Universal Streak Camera C10910 Series UV to near-infrared measurement with 1 ps temporal resolution The streak camera is an ultrahigh-speed detector which captures light emission phenomena occurring in extremely short time periods. In addition to superb temporal resolution, the streak camera can capture spatial (or spectral) data simultaneously. The C10910 series is a universal streak camera which incorporates all of the specialized technology and expertise that HAMAMATSU acquired over 20 years of research. The streak tubes are manufactured on a regular production Applications Fluorescence lifetime measurement, transient absorption measurement, time-resolved Raman spectroscopy Optical communications, response measurement of quantum devices Measurement of electron bunch for synchrotron and LINAC applications Research involving free electron lasers, and various other types of pulsed lasers schedule at Hamamatsu to provide consistency and reliability. Special requests and custom designs are also available. Plasma light emission, radiation, laser ablation, combustion and explosions Lidar Thomson scattering, laser distance measurement A diverse range of experimental setups from single light emitting phenomena to high-speed repeated phenomena in the GHz domain Simultaneous measurement of light intensity on temporal and spatial (wavelength) axis Spectrograph can be placed in front of the streak camera to convert the spatial axis to the wavelength. This enables highly efficient time-resolved spectroscopy measurements. UV to near-infrared wavelengths Optimize the streak camera’s performance by selecting the appropriate streak tube (light sensor) for desired spectral range. Ultra-high sensitivity (detection of single photons) The streak tube converts light into electrons which are then multiplied by an electron multiplier. This enables detection of extremely faint light (at the single-photon level). (See page 8 "The principle of photon counting integration") USB control Computer control enables remote operation and advanced measurements with ease of use. Improved S/N with the internal MCP Diverse selection of peripheral equipment System configuration A full lineup of peripheral devices including spectroscopes, optical trigger heads, and expansion units. Plug-in unit ⋅Horizontal blanking unit M10914-01 ⋅Shift blanking unit M10914-02 ⋅Synchronous blanking unit M10915-01 ⋅Dual time base extender unit M10916-01 ⋅High repetition dual time base extender unit M10916-03 Function expansion unit Peripheral equipment Main unit, Optics Readout system Readout camera Spectroscope A11119-02 R Input optics Output optics ORCA -R2 (Standard type) IEEE1394b A1976-01 A11695-01 A11771-01 A11350-14 C9300-508 (High frame rate type) A1974 Streak camera Main unit Camera Link Power supply unit C10910 C10910 A11695-02 A11771-02 Plug-in unit ⋅Synchroscan unit M10911-01, -02 Sweep unit ⋅Fast single sweep unit M10912-01 ⋅Slow single sweep unit M10913-01 2 Data analyzer SPECIFICATIONS: Main unit, Optics The C10910 streak camera includes a choice of streak tube detectors and a variety of plug-in options for optimum performance. Main unit Spectral response of the streak tube (typ.) Main unit C10910 100 C10910-01 S-20 200 nm to 850 nm C10910-02 S-1 300 nm to 1600 nm C10910-04 S-25 280 nm to 920 nm C10910-05 S-20ER 200 nm to 900 nm S-20ER S-25 0.15 mm × 4.42 mm (when coupled with ORCA-R2 CCD camera) 10 > 3 × 103 ⋅Phosphor characteristic P-43 ⋅Effective phosphorscreen size φ18 mm better than 40 lp/mm (center of photocathode, wavelength 530 nm) Spatial resolution Interface Power supply Power consumption Weight S-20 Radiant sensitivity (mA/W) Type number Photocathode Spectral response characteristic Effective photocathode size *1 MCP gain Phosphor screen USB 2.0 AC 100 V to AC 240 V, 50 Hz / 60 Hz Approx. 200 VA Approx. 19 kg *1 Effective photocathode size 0.5 mm x 4.42 mm is available as an option, and photocathode is serective from S-20 or S-20ER. Model number C10910-21 is for S-20, and C10910-25 for S-20ER. Please contact us for further information. <Photo cathode cooling option> Type number Cooling temperature M11748 Approx. 