In 1961, Peter Alden Franken, Alan Hill, C. Wilbur Peters and Gabriel Weinreich focused a pulsed ruby laser through a red optical filter into quartz. The filter suppressed xenon-flash background. A quartz-prism spectrograph used red-insensitive Eastman Type 103 plates. A single shot recorded a feature near from input. Removing the quartz or substituting glass removed the feature; changing polarization of waves and orientation followed their predicted pattern. These controls supported second-harmonic generation; photographic density gave an estimated yield.[ref]
Figure 1. . Original functional diagram; the output strip is illustrative, with no measured line heights. The red optical filter precedes the generating quartz; it cleans the input rather than isolating the ultraviolet output. The spectrograph separates output frequencies. This is a functional arrangement, not a scaled reconstruction or historical plate. The ideal photon panel illustrates conservation of energy. Source. Details.
A spectrograph turns output frequency into a recording position. Its spectral separation makes a faint new component distinguishable from bright input light. The reported rounded wavelengths do not constitute an independent precision measurement of the ratio two. Nor do these observations demonstrate perfect phase matching or complete conversion. The experiment and Nicolaas S later theoretical account are distinct contributions to nonlinear optics.

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