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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
  • Laser Source: 1550nm
  • Output Polarization: Linear
  • RMS Repeatability: Not Specified
  • RMS Precision: Not Specified
Data Sheet
PicoScale Sensor Head Type F01
SmarAct
The F01 is a sensor head type with focused probe beam. This allows to measure displacements of small targets. Furthermore, the sensor heads provide high angular tolerances. After pre-collimation, an integrated beam splitter splits the light into a reference and probe beam as shown in Figure 1. The reference beam is reflected off the ...
  • Interferometer Configuration: Not Specified
  • Laser Source: 1550nm
  • Output Polarization: Linear
  • RMS Repeatability: Not Specified
  • RMS Precision: Not Specified
Data Sheet
PicoScale Sensor Head Type C03
SmarAct
The C03 is a sensor head type optimized for moderate working distances and using retro-reflectors as target. The probe beam is enlarged so that its divergence is reduced and more optical power can be collected after reflection at the target mirror. The C03 sensor head type is based on the standard sensor head type C01, including the ...
  • Interferometer Configuration: Not Specified
  • Laser Source: 1550nm
  • Output Polarization: Linear
  • RMS Repeatability: Not Specified
  • RMS Precision: Not Specified
Data Sheet
PicoScale Sensor Head Type C01
SmarAct
The C01 is the standard sensor head type for the PICOSCALE Interferometer. Due to its collimated output beam, the compact form factor and the various customization options, it is appropriate for most common applications. Each sensor head (see figure 1) is based on two main components: the lens system, collimating the fiber output ...
  • Interferometer Configuration: Not Specified
  • Laser Source: 1550nm
  • Output Polarization: Linear
  • RMS Repeatability: Not Specified
  • RMS Precision: Not Specified
Data Sheet
µPhase® UNIVERSAL - Horizontal Setup For All Kinds of Interferometric Measurements
TRIOPTICS GmbH
Optimized for measurements in R&D, the μPhase® UNIVERSAL is the most flexible instrument of the μPhase® product line. The horizontal design enables the measurement of a large variety of lenses and components differing in size, radius and material.
  • Interferometer Configuration: Twyman–Green Interferometer
  • Laser Source: 633nm, 355nm, 532nm, 780nm, 1053nm, 1064nm
  • Output Polarization: Random
  • RMS Repeatability: <0.01 waves
  • RMS Precision: <0.01 waves
Data Sheet
µPhase® 1000 Flexible Interferometer Sensor
TRIOPTICS GmbH
These highly integrated phase-shifting Twyman-Green interferometer sensors meet the toughest demands for modern quality management. In combination with the μShape™ measuring and analysis software these high-performance precision measuring instruments provide information about the specimen\'s surface deviation or wave front ...
  • Interferometer Configuration: Twyman–Green Interferometer
  • Laser Source: 633nm
  • Output Polarization: Random
  • RMS Repeatability: <0.01 waves
  • RMS Precision: <0.01 waves
Data Sheet
µPhase® 500 Flexible Interferometer Sensor
TRIOPTICS GmbH
These highly integrated phase-shifting Twyman-Green interferometer sensors meet the toughest demands for modern quality management. In combination with the µShapeTM measuring and analysis software these high-performance precision measuring instruments provide information about the specimen\'s surface, wavefront or test ...
  • Interferometer Configuration: Twyman–Green Interferometer
  • Laser Source: 633nm
  • Output Polarization: Random
  • RMS Repeatability: <0.01 waves
  • RMS Precision: <0.01 waves
Data Sheet
AccuFiz Fizeau interferometers offer an unmatched combination of performance, quality and value, for accurate, repeatable measurement of surface shape and transmitted wavefront quality. AccuFiz laser interferometers are extremely easy to use in confined lab spaces. The compact, lightweight design is extremely rigid for maximum ...
  • Interferometer Configuration: Twyman–Green Interferometer
  • Laser Source: 633nm, 355nm, 532nm, 1053nm, 1064nm, 1550nm, 10.6um
  • Output Polarization: Circular
  • RMS Repeatability: <0.00005 waves
  • RMS Precision: <0.0005 waves
Data Sheet
Twyman-Green configuration interferometers offer several important advantages over more traditional Fizeau instruments: Vibration-insensitive measurement enables use in challenging environments such as cryo-vac testing or over long measurement paths. The design can be extremely compact, enabling use in tight spaces, or in ...
  • Interferometer Configuration: Twyman–Green Interferometer
  • Laser Source: 633nm, 355nm, 532nm, 1053nm, 1064nm, 1550nm, 10.6um
  • Output Polarization: Circular
  • RMS Repeatability: <0.001 waves
  • RMS Precision: <0.002 waves
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.