0 : S-1 1 0.1 0.01 <Gate function> Gating method Extinction ratio Gate time Gate trigger input Gate trigger delay time Horizontal blanking repetition frequency (Max.) MCP gate repetition frequency (Max.) Photocathode gate repetition frequency (Max.) MCP MCP + horizontal blanking + horizontal blanking + photocathode 1:106 min 1:108 min 50 ns to continuous TTL / 50 Ω max.300 ns 4 MHz 10 kHz 10 kHz 0.001 0.0001 200 400 600 800 1000 1200 1400 Wavelength (nm) Optics Input optics Spectral transmission Effective F value Image multiplication ratio Slit width Slit width reading precision Overall length Spectral transmittance of input optics A1976-01 A1974 200 nm to1600 nm 5.0 400 nm to 900 nm 1.2 1:1 0 mm to 5 mm 5 μm 98.2 mm 159 mm Output optics Type number Image multiplication ratio Effective F value Lens mount Corresponding camera 100 Transmittance(%) Type number A1974 A1976-01 80 60 40 20 0 200 400 600 800 1000 1200 1400 1600 Wavelength (nm) A11695-01 A11695-02 1:0.7 (50 mm:35 mm) 2.0 F-mount ORCA-R2 2:1 (105 mm:50 mm) 2.8 F-mount C9300-508 3 SPECIFICATIONS: TIONS: Plug-in unit (Plug-in: built into main unit) Sweep unit Function expansion unit (connected to side panel of main unit) (connected to top of main unit) Horizontal blanking unit M10914-01 Synchroscan unit M10911-01, -02 Sweep unit for high-sensitivity and high temporal resolution measurements when synchronized with a high-repetition laser such as a mode-locked Ti-sapphire laser. Type number M10911-01 M10911-02 Temporal resolution *1 < 1 ps FWHM < 2 ps FWHM Sweep time *2 Approx. 100 ps to 1/6 fs Approx. 200 ps to 1/6 fs Sweep range 5 selectable ranges 3 selectable ranges Synchroscan frequency Selectable from 75 MHz to 165 MHz 250 MHz Synchronous frequency fs ±0.2 MHz range Temporal resolution or less Trigger jitter –3 dBm to +17 dBm / 50 Ω Trigger signal input Trigger delay tuneup > 360 degree *1 At the center of window at 800 nm wavelength NOTE: The figure does not include phase noise of the light source or temporal broadening by a spectrograph. The time resolution changes as following values when using the C10910-04(S-25). Type number Temporal resolution M10911-01 < 4 ps FWHM M10911-02 < 4 ps FWHM *2 fs = synchroscan frequency The standard unit for return sweep blanking during single-sweep operation. For return sweep blanking in synchroscan operation, refer to M10914-02 or M1091501. Type number M10914-01 Sweep repetition frequency (Max.) 4 MHz Shift blanking unit M10914-02 For use in combination with synchroscan and pulse picker or regen amplifier, For applications such as fast picosecond risetime or lifetime decay of data which may include residual light extending beyond the synchroscan’s return sweep, e.g. nanoseconds to milliseconds. Type number M10914-02 Sweep repetition frequency (Max.) Trigger signal input Blanking time (Max.) 10 kHz ± 5 V/50 Ω 10 μs * Patented Fast single sweep unit M10912-01 High-speed sweep plug-in unit designed for high resolution single-shot measurements, but can also trigger up to 10 kHz at lower resolutions. Type number Temporal resolution *1 Sweep time Trigger jitter Trigger delay Sweep repetition frequency (Max.)) Trigger signal input Monitor out signal (With M10911-01 Synchroscan unit) Extends the performance of synchroscan operation by synchronously blanking the return sweep. For applications such as high-repetition light in the GHz range, or for picoseconds risetime and lifetime decay measurements on data which includes residual light beyond a few nanoseconds, but less than the synchroscan’s sweep period (e.g. < 10 ns). M10912-01 < 1 ps FWHM 0.1 ns to 50 ns / full (with ORCA-R2) <10 ps rms Approx. 