FILTER PRODUCTS

heliOptics WLI6
Heliotis AG
The heliInspetTM H6 has been engineered to meet the specifications of the most demanding 3D in-line inspec-tion tasks such as measuringstep heights, angles, shape, roughness, ripple, waviness, defects, scratches, wear off flatness, coplanarity, deformations film thickness (tomographic mode)Benefitting from Heliotis’ long experience ...
  • Interferometer Configuration: Twyman–Green Interferometer
  • Light Source: White Light
  • Output Polarization: Not Specified
  • RMS Repeatability: <0.01 waves
  • RMS Precision: <0.005 waves
Data Sheet
heliInspect H8
Heliotis AG
The new heliInspect™ H8 is the latest addition to Heliotis series of unrivaled optical in-line sensors. At its core, this industry grade White-Light-Interferometer utilizes Heliotis next generation 3D-pixel sensor heliSens™ S4.
  • Interferometer Configuration: Twyman–Green Interferometer
  • Light Source: White Light
  • Output Polarization: Not Specified
  • RMS Repeatability: Not Specified
  • RMS Precision: Not Specified
Data Sheet
Fizeau Interferometers IFV-300 And IFH-300
Armstrong Optical
Newly available from Armstrong Optical are a range of customer-proven phase-measuring Fizeau interferometers with 300mm (12”) aperture in both vertical (downward-looking) and horizontal configurations, IFV-300 and IFH-300. Both configurations are supplied with a certified lambda/20 transmission flat and an ergonomically designed ...
  • Interferometer Configuration: Fizeau Interferometer
  • Light Source: White Light
  • Output Polarization: Not Specified
  • RMS Repeatability: Not Specified
  • RMS Precision: Not Specified
Data Sheet
Fizeau Interferometer IFV-60
Armstrong Optical
Newly available from Armstrong Optical is a customer-proven phase-measuring Fizeau interferometer with 60mm aperture in a vertical (downward-looking) configuration, IFV-60. The aperture can also be increased to 100 if required. It is supplied with a certified lambda/20 transmission flat and an ergonomically designed sample handling ...
  • Interferometer Configuration: Fizeau Interferometer
  • Light Source: White Light
  • Output Polarization: Linear
  • RMS Repeatability: Not Specified
  • RMS Precision: Not Specified
Data Sheet
FDVI Mark IV 3000
Martin Froeschner & Associates
The new M,F& A Mark IV All Fiber Doppler Velocity Interferometer Systems offer enhanced capabilities in the measurement and recording of instantaneous velocity versus time histories. Two versions of the Mark IV Systems are now available. The original Mark IV has been in use all over the world and gives excellent results ...
  • Interferometer Configuration: Not Specified
  • Light Source: White Light
  • Output Polarization: Not Specified
  • RMS Repeatability: <0.01 waves
  • RMS Precision: <0.01 waves
Data Sheet
FiBO 300 Interferometer
Promet Optics
FiBO® 300 is a versatile phase-shifting interferometer for the analysis of fiber optic endface geometry. Measure non-standard, angle-polished and cleaved bare optical fiber with just one click. FiBO makes sophisticated interferometry easy and affordable.
  • Interferometer Configuration: Michelson Interferometer
  • Light Source: 355nm, 532nm
  • Output Polarization: Not Specified
  • RMS Repeatability: Not Specified
  • RMS Precision: Not Specified
Data Sheet
FiBO 250 Interferometer
Promet Optics
FiBO® 250 interferometer is a fully automated solution for fast and accurate fiber optic connector endface testing. 3D surface metrology and advanced defect detection capabilities are combined in one compact and portable system.
  • Interferometer Configuration: Michelson Interferometer
  • Light Source: 532nm, 355nm
  • Output Polarization: Not Specified
  • RMS Repeatability: Not Specified
  • RMS Precision: Not Specified
Data Sheet
FiBO 200 Interferometer
Promet Optics
FiBO® 200 Interferometer is an economical solution for complete and accurate fiber optic connector endface testing. High resolution 3D surface metrology and automated defect detection are combined in one robust, compact system for quick and easy inspection on the production floor or in the field.
  • Interferometer Configuration: Michelson Interferometer
  • Light Source: 532nm, 355nm
  • Output Polarization: Not Specified
  • RMS Repeatability: Not Specified
  • RMS Precision: Not Specified
Data Sheet
DAISI-MT Interferometer
Connected Fibers
Based on the design and philosophy which made the DAISI a success, the DAISI-MT  includes both a white and red ight source, to perform  measurements of end-face geometry of multi-fiber ferrules  and single-fiber connectors on the same system. Its revolutionary design makes it ideal for the use in the ...
  • Interferometer Configuration: Not Specified
  • Light Source: 632 nm or 633nm
  • Output Polarization: Not Specified
  • RMS Repeatability: Not Specified
  • RMS Precision: Not Specified
Data Sheet
3DScope-V2 Interferometer
Connected Fibers
The 3D-Scope v2 is the latest interferometer to be released by Data-Pixel for the use in a production environment. It was designed with speed, precision, simplicity, robustness and cost in mind. Non-compressed, real time and high quality images are transfered from the hardware to the software via a USB2.0 high speed link in ...
  • Interferometer Configuration: Not Specified
  • Light Source: 632 nm or 633nm
  • Output Polarization: Not Specified
  • RMS Repeatability: Not Specified
  • RMS Precision: Not Specified
Data Sheet
DAISI-V2 Interferometer
Connected Fibers
The ultimate production interferometer for measuring end-face geometry on single fiber and MT-RJ connectors, equipped with a revolutionary “no-exterior-moving-parts” mechanical design. DAISI v2 was designed with years of industry feedback in mind in order to satisfy the most demanding requirements for the use in the ...
