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Auto-Fluorescence Microscope
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Industry Line Scan Confocal Microscope
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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
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Hyperspectral Camera (220nm-4.2μm)
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Time-Resolved Imgae Intensifier
The TRiCATT is a compact lens-coupled image intensifier 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 TRiCATT features an 18 or 25 mm image intensifier with a highly efficient relay lens that can be matched to any CCD or CMOS camera, resulting in a flexible solution that can easily be integrated in an existing imaging system.
The TRiCATT (Time Resolved intensified Camera Attachment) is the best choice for ultra-fast imaging in the time domain and/or frequency domain.
With a wide range of Gen II and Gen III image intensifiers, the TRiCATT offers high sensitivity down to single photon level and the optimal spectral bandwidth for your application. Different models covering a range in spectral sensitivity, phosphor, spatial resolution, gain, linearity, minimum gate width and gating frequency are available.
For time-domain imaging the intensifier is equipped with a fast gate unit (TRiCATT G40n/G2n) that enables the intensifier to operate as an electro-optical shutter. The gate unit can be operated up to repetition rates of up to 2.5 MHz in burst.
A series of different intensifier control units provide functionality ranging from analog gain control to full digital control including an internal trigger generator and programmable gate trains.
For frequency-domain imaging the TRiCATT M supports gain modulation of 120 MHz (standard) and higher (external signal generator). Modulation is provided by a single-chip digital synthesizer to ensure an extremely low phase noise.
● 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
Gate width down to less than 3 ns (FWHM) with minimal jitter
● High gate repetition rates up to 300 kHz/2.5 MHz burst
● Compact design for an easy fit to your imaging or spectroscopy setup
● Overexposure protection User-definable current limitation and optional shutter
● Easy coupling
Flexible and efficient lens coupling to any CCD and CMOS camera (up to 500 fps)
● 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, a gate unit (e) is used together with the image intensifier to yield an electro-optical shutter. The gate unit either generates a high voltage pulse signal or follows an external TTL pulse. The pulse width is variable and follows a TTL input pulse over the range from less than 3 ns to DC at a repetition rate up to 300 kHz.
TRiCATT 25
Single-stage intensifier attachment
25 mm image intensifier Gated or modulated
F-mount and C-mount
TRiCATT 18
18 mm image intensifier Gated or modulated
TRiCATT 18C
Compact single-stage intensifier attachment
C-mount
Product specifications and Brochures
Product Brochure Link:
Image intensifier
Input window
TRiCATT G 40n: 40 ns
TRiCATT G 2n: < 3 ns with Gen II, 5 ns with Gen III
TRiCATT G 2n: 300 kHz, 2.5 MHz in burst mode
Photocathode
0.006
e/px/s
2x10-11
lm/cm2
2*10-11
3*10-23
Lens coupling/output flange
1:1 C-mount
2:1 C-mount
1:1; 2:1; 3:1 F-mount on reques
1:1 F-Mount
2:1 F-mount
3:1 F-mount
Gating
The TRiCATT G can be used as an ultra-fast electro-optical shutter by gating the image intensifier. This eliminates motion blur and reduces the effective exposure time, thereby significantly widening the camera dynamic range. To prevent loss of intrascene dynamic range when using a shorter gate the user can set a higher MCP gain. The pulse width and frequency are user defined: any pulse width from DC down to a few nanoseconds can be applied.
The table below summarizes the range of different intensifier control units available with the TRiCATT G. The gain-control models act as a power supply for the image intensifier, gate pulse trains are supplied externally. The gate-control model has its own pulse generator, giving the user direct control of the gate width and gate delay. The gate-generator models have an enhanced version of the pulse generator with lower jitter. These models allow the image intensifier to be synchronized to the exposure time of the camera by supplying a trigger signal. All models allow the gate frequency to be set by an external TTL signal.
The enhanced pulse generator of the gate-generator models has 4 independent programmable pulse outputs (one of which is used for gating) that provide precise timed TTL pulses with pulse widths down to less than 3 ns (FWHM).
Intensifier Gain
Control
Intensifier Gate
Generato
Gain control
Resulting min pulse width (increments)
Pulse repetition rate
Insertion delay
Programmable trigger level,
divider and bursts
(m out of n triggers)
Modulation control unit
The TRiCATT M provides highly accurate frequency-domain imaging with high-resolution gain modulated Gen II and Gen IIIimage intensifiers.
The TRiCATT M combines the image intensifier with a separate modulation control unit. The modulation control unit contains a single-chip dual channel DDS for generation and amplification of two RF modulation signals, one for the modulated lightsource or acousto-optic modulator (AOM) and one for the image intensifier (100 kHz – 120 MHz standard). The control unit further supplies the high-voltage for 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 RS-232 serial communications port.
Modulation frequencies below 100 kHz are supported by the optional gate unit and pulse generator. This also produces the synchronization signal for an external modulated light source or AOM.
TRiCATT M
Frequency range
100 kHz–120 MHz (standard)
Up to at least 250 MHz with an external signal generator
Frequency deviation
Harmonics suppression
High light level protection
Output 1. TRiCATT
AC signal level
AC signal after amplification
Output 2. Lightsource
Programmable options:
a) Multi-LED
DC current adjust
b) Modulated laser diode
DC level adjust
c) AOM for CW laser
Frequency
Modulation input
Trigger input
Monitor output
Min. gate width (FWHM)
Gate pulse width control
Gate delay time control
Dead time after trailing edge
Pulse generator resolution ; jitter
Mechanical Shutter
The TRiCATT can be supplied with an optional mechanical shutter for preventing damage to the image intensifier by high intensity stray light or direct laser light. It is further recommended to close the shutter between measurements to increase the lifespan of the image intensifier.
The shutter is encased in an aluminum housing with a standard F-mount input that replaces the original F-mount adapter of the TRiCATT. The back focal distance of the F-mount input is unchanged, so any F-mount objective can be used. The shutter comes with a power supply and a remote control. A timer can be used to automatically close the shutter after a predetermined time. The remote control has an ergonomic design and a large LCD screen.
The shutter can also be controlled by the Windows software of the TRiCATT or by an external TTL signal.
Shutter control via
- Hand-held remote control with push-button and timer
- External TTL signal
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.
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%
S20 : 14800, S25:30000GaAs: 40000, GaAsp: 20000
Microscop Cameras
Scientific Cameras
Short-wave, Mid-wave, Long-wave Infrared Cameras
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