10 ns (fastest sweep range) Type number Synchroscan frequency Horizontal shift width M10915-01 Selectable from 75 MHz to 165 MHz 3 mm or 13 mm (at phosphor screen) 10 kHz ± 5 V/50 Ω 3 Vp-p (typ.) *1 At the center of window at 800 nm wavelength NOTE: The figure does not include phase noise of the light source or temporal broadening by a spectrograph. The time resolution changes as following values when using the C10910-04(S-25). Type number Temporal resolution Synchronous blanking unit M10915-01 M10912-01 < 4 ps FWHM Slow single sweep unit M10913-01 A sweep unit for randomly triggered or single-shot measurements of slower phenomena. Dual time base extender unit M10916-01 (Can be used with all sweep units) For simultaneous dual-sweep operation and single channel narrow V-slit input. Compatible with all sweep plug-in units, the M10916-01 extender unit provides slower time axis in a perpendicular axis, e.g. simultaneous high-speed vertical sweep and horizontal slower sweep. For applications such as bunch length measurements or phase stability in synchrotrons. Type number Sweep time Sweep repetition frequency (Max.) Trigger signal input Monitor out signal M10916-01 100 ns to 100 ms / full (with M10911-01, -02, with ORCA-R2) 1 ms to 100 ms / full (with M10912-01, with ORCA-R2) 2 μs to 100 ms / full (with M10913-01, with ORCA-R2) 10 Hz ± 5 V/50 Ω 3 Vp-p (typ.) High repetition dual time base extender unit M10916-03 Type number Temporal resolution Sweep time Trigger jitter Trigger delay Sweep repetition frequency (Max.) Trigger signal input Monitor out signal 4 M10913-01 <20 ps FWHM 1.2 ns to 1 ms / full (with ORCA-R2) Temporal resolution or more Approx. 40 ns (fastest sweep range) 4 MHz (fastest sweep range) ± 5 V / 50 Ω 3 Vp-p (typ.) High repetition version of the M10916-01. Enables higher-repetition frequency measurements for applications such as photon correlation. Type number Sweep time Sweep repetition frequency (Max.) Trigger signal input Monitor out signal M10916-03 50 ns, 100 ns, 200 ns, 400 ns, 600 ns / full (with C9300-508) 1 kHz ± 5 V/50 Ω 3 Vp-p (typ.) SPECIFICATIONS: Readout system Streak camera Readout camera Data analyzer Digital CCD camera ORCA-R2 IEEE1394b Streak camera Main unit C10910 IEEE1394b board lens output Mount table A11771-01 PC ORCA-R2 Camera control unit Digital CCD camera C9300-508 Camera Link Control & readout software HPD-TA Camera Link I/F board AC adapter Mount table A11771-02 USB Readout camera Data analyzer Digital CCD camera ORCA-R2 Control & readout software HPD-TA Recommended readout camera for universal applications, including singleshot, analog and photon counting integration. The HPD-TA is a high-performance digital data acquisition and control system specifically designed to read out images from the streak camera's phosphor screen. The HPD-TA allows the remote control of the C10910 via USB interface. The entire system is controlled through a powerful but user friendly software application that runs on a Microsoft Windows platform. Data acquisition Type number Effective number of pixels Cell size Effective area Working area on phosphor screen Working size of photocathode Exposure time Readout speed A/D converter ORCA-R2 (C10600-10B) 1344 (H) × 1024 (V) 6.45 μm (H) × 6.45 μm (V) 8.67 mm (H) × 6.60 mm (V) 12.39 mm (H) × 9.43 mm (V) Approx. 4.42 mm (H) 10 μs to 4200 s 28.4 frames/s (2×2 binning / fast scan mode) 12 bit /16 bit Device control Profile functions Data corrections Axis calibration File formats (images) File format (profiles) Live mode, analog integration photon counting, sequence recording C10910, CCD camera, spectrograph, delay units Real-time display, min/max, FWHM, Gauss fit Background, sensitivity, curvature, jitter Channel, time, wavelength Binary (up to 32 bits), TIFF, ASCII ASCll Mount table (for ORCA-R2) A11771-01 Digital CCD camera C9300-508 Readout camera optimized for rapid photon counting operation. Type number Effective number of pixels Cell size Effective area Working area on phosphor screen Working size of photocathode Exposure time Readout speed A/D converter C9300-508 640 (H) × 480 (V) 7.4 μm (H) × 7.4 μm (V) 4.74 mm (H) × 3.55 mm (V) 9.95 mm (H) × 7.46 mm (V) Approx. 