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 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 (400-850nm)
Spectrophotometer (240-2150nm)
Single Photon Counting Imager
Visible Single Photon Detector(SPD)
Infrared Single Photon Detector(SPD)
Photodiode & Photomultiplier (200nm-12um)
Pyroelectric Infrared Detectors (2-12um)
Standard Beam Profiler (190-1100nm)
1inch Aperture Beam Profiler (190-1100nm)
SWIR Beam Profiler (900-1700nm)
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
Options and Accessories
Autocorrelator - Single Shot
Autocorrelator - Multi Shot
FROG - Single Shot
FROG - Multi Shot
LIV Test Systems for Laser Diode / LED
Optical Test Measurement System
RF Test Measurement System
CW Pigtail Laser Diode (400-1920nm)
CW Laser Diode Module (375-785nm)
CW Triplex Fiber Coupled Laser Diode (RGB)
DPSS Nanosecond Pulsed Lasers
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 Single Mode Fiber Laser (405nm - 2um)
CW Narrow Linewidth Lasers (1530nm-2un)
C-Band Tunable Laser (1529 -1567nm)
L-Band Tunable Laser (1554 -1607nm)
2 Micron Tunable Laser (1900-2050nm)
Supercontinuum Fiber Lasers 450-2300nm
Broadband Femtosecond Laser 950-1150nm
Erbium Doped Fiber Amplifier
Ytterbium Doped Fiber Amplifier
Thulium-Doped Fiber Amplifier
Fiber Raman Amplifier
Microscope Light & Lamp (185 - 5500nm)
Single Wavelength LED Source(240-980nm)
Multi-wavelength LEDs Source (240-980nm)
ASE/SLD Light Sources (1250-2000nm)
IR Emitter Chip (2-14um)
Light Field Sythesizer
White Light Interferometer
CRD Loss Meter and Reflectometer
Hollow-Core Fiber Compressor
High Powered Hollow-Core Fiber Compressor
Ultra-High Contrast 3rd-Order Autocorrelator
Terahertz Quantum Cascade Lasers(1-4.5Thz)
CW LWIR Quantum Cascade Lasers (10-17um)
Raman Microscope
Smart 3D Stereo Microscope
USB Digital Microscope With Platform
Microscope CCD Camera (VIS-NIR)
Microscope CMOS Camera (UV-NIR)
UV & NIR Enhanced CMOS Camera
Snapshot Hyperspectral Camera for Microscope (450-950nm)
Microscope Light & Lamp
Soft X-Ray BSI sCMOS Camera (80-1000eV)
XUV/VUV CCD Cameras (1-350nm)
UV-NIR sCMOS Camera (200-1100nm)
Intensified CMOS Camera (200-1100nm)
Imaging Intensifier Tube
HDMI Color CMOS Camera (Monitor)
Infrared Pyrometers (-40-3000C)
Infrared linear Array Camera
Infrared Matrix Array Cameras
Blackbody Calibration Sources -15 to 1500°C
Hyperspectral Camera LineScan (0.22-4.2um)
Hyperspectral Camera SnapShot(0.35-1um)
Optical Coherence Tomography (OCT)
Short-Wave Infrared Camera (SWIR)
Mid-Wave Infrared Camera (MWIR)
Long-Wave Infrared Camera (LWIR)
Ultra-fast Pulse Generator for TCSPC
ID900 Timing Controller
ID1000 Timing Controller
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
Neutral Density Filters
Bandpass Filters
Edgepass Filters
Birefringent Filters
Fluorescence Filters
Laser Crystals
Nonlinear Optical Crystals
Birefringent Crystals
Optical Crystals
Electro-optical Crystals
Lens Mounts
Mirror Mounts
Filter Mounts
Manual Stages
Piezo Stages
Multi-Axis Stages
Solid Vibration Isolation Optical Table
Solid Vibration Isolation Table
Pneumatic Optical table
Pneumatic Optical Table With Pendulum Rod
Honeycomb Optical Breadboard
GLACIER-C
The GLACIER-C is a further development of our successful GLACIER reflectometer. The GLACIER
allows for measurement of losses of optical coatings down to 5 ppm using the extreme sensitive
cavity ring-down spectroscopy method. It is therefore often used to characterize highly reflective
mirrors where conventional reflection and absorption measurements are insufficient. The new
innovation of the GLACIER-C device is the employment of a super-continuum laser source in
combination with a tunable monochromator. This allow for a freely electable wavelength within 450nm
and 2000 nm and thus offer an unprecedented flexibility as it is not limited to available diode laser
wavelengths. The GLACIER-C combines the unrivalled sensitivity of the GLACIER system with an
unrivalled flexibility creating the most powerful deviceon the market. The device features high-speed
data acquisition and allows to record measurements within seconds. Easy and fast change of
wavelength is facilitated through the user friendly software and easy change of optics on kinematic
mounts.
Key Product Features
Reflectivity measurements up to 99.9995%
Various angles of incidence: 5°-45° (and 0°)
S and p polarization (separately)
Antireflective coating characterization down to 0.0005% (5 ppm)
Simple and reproducible alignment for 0.5”, 1” and 2” optics
Spring-loaded mirror fixtures for reproducible mounting without strain
Computer and user-friendly software interface included
High-speed data acquisition and real-time analysis
Super-continuum laser source and tunable monochromator. Easy and fast change of wavelength
Freely selectable wavelength: 450-2000 nm
Footprint 90 x 55 cm²
Working Principle
The principle of reflectivity/loss measurements with cavity ring-down spectroscopy is based on very low losses at each mirror bounce. Pulses travelling inside a cavity
experience optical losses over and over again during each round trip. The device measures the time-dependent intensity I(t) leaked through an end mirror of the cavity
(center). The signal decays with a time constant depending on the intra-cavity losses.
Sketch of the working
principle of our cavity
ring-down device
including measurement
and fitting procedure
ght Source
The source consists of a super-continuum laser source
and a monochromator. The monochromator is tunable
as it employs Acousto Optic Tunable Filters (AOTF).The
monochromator comes with two AOTF crystals each
active in separate broad wavelength ranges. The choice
of crystals defines the available wavelengths and can be
chosen from seven different crystals as to fit individual
requirements.
Example 1: 640 nm – 1100 nm & 1200 nm – 2000 nm
Example 2: 450 nm – 650 nm & 800 nm – 1400 nm
The figures to show three typical measurements of high
reflective samples and measurement of an empty cavity
(at 1417 nm) where humidity in the cavity causes extra
losses. All measurements are recorded on the same
GLACIERC device demonstrating the wavelength
flexibility. The loss measurements are realized through
a comparison of measurements of cavity losses with and
without the test sample.
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Company
Light Analysis
Microscope
Light Sources
Imaging
Optics