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
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Auto-Fluorescence Microscope
Confocal Raman Microscope
Spinning Disk Confocal Microscope
Industry Line Scan Confocal Microscope
Research Line Scan Confocal Microscope
Laser Point Scanning Confocal Microscope
TCSPC System for SPAD (APD) Testing
Maskless Lithography UV Laser Writer
Laser Doppler Vibrometer 0.1Hz to 5Mhz
OCT Imaging System
NEW Product
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)
FT Infrared Spectrometer(900-16000nm)
Hyperspectral Camera (220nm-4.2μm)
Monochromator & Spectrograph
Single Photon Detector (SPD)(200-1700nm)
Photomultiplier Tubes (PMT)(160-900nm)
Photodiode Detector (PD) (200nm-12um)
Pyroelectric Infrared Detectors (2-12um)
Single-Photon Avalanche Diode Array
IR Beam Profiler
Terahertz Beam Profiler
Scanning Slit Beam Profiler
UV-VIS Beam Profiler(190-1100nm)
Infrared Beam Profiler(350-1750nm)
Compact Beam Profiler(190-1100nm)
Photodiode Power Sensors 250-2500nm
Power Meter Console
Integrating Spheres (10mm-100mm)
Power Meter Adaptor & Accessories
Thermoelectric laser power meter(0.19-25 μm)
Photoelectric laser power meter(200-1100nm)
VUV/UV Spectrograph
1/8m Monochromator/Spectrograph
1/2m&1/4m Monochromator/Spectrograph
Monochromator Accessories
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-Channel Lasers (405-640 nm)
CW Narrow Linewidth Diode Lasers (532-1064 nm)
Nanosecond Pulsed Laser (266nm-3.4μm)
DFB/FP Picosecond Laser (370-1550nm)
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
Short-pulse OPA (650 - 2600nm)
Femtosecond OPA (650 - 2600nm)
Broadband Femtosecond Laser 950-1150nm
Erbium Doped Fiber Amplifier
Ytterbium Doped Fiber Amplifier
Thulium-Doped Fiber Amplifier
Semiconductor Optical Amplifier
Fiber Raman Amplifier
EUV Light Sources(58-130nm)
VUV Light Sources(115-400nm)
ASE Light Sources (830-2000nm)
Microscopy Imaging LED Sources 360-780nm
Collimated LED Sources (240-980nm)
Fiber-Coupled LED Sources (265-940 nm)
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 (4-17um)
Fluorescence Upright / Inverted Microscope
Biological Upright / Inverted Microscope
Phase Contrast Microscope
Dark Field Microscope
Polarizing Microscope
Metallographic Upright / Inverted 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)
High-Speed sCMOS Camera
High Sensitivity sCMOS Camera
38M Pixel large Format sCMOS Camera
Compact BSI/FSI sCMOS Camera
Intensified CMOS Camera (200-1100nm)
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)
Solar Blind UV Imaging Module 240-280nm
UV-VIS Online Monitoring Module
UV-VIS Dual Channel Camera
UV-VIS-IR Triple Spectral Fusion Camera
Ultraviolet Camera for Drone
Free Space Acousto-Optic Modulators (AOM)
Fiber Coupled Acousto-Optic Modulators
Free Space Acousto-Optic Tunable Filter
Fiber-coupled Acousto-optic Tunable Filter
Acousto-Optic Q-switch (AOQ)
Acousto-Optic Frequency Shift (AOFS)
Electro-optical Amplitude Modulator
Electro-optic Phase Modulator
Ultra-fast Pulse Generator for TCSPC
Single-photon time counter
ID1000 Timing Controller
Phase Spatial Light Modulator
Transmission Amplitude SLM
Reflection Amplitude SLM
Digital Micromirror SLM
Pulsed Voltage
Pulsed Current
General Purpose Pulse Generators
Medium and High Voltage Pulse Generators
High Speed Impulse Generator
Very High Speed Pulse Generators
Function Generators
Pulse Amplifiers
Single-channel Lock-in Amplifier
Dual-channel Lock-in Amplifier
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 Filters Fluorescence Microscope
Filters for Raman Spectroscopy
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Filters for FISH
Filters for TIRF Microscope
Filters for FRET Microscope
Laser Crystals
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Optical Crystals
Electro-optical Crystals
Micro-Channel Plate (MCP)
Micro-Channel Plate Assembly (MCP)
Fiber Optic Plates (FOP)
Micro Pore Optics
X-Ray Collimators
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Electrically Adjustable Optical Delay Line
Manually Adjustable Optic Delay Line
Optical Circulator
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Single Axis Motorized Piezo Stage
XY Motorized Piezo Stages
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Nano Electric Actuator
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XYZ 3 Axis Stepper Motor Stages
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FWR Motorized filter wheels
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25mm Linear Stages
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Solid Vibration Isolation Optical Table
Solid Vibration Isolation Table
Pneumatic Optical table
Pneumatic Optical Table With Pendulum Rod
Honeycomb Optical Breadboard
Lens Mounts
Mirror Mounts
Filter Mounts
Time-Resolved iCMOS
The TRiCAM is an intensified CMOS camera for scientific and industrial applications that require 1) low-light level imaging, 2) ultra-short exposures through fast gating, and/or 3) frequency domain imaging using lock-in detection. The TRiCAM features a fast CMOS sensor that is fiber-optically coupled to an image intensifier for optimal transmission efficiency. The high sensitivity of the TRiCAM, down to the single photon level, is supplemented with an acquisition speed up to 162 fps.
