Page 2 - Not Specified Interferometers

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. 

Specifications

Interferometer Configuration: Not Specified
Light Source: 632 nm or 633nm
Output Polarization: Not Specified
RMS Repeatability: Not Specified
RMS Precision: Not Specified
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. 

Specifications

Interferometer Configuration: Not Specified
Light Source: 632 nm or 633nm
Output Polarization: Not Specified
RMS Repeatability: Not Specified
RMS Precision: Not Specified
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. 

Specifications

Interferometer Configuration: Not Specified
Light Source: 594nm
Output Polarization: Not Specified
RMS Repeatability: Not Specified
RMS Precision: Not Specified
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.

Specifications

Interferometer Configuration: Not Specified
Light Source: 594nm
Output Polarization: Not Specified
RMS Precision: Not Specified
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.

Specifications

Interferometer Configuration: Not Specified
Light Source: 543nm
Output Polarization: Not Specified
RMS Repeatability: Not Specified
RMS Precision: Not Specified
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. 

Specifications

Interferometer Configuration: Not Specified
Light Source: 543nm
Output Polarization: Not Specified
RMS Repeatability: Not Specified
RMS Precision: Not Specified
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.  

Specifications

Interferometer Configuration: Not Specified
Light Source: White Light
Output Polarization: Not Specified
RMS Repeatability: Not Specified
RMS Precision: Not Specified
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 ...

Specifications

Interferometer Configuration: Not Specified
Light Source: White Light
Output Polarization: Not Specified
RMS Repeatability: Not Specified
RMS Precision: Not Specified
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 ...

Specifications

Interferometer Configuration: Not Specified
Light Source: 1550nm
Output Polarization: Linear
RMS Repeatability: Not Specified
RMS Precision: Not Specified
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 ...

Specifications

Interferometer Configuration: Not Specified
Light Source: 1550nm
Output Polarization: Linear
RMS Repeatability: Not Specified
RMS Precision: Not Specified
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 ...

Specifications

Interferometer Configuration: Not Specified
Light Source: 1550nm
Output Polarization: Linear
RMS Repeatability: Not Specified
RMS Precision: Not Specified
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 ...

Specifications

Interferometer Configuration: Not Specified
Light Source: 1550nm
Output Polarization: Linear
RMS Repeatability: Not Specified
RMS Precision: Not Specified