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OCT compatible components are components that have gone through additional steps in the design and product testing phase in order to verify their suitability for use in OCT imaging systems. The F260APC-C and F280APC-C are two collimation / coupling packages that are ideal for use in an OCT scan head. Specifically, the F280APC-C collimator when paired with any of the LSM scan objectives using the SL1325-P16 as a light source can be used to produce a high-performance OCT scan head. The collimator is designed for FC/APC connectorized patch cords, which minimize back reflections that degrade the image produced by the OCT imaging system. The LSM scan lenses are designed to create a uniform spot size and optical path length for the laser for every scan position, which allows a uniform, high-quality, image of the sample to be formed. In addition, the design of the scan lenses and the lens coatings used were chosen to minimize back reflections, which can severely degrade the OCT image quality.  OCT Scan HeadThe schematic to the right shows the basic design of a scanning head for an Optical Coherence Tomography (OCT) Imaging System. The F260APC-C and F280APC-C have been extensively tested and modeled to determine their performance characteristics when placed in a systems like this. Below are the results for the beam divergence of the collimator, spot size produced by the scan head using and LSM03 scan lens, and the coupling efficiency. The collimator should be positioned so that the beam waist is coincident with the entrance pupil of the scan lens. The beam waist / entrance puipil should also be coincident with the center of the reflective face of the 2D steering mirror (galvo mirror). For systems using two 1D galvo mirrors, the beam waist / entrance pupil should be located between the two mirrors in order to minimize any optical path length differences in the system. The beam waist with respect to the end of the collimator housing: - F260APC-C: 14.8 mm
- F280APC-C: 18.0 mm

The plot above shows the beam waist data used to determine the theoretical and measured beam divergence of the F260APC-C OCT collimator when used with a 1310 nm source. The fits yield a measured beam waist of 1.13718 mm and a theoretical beam waist of 1.35548 mm. The calculated full angle beam divergence using the measured and theoretical beam waist fits are 0.042° and 0.035°, respectively. 
The plot above shows the beam waist data used to determine the theoretical and measured beam divergence of the F280APC-C OCT collimator when used with a 1310 nm source. The fits yield a measured beam waist of 1.28102 mm and a theoretical beam waist of 1.63133 mm. The calculated full angle beam divergence using the measured and theoretical beam waist fits are 0.037° and 0.029°, respectively. The theoretical data was generated using Zemax while the measurement was done using a previous generation of Thorlabs' complete M² IR beam analysis system (information on the current version, the M2SET-BP209IR, can be found here). The M² analysis system can measure the times-diffraction-limit M² factor of a laser beam, its reciprocal beam quality (K=1/M²) in addition to the divergence, waist diameter, Rayleigh range, and astigmatism of the beam. 
The plot above shows the data used to determine the theoretical and measured focal spot size of an OCT Scan Head. The OCT scan head used (modeled) to generate this data consisted of a fiber coupled 1310 nm source, an F260APC-C OCT Collimator, and an LSM03 Scan Lens. The component arrangement can be seen in the schematic above. 
The plot above shows the data used to determine the theoretical and measured focal spot size of an OCT Scan Head. The OCT scan head used (modeled) to generate this data consisted of a fiber coupled 1310 nm source, an F280APC-C OCT Collimator, and an LSM03 Scan Lens. The component arrangement can be seen in the schematic above. The theoretical data was generated using Zemax while the measurement was done using a previous generation of Thorlabs' complete M² IR beam analysis system (information on the current version, the M2SET-BP209IR, can be found here). The M² analysis system can measure the times-diffraction-limit M² factor of a laser beam, its reciprocal beam quality (K=1/M²) in addition to the divergence, waist diameter, Rayleigh range, and astigmatism of the beam. .jpg)
The plot above shows the data used to determine the theoretical and measured coupling efficiency of the F260APC-C OCT collimator when used with an LSM03 Scan Lens. .jpg)
The plot above shows the data used to determine the theoretical and measured coupling efficiency of the F280APC-C OCT collimator when used with an LSM03 Scan Lens. The coupling efficiency is the percentage of light collected and collimated by the LSM03 scan lens that is coupled into an SMF-28e single mode fiber using the OCT collimator indicated in the caption below each plot.
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