  • Interferometer Configuration: Not Specified
  • Light Source: 632 nm or 633nm
  • RMS Repeatability: Not Specified
  • RMS Precision: Not Specified
Data Sheet
NSLI-632-2 N-Slit Laser Interferometer
Interferometric Optics
Based on multiple-prism beam expansion and digital detection the N-slit interferometer allows for the rapid interferometric characterization of transmission optical surfaces in general. A significant advance over traditional point-by-point incoherent microdensitometers and point-by-point incoherent microscopes. 
  • Interferometer Configuration: Not Specified
  • Light Source: 632 nm or 633nm
  • Output Polarization: Not Specified
  • RMS Repeatability: Not Specified
  • RMS Precision: Not Specified
Data Sheet
NSLI-632-1 N-Slit Laser Interferometer
Interferometric Optics
Based on multiple-prism beam expansion and digital detection the N-slit interferometer allows for the rapid interferometric characterization of transmission optical surfaces in general. A significant advance over traditional point-by-point incoherent microdensitometers and point-by-point incoherent microscopes. 
  • Interferometer Configuration: Not Specified
  • Light Source: 632 nm or 633nm
  • Output Polarization: Not Specified
  • RMS Repeatability: Not Specified
  • RMS Precision: Not Specified
Data Sheet
NSLI-594-2 N-Slit Laser Interferometer
Interferometric Optics
Based on multiple-prism beam expansion and digital detection the N-slit interferometer allows for the rapid interferometric characterization of transmission optical surfaces in general. A significant advance over traditional point-by-point incoherent microdensitometers and point-by-point incoherent microscopes. 
  • Interferometer Configuration: Not Specified
  • Light Source: 594nm
  • Output Polarization: Not Specified
  • RMS Repeatability: Not Specified
  • RMS Precision: Not Specified
Data Sheet
NSLI-594-1 N-Slit Laser Interferometer
Interferometric Optics
Based on multiple-prism beam expansion and digital detection the N-slit interferometer allows for the rapid interferometric characterization of transmission optical surfaces in general. A significant advance over traditional point-by-point incoherent microdensitometers and point-by-point incoherent microscopes.
  • Interferometer Configuration: Not Specified
  • Light Source: 594nm
  • Output Polarization: Not Specified
  • RMS Precision: Not Specified
Data Sheet
NSLI-543-2 N-Slit Laser Interferometer
Interferometric Optics
Based on multiple-prism beam expansion and digital detection the N-slit interferometer allows for the rapid interferometric characterization of transmission optical surfaces in general. A significant advance over traditional point-by-point incoherent microdensitometers and point-by-point incoherent microscopes.
  • Interferometer Configuration: Not Specified
  • Light Source: 543nm
  • Output Polarization: Not Specified
  • RMS Repeatability: Not Specified
  • RMS Precision: Not Specified
Data Sheet
NSLI-543-1 N-Slit Laser Interferometer
Interferometric Optics
Based on multiple-prism beam expansion and digital detection the N-slit interferometer allows for the rapid interferometric characterization of transmission optical surfaces in general. A significant advance over traditional point-by-point incoherent microdensitometers and point-by-point incoherent microscopes. 
  • Interferometer Configuration: Not Specified
  • Light Source: 543nm
  • Output Polarization: Not Specified
  • RMS Repeatability: Not Specified
  • RMS Precision: Not Specified
Data Sheet
GEMINI Ultra-Stable Interferometer
Nireos
GEMINI is a novel and compact interferometer that can guarantee very high robustness and stability between the two generated replicas of light.  
  • Interferometer Configuration: Not Specified
  • Light Source: White Light
  • Output Polarization: Not Specified
  • RMS Repeatability: Not Specified
  • RMS Precision: Not Specified
Data Sheet
GEMINI-2D
Nireos
GEMINI-2D Interferometer is the advanced model of the GEMINI, specially designed to: keep constant the dispersion during the scan of the relative delay between the two generated replicas of light keep fixed the absolute arrival time of one of the two replicas (with attosecond stability) The capability of ...
  • Interferometer Configuration: Not Specified
  • Light Source: White Light
  • Output Polarization: Not Specified
  • RMS Repeatability: Not Specified
  • RMS Precision: Not Specified
Data Sheet
PicoScale sensor head type L01
SmarAct
The L01 is a sensor head for the PICOSCALE laser interferometer. The target beam is focused along only one axis with a cylinder lens so that a line focus is generated. This way, the sensor head has a relatively large angular working range along the focused axis while having a large diameter along the orthogonal axis. Typically, these ...
  • Interferometer Configuration: Not Specified
  • Light Source: 1550nm
  • Output Polarization: Linear
  • RMS Repeatability: Not Specified
  • RMS Precision: Not Specified
Data Sheet

Did You know?

Invented by Albert Michelson in the late 19th century, interferometers are powerful tools developed to make incredibly small measurements. These investigative devices are called interferometers because they work by merging two or more sources of light to create an interference pattern, which can be measured and analyzed. Interferometers are so powerful that some have even been designed to measure a distance of 1/10,000th of a proton. The ability to take such small measurements is useful in fields such as astronomy, seismology, fiber optics, and quantum mechanics.