3.55 mm (H) 33.1 μs to 1 s 150 frames/s (1×1 binning) 12 bit * Computer environment The HPD-TA requires an industry-standard PC with Microsoft Windows. A high-resolution graphics configuration is recommended. Depending on the streak system configuration, a number of PCI or PCIe slots as well as some USB ports may be required. Mount table (for C9300-508) A11771-02 5 SPECIFICATIONS: TIONS: Peripheral equipment Optical trigger Light-emitting phenomenon ND filter set A7664 Incident light Streak camera Input section Spectroscope C11119-02 Beam splitter Variable ND filter Trigger Streak camera main unit C10910 Spectroscope mount table A11350-14 Trigger unit ⋅Delay unit C1097-05 ⋅RF up converter unit C6207 ⋅High-stability delay unit C12270 ⋅Digital delay generator DG645 ⋅Streak trigger unit C4547-02 ⋅Synchronous delay generator C10647-01 PIN diode head C1083-01, C1808-03 Input section Optical trigger (PIN diode head) PIN diode head C1083-01 (for low repetition) Spectroscope C11119-02 Used to generate a trigger signal for the streak camera with lasers with low repetition rates. The combination with streak camera enables to measure wavelength, time and light intensity simultaneously. The following are needed in order to connect these units to the streak camera: Spectroscope mount table Light source for wavelength axis calibration (mercury lamp, etc.) Type number C11119-02 Optical layout Czerny-Turner model (with toroidal mirror for aberration correction) Focal distance F value Incident light slit width Grating Type number 300 mm 4.0 Variable between 10 μm to 3 mm Spectral response Risetime Dimensions/ weight Power supply C1083-01 400 nm to 1100 nm 0.8 ns Head: (W)100 mm ×(D)50 mm ×(H)160 mm to 235 mm / 400 g Power supply unit: (W)100 mm ×(D)100 mm ×(H)83 mm / 400 g +18 V (battery) 3 ( Additional turret/grating available) Reciprocal dispersion PIN diode head C1808-03 (for high repetition) 2.38 nm/mm (when using 1200 gr/mm) Dimenstions/weight Used to generate a synchronization signal for the streak camera with modelocked lasers. (W)377 mm × (D)305 mm × (H)217 mm / 15.9 kg Spectroscope mount table A11350-14 A mount table to set up and to fix a streak camera and a spectrograph. Fiber-optic input optics (FC Connector) A6368 Fiber-optic input optics can be connected in place of the incident light slit in the streak camera. Type number Gratings (typical examples) No. of grooves Blaze wavelength Wavelength range Measurement wavelength range * resolution 40 gr/mm 500 nm 335 nm to 750 nm Approx. 354 nm Approx. 5.1 nm 50 gr/mm 600 nm 400 nm to 1200 nm Approx. 283 nm Approx. 4.2 nm 100 gr/mm 450 nm 300 nm to 700 nm Approx. 141 nm Approx. 2.1 nm 150 gr/mm 300 nm 200 nm to 500 nm Approx. 94 nm Approx. 1.4 nm 150 gr/mm 500 nm 335 nm to 750 nm Approx. 94 nm Approx. 1.4 nm 300 gr/mm 500 nm 335 nm to 750 nm Approx. 46 nm Approx. 0.7 nm 600 gr/mm 500 nm 335 nm to 750 nm Approx. 22 nm Approx. 0.34 nm 1200 gr/mm 500 nm 335 nm to 750 nm Approx. 10 nm Approx. 0.15 nm * This is the wavelength range within which simultaneous measurement is possible when used in combination with C10910 and ORCA-R2. 6 Minimum input level Saturation output level Frequency band Power supply C1808-03 1 mW (f=80 MHz, λ=800 nm, FWHM<1 ps) Approx. 1.5 Vp-p (50 Ω) <100 MHz AC100 V to AC240 V, 50 Hz / 60 Hz ND filter set A7664 The adjustment tool of input light intensity for C1808-03. A variable ND filter and a laser beam splitter are included. Trigger units Delay unit C1097-05 High stability delay unit C12270 A jitter-free delay unit that can be used for single-sweep as well as synchroscan setups. Type number Variable delay range Delay setting range Minimum delay time Maximum input voltage Interface Power supply Power consumption Dimensions / weight C1097-05 0 ns to 31.96 ns 30 ps, 60 ps, 120 ps, 250 ps, 500 ps, 1 ns, 2 ns, 4 ns, 8 ns, 16 ns Approx.12 ns 30 V USB 2.0 AC 85 V to AC 250 V Approx. 