Anti-Reflection Coating
A quarter-wave coating thins away to nothing and the reflected leg returns with it while the reflectance gauge fills, then the layer rebuilds and cancels it again.
A quarter-wave coating thins away to nothing and the reflected leg returns with it while the reflectance gauge fills, then the layer rebuilds and cancels it again.
A beam meets a splitter at forty-five degrees and its share slides from the transmitted leg to the turned one, the ratio bar below handing the same share across.
A parallel bundle through a converging lens releases its focal point and runs flat, then pulls back in until the focus marker lands on the axis again.
An analyser turns a half revolution over a fixed polariser and the transmitted intensity gauge beside it falls to extinction and returns.
The ruling of a grating closes up and its diffracted orders walk outward along the detector, the zero order holding the axis.
A single beam leaving a prism closes into one undivided ray and opens again into a five-way fan about the mean deviation.
A lens element runs back along its rail while the disc on the sensor plane opens from a point into a circle of confusion and the sharpness bar empties with it.
A reference mirror walks along its axis and the interference fringes on the screen slide with it, the whole pattern shifting order by order.
A ray crossing stratified layers straightens out into one undeviated line and curves back into the arc of a ray that has turned right around inside the gradient.
A ray launched into a step-index fibre leaks out through the cladding while its angle sits outside the acceptance cone, then locks into a guided zig-zag when it comes back inside.
The iris stops down and the two point images on the detector broaden past the dashed Rayleigh circles until they run into one another as a single unresolved spot.
A galvanometer facet turns through its range and the reflected beam, swinging twice as far, sweeps its landing point the length of the target rule.
The jaws close on a slit and the diffraction envelope on the screen spreads up its axis and loses height, reaching the dashed reference profile.
A ray crossing a flat interface swings toward the normal as the index ratio of the lower medium rises, the gauge below reading the same change.
Retardance runs from a quarter wave down to zero and back, and the polarisation trace closes from a circle onto the fast axis as a line before opening out again.