Raman Spectrometer 532/785/1064nm
Standard Spectrometer 200-1100nm
High Sensitivity UV Enhanced Spectrometer
BSI Cooled High Sensitivity Spectrometers
Large NA High QE Spectrometer 200-1450nm
Near Infrared Spectrometer 900-2500nm
More
Laser Point Scanning Confocal Microscope
Laser Line Scan Confocal Microscope
Spinning Disk Confocal Microscope
Structured Illumination Microscope
Raman Microscope Wide Field
Fluorescence / PL Microscope
TCSPC System for SPAD (APD) Testing
Maskless Lithography UV Laser Writer
Laser Doppler Vibrometer 0.1Hz to 5Mhz
OCT Imaging System
X-ray/XRD Heating & Cryo Stage
Optical Heating & Cryo Stage
Electrical Probe Temperature Stage
Adjustable Electrical Probe Station
Tensile Strain Temperature Stage
Fiber Spectrometers (200nm to 5um)
X-Ray/XUV/VUV Spectrometers (1-300nm)
Hyperspectral Camera (220nm-4.2μm)
Multi-Spectral Camera (400-1000nm)
Spectrophotometer (240-2150nm)
Photomultiplier Tubes (PMTs)
Visible Single Photon Detector(SPD)
Infrared Single Photon Detector(SPD)
Photodiode PD (200nm-12um)
Pyroelectric Infrared Detectors (2-12um)
IR Beam Profiler (2-16um)
Terahertz Beam Profiler(1-18 THz)
Scanning Slit Beam Profiler (190-2500nm)
Photodiode Power Sensors 250-2500nm
Power Meter Console
Integrating Spheres (10mm-100mm)
Power Meter Adaptor & Accessories
1/8m Monochromator/Spectrograph
1/2m&1/4m Monochromator/Spectrograph
Monochromator Accessories
Filter & Wheel
LIV Test Systems for Laser Diode / LED
White Light Interferometer
Optical Coating CRD Reflectrometer
Optical Test Measurement System
RF Test Measurement System
CW Pigtail Laser Diode (400-1920nm)
CW Laser Diode Module (375-785nm)
CW Multi Wavelength Laser
DPSS Nanosecond Pulsed Lasers
DFB/FP Picosecond Laser (370-1550nm)
High-Power Femtosecond Solid-State Lasers
Nanosecond Pulse Fiber Laser(1064-2um)
Picosecond Pulse Fiber Laser (515nm - 2um)
Femtosecond Pulse Fiber Laser 780nm-2um
CW Fiber Laser System (405nm - 2um)
CW Narrow Linewidth Lasers (1530nm-2um)
C-Band Tunable Laser (1529 -1567nm)
L-Band Tunable Laser (1554 -1607nm)
Supercontinuum Fiber Lasers 450-2300nm
Femtosecond OPA(650 - 2600nm)
Short-pulse OPA(650 - 2600nm)
Broadband Femtosecond Laser 950-1150nm
Erbium Doped Fiber Amplifier
Ytterbium Doped Fiber Amplifier
Thulium-Doped Fiber Amplifier
Fiber Raman Amplifier
Semiconductor Optical Amplifier (SOA)
Microscope Light & Lamp (185 - 5500nm)
Single Wavelength LED Source(240-980nm)
Multi-wavelength LEDs Source (240-980nm)
ASE Light Sources (830-2000nm)
IR Emitter Chip (2-14um)
Light Field Sythesizer
Hollow-Core Fiber Compressor
High Powered Hollow-Core Fiber Compressor
Ultra-High Contrast 3rd-Order Autocorrelator
Coherent Ultrabroadband XUV Light Source
Enhanced Cavities for Laser Light
Terahertz Quantum Cascade Lasers(1-4.5Thz)
CW IR Quantum Cascade Lasers(3-12μm)
CW LWIR Quantum Cascade Lasers (10-17um)
Raman Microscope
Fluorescence Microscope
Biological Microscope
Phase Contrast Microscope
Dark Field Microscope
Polarizing Microscope
Metallographic Microscope
Smart 3D Stereo Microscope
USB Digital Microscope With Platform
Built-in Digital Microscope
Plan Apochromatic Objective
Industrial Plan Objective
Biology Plan Objective
Microscope CCD Camera (VIS-NIR)
Microscope CMOS Camera (UV-NIR)
UV & NIR Enhanced CMOS Camera
Hyperspectral Camera for Microscope
Multispectral Camera For Microscope
Microscope Light & Lamp
Soft X-Ray BSI sCMOS Camera (80-1000eV)
UV-NIR sCMOS Camera (200-1100nm)
Intensified CMOS Camera (200-1100nm)
Imaging Intensifier Tube