30 VA (W)215 mm × (D)350 mm × (H)102 mm / 3.4 kg Used in combination with a synchroscan unit M10911-01,-02, the C12270 is used to adjust the phase of the synchronization signal. In addition, the phase can be stabilized, thereby allowing the stable acquisition of streak images over a long period of time. Type number C12270-01 C12270-02 C12270-03 250 MHz 75 MHz to 110 MHz 110 MHz to 165 MHz -3 dBm/50 Ω to 6 dBm/50 Ω -3 dBm/50 Ω to 6 dBm/50 Ω 0 dBm/50 Ω to 6 dBm/50 Ω Ref.in Input level : -35 dBm/50 Ω to 10 dBm/50 Ω Output signal level 0 dBm/50 Ω to 10 dBm/50 Ω Valuable delay range Phase angle : 360 ° Interface USB 2.0 Power supply AC100 V to AC240 V, 50 Hz/60 Hz Power consumption Approx. 50 VA Dimensions / weight (W)262 mm × (D)333 mm × (H)74 mm / 3.5 kg Input signal Input * Patented * Output signale level is fluctuated along with input signal level * The output signal level is changed by the delay and the drift level of phase lock. RF up converter unit C6207 Generates 100 MHz output signal synchronized with 10 MHz input signal. Can be used to stably synchronize a synchroscan unit by inputting the reference output signal of a commercially available frequency synthesizer. Type number Input signal frequency Input level Output frequency Output signal level (typ.) Timing jitter Power supply Power consumption Dimensions / weight C6207 10 MHz ±10 Hz -10 dBm to 0 dBm / 50 Ω 100 MHz 3 dBm / 50 Ω < 1 ps rms AC 100 V to AC 240 V, 50 Hz/60 Hz Approx. 20 VA (W)262 mm × (D)330 mm × (H)74 mm / 3.2 kg Streak trigger unit C4547-02 Convert external trigger signal to gate trigger and streak trigger signal, and provide them to a single sweep unit. Dividing function enables to operate an external trigger that is faster than the sweep frequency of a single sweep unit. Type number Input signal frequency Input level Output signal level Output frequency Dimensions / weight C4547-02 10 MHz to 200 MHz 0 dBm to 15 dBm / 50 Ω 3 Vp-p/50 Ω 1 Hz to 100 kHz (variable) (W)262 mm × (D)333 mm × (H)74 mm / 2.5 kg Digital delay generator DG645 The DG645 is a general-purpose delay generator that matches the streak camera timing with the pulsed laser timing, mainly for slower streak times. Synchronous delay generator C10647-01 When using a Ti-Sapphire laser in conjunction with a pulse picker, this unit generates low-jitter trigger signals synchronized with the laser repetition rate. Type number Type number Input signal frequency Input signal level Impedance Input signal frequency TRIG.IN Input signal level Impedance Output signal level OUTPUT A Impedance OUTPUT B, C, D Output signal level Impedance Mode-lock IN Operation mode Dimensions / weight C10647-01 10 MHz to 200 MHz 0 dBm to 15 dBm 50 Ω 0 MHz to 16 MHz +0.25 V to +3 V 50 Ω / High Z (10 kΩ) 2V 50 Ω 2.5 V 50 Ω Internal, External, Dump (W)333 mm × (D)262 mm × (H)74 mm / 3.2 kg Number of output channels Output level Variable delay range Delay resolution Internal delay time Repetition rate Jitter Interface Dimensions / weight DG645 4 ch (AB, CD, EF, GH output terminal) 0.5 V to 5.0 V / 50 Ω 0 ps to 2000 s 5 ps 85 ns Single to 10 MHz < 25 ps rms GPIB/RS-232C (W)216 mm × (D)330 mm × (H)89 mm / 4.1 kg Other Other peripheral devices may also be available. Please feel free to consult with HAMAMATSU. 7 Dimensional outlines (Unit : mm) Operating principle Streak camera main unit C10910 (Approx.19.0 kg Main unit only) Input optics A1976-01 225±1 Sweep unit OPERATING PRINCIPLE Function expansion unit Output optics A11695-01 Sweep circuit Trigger signal Readout camera ORCA-R2 C10600-10B Sweep electrode (where electrons are swept in the direction from top to bottom) Streak image on phosphor screen Lens 160±1 305±1 Optical intensity Space Time Incident light 300±1 40.8±3 620±1 Time Slit Photocathode (light electrons) 48±5 Power supply unit C10910 (Approx. 