For time-domain imaging the iCMOS is equipped with an integrated timing pulse generator and gate-unit (TRiCAM G). The TRiCAM G includes the LI-Capture software for control of gate width, gate frequency, delay, gain and binning. Two synchronised TTL output signals (output A and B) are provided for driving pulsed lasers or LEDs.
For frequency domain imaging the iCMOS supports gain modulation of 120 MHz (standard) and higher (external signal generator). This is the TRiCAM M model. Modulation is provided by a single-chip digital synthesizer to ensure a very low phase noise. The TRiCAM is the key component of the Lambert Instruments LIFA system for FLIM.
The TRiCAM is highly customizable and can be equipped with the image intensifier that best matches your application. Different camera models covering a range in spectral sensitivity, phosphor, spatial resolution, gain, linearity, minimum gate width and gating frequency are available.
Features
● High-resolution image intensifiers
Image intensifiers offering the world’s highest resolution and sensitivity in the
UV, Visible or Near Infrared
● Small gate widths
Down to less than 3 ns (FWHM) with minimal jitter
● Single-chip digital synthesizer for frequency-domain acquisition
For high dynamic range fluorescence lifetime imaging at the lowest possible
phase noise
● Compact camera design
For an easy fit to a microscope body or imaging spectroscope
● LI-Capture software
For complete camera control; the SDK enables integration with third-party
software
Applications
● Time-resolved imaging and spectroscopy
● Particle Image Velocimetry (PIV)
● Laser Induced Fluorescence (LIF)
● Time-gated luminescence
● Fluorescence Lifetime Imaging Microscopy (FLIM)
● Förster Resonance Energy Transfer (FRET)
● Oxygen imaging
● Viscosity imaging
● Single molecule imaging
● Bio- and Chemiluminescence Imaging
● Solar PV and LED characterization
● Combustion
● Time-gated Raman
● Plasma physics
● X-ray Imaging
For time-resolved imaging the image intensifier is used as an electro-optical shutter during the process of image acquisition. This uses either a signal generated by the gate unit and timing unit (e & f - the TRiCAM G model) or a high-frequency modulation signal (g - the TRiCAM M model) provided by a direct digital synthesizer. The camera provides multiple output signals (h) for accurate synchronization of external equipment such as a pulsed light source.
Figure caption: a) lens mount, b) image intensifier, c)fiber-optic taper, d) CMOS camera module, e) gate unit, f) timing unit, g) intensifier modulation input, h) output synchr. gate pulses.
Spectral Response and Phosphor Decay Time
The TRiCAM has a built-in image intensifier that boosts the incoming light. This way, you can capture detailed images in the most challenging light conditions.
Our experienced engineers will help you pick the right image intensifier for your application.
Image intensifiers
An image intensifier boosts the intensity of the incoming light.
By converting photons to electrons and back to photons, the
light intensity can be increased significantly. Another feature of
an image intensifier is that it can act as an ultra-fast shutter.
Photocathodes
The photocathode is the entrance of the image intensifier.
This is where the incoming photons are converted to electrons.
The quantum efficiency of the photocathode material specifies
how efficient this conversion is for each wavelength.
TRiCAM G
Gated Image Intensifier
TRiCAM M
Modulated Image Intensifier
TRiCAM GM
Gated and Modulated intensifier
Product specifications and Brochures
Product Brochure Link:
Max. frame rate at full resolution
72 dB
162 fps
Integration time control
14 eˉ
0.005 ms – 3.2 s
Input diameter
Single-stage MCP Gen II or Gen III (filmless)
18 mm
TRiCAM M: S20, S25, GaAs, GaAsP (blue curves graph Overview)
TRiCAM G: P20,P24,P43,P46; TRiCAM M: P43
S20: 0.006 photo eˉ/pix/s, S25: 0.008 photo eˉ/pix/s,
GaAs: 0.024 photo eˉ/pix/s, GaAsP: 0.006 photo eˉ/pix/s
Gating
The TRiCAM G can be used as an ultra-fast electro-optical shutter by gating the image intensifier and thereby reducing the effective exposure time. Time domain gating eliminates motion blur and significantly widens the range of light levels at which the camera can be used.
The user has full control of the camera gate pulse width, delay and gain through either the dedicated LI-Capture software or the software SDK. The software supports an array of gating modes, including synchronization of the internal oscillator to an external source. The standard camera has two additional output channels (output A and B) synchronised with the gate frequency. For both channels the user has control of the delay time as well as the pulse width and polarity.
For the TRiCAM M model the camera modulation signal at frequencies below 100 kHz can be produced using the optional gate unit and timing pulse generator. The pulse generator also generates the synchronisation signal for a modulated light source or acousto-optic modulator.
Gen III: 5 ns
The TRiCAM M provides highly accurate frequency-domain imaging with high-resolution gain modulated Gen II and Gen III image intensifiers.
The TRiCAM M combines the ICMOS camera with a separate modulation control unit. The modulation control unit contains a single-chip dual channel DDS for generation and amplification of the RF modulation signals for the modulated lightsource and the image intensifier (100 kHz – 120 MHz standard). The control unit further supplies the required high-voltages to the image intensifier. A software SDK is provided for digital control of the gain, modulation and cathode bias voltages via an USB interface, emulating a standard RS232 serial communicationsport.
Modulation frequencies below 100 kHz are supported by the optional gate unit and time pulse generator. The pulse generator generates the synchronisation signal for an external modulated light source or acousto-optic modulator.
Programmable options:
AC signal level (DC current adjust)
AC signal level (DC level adjust)
Trigger input
Monitor Output
Gate delay time control
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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