Full Frame CCD Camera for UV VIS NIR
Full Frame CCD Camera for VUV EUV X-ray
Full Frame In-vacuum CCD Cameras
Large Format In-vacuum CCD Cameras
HDMI Color CMOS Camera (Monitor)
High Speed Line Scan Camera
Large Format Camera
High Speed Large Format Camera
Frame Grabber
Infrared Pyrometers (-40-3000C)
Infrared linear Array Camera
Infrared Matrix Array Cameras
Blackbody Calibration Sources -15 to 1500°C
Short-Wave Infrared Camera (SWIR)
Mid-Wave Infrared Camera (MWIR)
Long-Wave Infrared Camera (LWIR)
Hyperspectral Camera LineScan (0.22-4.2um)
Hyperspectral Camera SnapShot(0.35-1um)
Optical Coherence Tomography (OCT)
Ultra-fast Pulse Generator for TCSPC
Multi-Channel Single Photon Counting Device
ID1000 Timing Controller
Photodetectors
General Purpose Pulse Generators
Medium and High Voltage Pulse Generators
High Speed Impulse Generator
Very High Speed Pulse Generators
Function Generators
Pulse Amplifiers
Pulsed Voltage
Pulsed Current
Phase Modulator
Amplitude Modulator
Education Kits
Acousto-Optic Modulators (AOM)
Acousto-Optic Tunable Filter (AOTF)
Acousto-Optic Deflector (AODF)
Acousto-Optic Frequency Shift (AOFS)
Phase Modulators
Acousto-optic Q-switch (AOQS)
TPX / HDPE Terahertz Plano Convex Lens
Off-Axis Parabolic Mirrors
Terahertz Hollow Retro Reflector
Terahertz Metallic Mirrors
ZnTe / GaSe Terahertz Crystals
Terahertz Beam Expander Reflection
Waveplates
Optical Isolator
Optical Polarizers
Beamsplitter Plate
Beamsplitter Cube
Dichroic Beamsplitters
Ultrathin Beamsplitter Plate
Bandpass Filter Fluorescence Microscope
Filter for Raman Spectroscopy
Narrow BandPass Filters for Laser
Filter for FISH
Filter for TIRF Microscope
Filter for FRET Microscope
Laser Crystals
Nonlinear Optical Crystals
Birefringent Crystals
Optical Crystals
Electro-optical Crystals
Micro-Channel Plate (MCP)
Micro-Channel Plate Assembly (MCP)
Fiber Optic Plates (FOP)
Micro Pore Optics
X-Ray Collimators
Optical Circulator
Filter Coupler
In-line Polarizer/PBC/PBS
WDM/DWDM/CWDM/Bandpass Filter
Faraday Rotator
Lens Mounts
Mirror Mounts
Filter Mounts
13mm Linear Stages
25mm Linear Stages
Rotation and Tilt Stages
Rack and Pinion Stages
Vertical Axis Stages
2-Axis Stages
Solid Vibration Isolation Optical Table
Solid Vibration Isolation Table
Pneumatic Optical table
Pneumatic Optical Table With Pendulum Rod
Honeycomb Optical Breadboard
Single Axis Motorized Piezo Stage
XY Motorized Piezo Stages
Multi Axis Motorized Piezo Stages
XY Microscope Piezo Stages
Vacuum Non-magnetic Piezo Stage
Nano Electric Actuator
High-speed Gated Intensified Camera
The HiCAM is an integrated camera system that was designed for high-speed imaging in low-light conditions. It features a 1.3 megapixel image sensor that captures detailed images at high frame rates of up to 500 fps at full resolution. Reducing the resolution allows for even higher framerates.
A high-quality image intensifier boosts light levels, which offers a unique combination of exposed high-speed recordings in low-light conditions. The dual-stage image intensifier can be equiped with a variaty of photocathodes; ranging from ultraviolet to infrared. And because the image intensifier is fiber-optically coupled, the signal-to-noise ratio of the camera is far superior to a lens-coupled system.
With gating, the image intensifier is used as an ultra high speed shutter, reducing the effective exposure time. This enables time-resolved filtering and also eliminates motion blur. The fanless design of the camera minimizes vibrations to ensure sharp images.