5.9 kg) POW 230±3 292±3 4±2 123.5±2 C10910 28±2 250±3 308±3 Main unit C10910 + Spectroscope + Mount table 50±0.3 40±0.5 6-M6 Installation hole 300±0.3 450±0.3 200±0.3 470±1 SLIT 300±0.5 100±0.3 Accelerating electrode (where electrons are accelerated) MCP (which multiplies electrons) Phosphor screen (electrons light) Space The intensity of the incident light can be read from the brightness of the phosphor screen, and the time and space from the position of the phosphor screen. The light pulse to be measured is projected onto the slit and is focused by the lens into an optical image on the photocathode of the streak tube. Changing the temporal and spatial offset slightly each time, four light pulses, each with a different light itensity, are introduced through the slit and conducted to the photocathode. Here, the photons are converted into a number of electrons proportional to the intensity of the incident light. The four light pulses are converted sequentially to electrons which are then accelerated and conducted towards the phosphor screen. As the group of electrons created from the four light pulses passes between a pair of sweep electrodes, a high voltage is applied (see above), resulting in a high-speed sweep (the electrons are swept in the direction from top to bottom). The electrons are deflected at different times, and at slightly different angles in the perpendicular direction, and are then conducted to the MCP (micro-channel plate). As the electrons pass the MCP, they are multiplied several thousands of times and are then bombarded against the phosphor screen, where they are converted back into light.The fluorescence image corresponding to the first incident light pulse is positioned at the top of the phosphor screen, followed by the others, with images proceeding in descending order; in other words, the axis in the perpendicular direction on the phosphor screen serves as the temporal axis. The brightnesses of the various fluorescence images are proportional to the intensities of the corresponding incident light pulses. The positions in the horizontal direction on the phosphor screen correspond to the positions of the incident light in the horizontal direction. THE PRINCIPLE OF PHOTON COUNTING INTEGRATION 10±1 Photoelectrons given off from the photocathode of the streaktube are multiplied at a high integration rate by the MCP, and one photoelectron is counted as one intensity point on the phosphor screen. A threshold value is then used with this photoelectron image to clearly separate out noise. 1090±1 Photon counting integration C10910 200±1 345±2 Separation of photoelectron image and noise A/D conversion value Photoelectron image Threshold value Signal output from CCD camera Noise Time (wavelength) 0ps 200ps 400ps 600ps 800ps 1ns 1.2ns 1.4ns 1.6ns 1.8ns Light source: PLP (λ =800 nm) Integration time: 1 min Positions in the photoelectron image which are above the threshold value are detected and are integrated in the memory, enabling noise to be eliminated completely. This makes it possible to achieve data measurements with a high dynamic range and high S/N. ★ ORCA is registered a trademark of Hamamatsu Photonics K.K. ★ Product and software package names noted in this documentation are trademarks or registered trademarks of their respective manufacturers. ● ● Subject to local technical requirements and regulations, availability of products included in this promotional material may vary. Please consult your local sales representative. Information furnished by HAMAMATSU is believed to be reliable. However, no responsibility is assumed for possible inaccuracies or omissions. Specifications and external appearance are subject to change without notice. © 2014 Hamamatsu Photonics K.K. HAMAMATSU PHOTONICS K.K. www.hamamatsu.com HAMAMATSU PHOTONICS K.K., Systems Division 812 Joko-cho, Higashi-ku, Hamamatsu City, 431-3196, Japan, Telephone: (81)53-431-0124, Fax: (81)53-435-1574, E-mail: [email protected] U.S.A.: Hamamatsu Corporation: 360 Foothill Road, Bridgewater, N.J 08807, 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)8152-265-8 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, UK, Telephone: (44)1707-294888, Fax: (44)1707-325777 E-mail: [email protected] North Europe: Hamamatsu Photonics Norden AB: Torshamnsgatan 35 16440 Kista, Sweden, Telephone: (46)8-509-031-00, Fax: (46)8-509-031-01 E-mail: [email protected] 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] Cat. No. SHSS0016E08 AUG/2014 HPK Created in Japan