UT

VO

LTA

GE

(V

)

10021

10022

10023

10024

10025

10026

10027

10028

10029

10030

Input voltage: +15 VControl voltage: +5 VInput impedance: 100 MΩ

Stability: 43 ppm/h (Typ.)

High-Voltage Power Supply ModulesAs a leading manufacturer of high-sensitivity photosensors and photomulti-plier tubes, Hamamatsu Photonics offers high-voltage power supplies with advanced features utilizing technologies that have been developed and accumulated over many years. Our high-voltage power supplies help to improve reliability in a wide range of applications including mass spectrom-eters, scanning electron microscopes (SEM), and electrostatic chucks.

High-Voltage Power Supply Module C14051-55

The C14051-55 is a compact, high-efficiency, high-voltage power supply designed to provide high voltage output up to +10 kV and 200 µA. The C14051-55 is provided with high safety by comprising a double insulation structure and vari-ous protective function. It also has wide input voltage range and output monitor (voltage / current). So it is suitable for incorporating to apparatus.

Regulated high-voltage DC power supply capable of high voltage output up to +10 kV and 200 µA

NEW

High-Voltage Power Supply Module C14921-01

The C14921-01 is a bipolar high-voltage power supply with a maximum output of ±5 kV and 200 µA. Our previous models of high-voltage power supplies are single-polarity types or dual-polarity types required with switching polarity beforehand. The C14921-01, makes it possible to control the output voltage continuously by using control-ling voltage without requiring a switch or selector.

Regulated bipolar high-voltage power supply that provides output varied continu-ously from -5 kV to +5 kV without switching beforehand

Devlp.

Stability (Typ.)

Features●High voltage output: Maximum +10 kV and 200 µA●Wide input voltage range: +11 V to +16 V●Output monitor (voltage / current) included●Safety design with multiple protective functions

Features●Bipolar output: Maximum ±5 kV and 200 µA●Polarity switching by control voltage●High-speed time response: 250 µs (10 % to 90 %) ●Output monitor (voltage / current) included

Electron Tube Division, HAMAMATSU PHOTONICS K.K.314-5, Shimokanzo, Iwata City, Shizuoka Pref., 438-0193, JapanTelephone: (81)539/62-5248, Fax: (81)539/62-2205www.hamamatsu.com

Main ProductsElectron TubesPhotomultiplier tubesPhotomultiplier tube modulesMicrochannel platesImage intensifiersXenon lamps / mercury-xenon lampsDeuterium lampsLight source applied productsLaser applied productsMicrofocus X-ray sourcesX-ray imaging devices

Opto-semiconductorsSi photodiodesAPDMPPC®

Photo ICImage sensorsPSDInfrared detectorsLEDOptical communication devicesAutomotive devicesX-ray flat panel sensorsMini-spectrometersOpto-semiconductor modules

Imaging and Processing SystemsCameras / Image processing measuring systemsX-ray productsLife science systemsMedical systemsSemiconductor failure analysis systemsFPD / LED characteristic evaluation systemsSpectroscopic and optical measurement systems

Laser ProductsSemiconductor lasersApplied products of semiconductor lasersSolid state lasers

Sales Offices

Information in this catalog is believed to be reliable. However,no responsibility is assumed for possible inaccuracies or omission.Specifications are subject to change without notice. No patentrights are granted to any of the circuits described herein.© 2020 Hamamatsu Photonics K.K.

Quality, technology and service are part of every product.

REVISED APR. 2020

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United Kingdom:HAMAMATSU PHOTONICS UK LimitedMain Office2 Howard Court, 10 Tewin Road, Welwyn Garden City,Hertfordshire AL7 1BW, UKTelephone: (44)1707-294888, Fax: (44)1707-325777E-mail: info@hamamatsu.co.uk

South Africa Contact:9 Beukes Avenue, Highway Gardens, Edenvale1609 South AfricaTelephone/Fax: (27)11-609-0367

France, Portugal, Belgium, Switzerland, Spain:HAMAMATSU PHOTONICS FRANCE S.A.R.L.Main Office19, Rue du Saule Trapu, Parc du Moulin de Massy,91882 Massy Cedex, FranceTelephone: (33)1 69 53 71 00, Fax: (33)1 69 53 71 10E-mail: infos@hamamatsu.fr

TOTH0029E02APR. 2020 IP

MIGHTION, CERARION, DIUTHAME, LIGHTNINGCURE are registed trademarks of Hamamatsu Photonics K.K.