The Lynx camera is currently on back-order, with availability expected by the end of November. You may place your order now, but delivery is anticipated for November/December.

Simple and fast calculation of beam sizes from a single monochrome image based on the ISO 11146 method of variances. Some effort has been made to make the algorithm less sensitive to background offset and noise.

Resolution : 720 × 540Sensor Type : CMOS, Global ShutterLens : 2.8-10mm VarifocalInterface : GigE (Gigabit Ethernet)Power Requirement : Power over Ethernet (PoE)

The Lynx GigE Camera is built for professionals who need fast, reliable video analysis. With a frame rate of up to 320 frames per second, it captures high-speed movements with precision, making it ideal for sports performance analysis and research.

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This module also supports M² calculations based on a series of images collected at various distances from the focused beam.

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Here is an analysis of a set of images that do not meet the ISO 11146 requirements for determining M² (because the image locations are not taken in right locations relative to the focus). These beam images are from a HeNe laser with slightly misaligned mirrors to primarily lase in a TEM₀₁ transverse mode. The laser resonator had a fixed rotation of 38.7° from the plane of the optical table.:

To make the most of your video analysis, it's essential to use a camera designed specifically for this purpose. The Lynx GigE Camera is optimized for Swing Catalyst software, ensuring seamless integration and precise data capture. Unlike general-use cameras, this model is built for high-speed motion capture, delivering the accuracy needed for detailed performance analysis. Investing in a specialized camera like the Lynx means better results, more reliable footage, and a smoother workflow, making it a vital tool for serious athletes and coaches.

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Determining M² for a laser beam is also straightforward. Just collect beam diameters from five beam locations within one Rayleigh distance of the focus and from five locations more than two Rayleigh distances:

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In the graph on the below right, the dashed line shows the expected divergence of a pure gaussian beam. Since real beams should diverge faster than this (not slower) there is some problem with the measurements (too few!). On the other hand, the M² value the semi-major axis 2.6±0.7 is consistent with the expected value of 3 for the TEM₁₀ mode.

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