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A laser generates amplified light through stimulated emission. Its name abbreviates “light amplification by stimulated emission of radiation”. Lasers supply the intense beams used in optical tweezers; optical coherence also makes them useful for wave interference measurements. ^[ref].

In the usual material picture, a gain medium stores energy supplied by pumping, for example by incident light or an electric current. Stimulated emission transfers that stored energy to a selected optical normal mode, while competing photon absorption removes light. Producing net optical gain requires a suitable population distribution, such as population inversion in the simple model below.

A familiar laser oscillator uses mirrors to return light through the gain medium. This optical feedback favours resonant normal modes; a partly transmitting mirror lets useful power escape. Feedback and mode selection have different implementations, including ring arrangements: every laser need not resemble the same two-mirror device. The laser threshold example treats just that device. ^{[ref] [ref]}.

The useful combination is concentrated power and controlled optical normal modes. It gives optical tweezers a localized source of force and wave interference measurements a source with useful optical coherence. A laser can nevertheless emit several frequencies; “laser” alone does not guarantee a single frequency. ^[ref].

An original experimental landmark is T. H. Maiman's 1960 report of stimulated optical radiation from optically pumped ruby at about $694.3\mathrm{nm}$. His paper describes both the pumping path and the observed emission, connecting stored material energy with amplified light. ^[ref].

Theodore Harold Maiman and Irnee J. D'Haenens obtained laser action in May 1960. Their arrangement put a ruby rod inside a helical xenon flashlamp. Increasing excitation produced a marked intensity threshold, with subsequent measurements showing narrowing of the ruby emission line.^[ref] The 1960 letter describes silvered parallel crystal faces and compares low- and high-excitation spectra.^[ref]

The controls answer different questions. Increased brightness establishes neither optical feedback nor narrow-band emission by itself: ordinary fluorescence can also brighten with pumping. Comparing spectra at lower and higher excitation, retaining the same optical collection geometry, tests a change in the emission process. Spectrometer resolution, response saturation and heating can alter an apparent line profile; a bright spot alone cannot distinguish those effects. These are interpretation requirements, rather than additional measurements attributed to the short original letter.

Several experimental models were made. The Smithsonian's surviving head has uncertain priority, and its installed crystal came from a later experiment.^[ref] The functional diagram therefore describes the optical mechanism rather than claiming to reconstruct the first surviving unit.

A ruby laser uses chromium ions in ruby as its amplifying medium. Maiman's report identifies a metastable state fed by optical excitation and red emission near $694.3\mathrm{nm}$.^[ref] The pump stores excitation in the medium; stimulated emission transfers it into the optical field. The simplified three-level laser rate equation explains why the stored population and the output pulse evolve together.