Data can either be temporarily stored in the built-in memory of the HiCAM 500 or streamed directly to a frame grabber by the HiCAM 500S. Camera control and data download is done over a gigabit ethernet connection using the bundled software. Intensifier gain and gating are also configurable from the software.
● High resolution image intensifiers
Gen II and Gen III image intensifiers offering the world’s highest resolution and sensitivity in the
UV, visible or near infrared.
● Small gate widths
Down to 40 ns (FWHM) with minimal jitter.
● High gate repetition rates
Up to 100 kHz.
● Compact design
For an easy fit to your imaging or spectroscopy setup.
Applications
● Combustion research
● Plasma physics
● Time-resolved fluorescence
● Dynamic phenomena in microscopy
● Laser Induced Fluorescence (LIF)
● Particle Image Velocimetry (PIV)
● Micro-fluidics
● Blood-flow analysis
The number of dark spots, exceeding a contrast with their surrounding area of 20%, is less than or equal to the number indicated below. The size of non-circular spots is determined on the basis of equal area to circular spots. When the distance between two spots is less than the maximum dimension of either spot, the two spots are considered to be one spot. There shall be no bright spots in the active area.
The dark and white spots which exceed a contrast of 30 percent of their surrounding area should not exceed the following values over the guarantee area. Spot size is defined as the diameter of the circle, with an area equal to the area of the spot. N/A denotes 'Not applicable' in the table below.
This cloud of electrons is accelerated towards the anode screen, where the electrons are converted back into photons by the phosphor layer. The second stage of the intensifier (the booster) further increases the light intensity. Finally, the photons are transferred to the sensor by a fiberoptical taper.
Product specifications and Brochures
Product Brochure Link:
Luminous sensitivity (µA/lm)
Min.
Typ.
150
175
500
700
400
800
1000
1200
Gain
1500 ph/ph
3000 lm/m2/lx
2200 ph/ph
7500 lm/m2/lx
2000 cd/m2/lx
3600 lm/m2/lx
5000 cd/m2/lx
11000 lm/m2/lx
20
17
35
50
27
Resolution (lp/mm)
45
56
57
40
EBI (µlx)
Max.
0.1
0.25
0.03
0.3
Input window thickness
Second stage
Photon gain (ph/ph)
Photocathodes
Second generation image intensifiers
The photocathode of a second generation image intensifier can have a quantum efficiency of up to 25%.
S25 photocathodes are only available in the 18 mm diameter image intensifiers.
Typical QE
Typical quantum efficiency (%) of second generation image intensifiers as a function of wavelength (nm).
Second generation high QE image
intensifiers
The photocathode of a second generation high QE image intensifier can have a quantum efficiency of over 30%.
Please note that these image intensifiers are only available with a diameter of 18 mm.
Typical QE, 200 ns gate width
Typical quantum efficiency (%) of second generation high QE image intensifiers as a function of wavelength (nm).
Second generation fast-gated high QE image intensifiers
The photocathode of a second generation high QE image intensifier can have a quantum efficiency of over 25%.
Typical QE, 3 ns gate width
Third generation image intensifiers
The photocathode of a third generation image intensifier can have a quantum efficiency of up to 50%.
Typical quantum efficiency (%) of third generation image intensifiers as a function of wavelength (nm).
Phosphors
Phosphor Decay Time
The anode screen of the image intensifier contains a layer of phosphorescent material. Upon impact of an electron, the phosphor screen will emit light. Depending on the type of phosphor, the intensity of the emitted light will decrease faster. The more efficient the phosphor, the slower its light intensity decays after excitation.
Our time-resolved cameras and camera attachments use P43 phosphor. The high luminous efficiency of this phosphor increases the light levels at the output of the image intensifier. This increases the quality of the resulting image.
Our high-speed cameras and camera attachments use P46 phosphor. This phosphor has a short decay time, so the light signal of consecutive frames doesn't get mixed up.
P47 phosphor is available on request, when even faster decay times are required.
EMISSION
EFFICIENCY (E/KV)
DECAY TO 1%
Microscop Cameras
Scientific Cameras
Intensified CMOS Cameras
Imaging Intensified Tube
S20 : 14800, S25:30000GaAs: 40000, GaAsp: 20000
Short-wave, Mid-wave, Long-wave Infrared Cameras
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Company
Light Analysis
Microscope
Light Sources
Imaging
Optics