JOVANA
Explore Library Glossary Getting Started Three Levels Fields How it works Mission
Join the mission
Back to the library
Physics 1960

Stimulated Optical Radiation in Ruby

Theodore H. Maiman

Pump a ruby hard enough and its atoms shine as one — the first laser light.

Choose your version
In depth · the introduction

In May 1960 a coil of flashlamp lit up a fingertip of ruby, and a thin, pure-red beam crossed the lab bench — light had a new kind.

The idea

The light from a bulb or the Sun is a jumble: many colours mixed together, spilling out in every direction, the waves all out of step. Laser light is the opposite — one single colour, one direction, every wave marching in lockstep. Physicists call that last quality coherent.

The trick that makes it is stimulated emission. An atom holding extra energy, when a passing light wave of just the right colour brushes by, lets go of a photon that is an exact copy of the one that triggered it — same colour, same direction, in step. One photon becomes two, two become four, and an avalanche of identical light builds. Maiman's ruby was the first machine to make that avalanche.

How it happened

The theory came first. Einstein predicted stimulated emission back in 1917; in 1958 Arthur Schawlow and Charles Townes worked out how one might build an "optical maser." A quiet race followed. Theodore Maiman, at Hughes Research Laboratories in California, bet on a material others had written off — a small rod of synthetic ruby, wrapped inside a helical photographic flashlamp. On 16 May 1960 it fired. His write-up was so terse that a leading physics journal had already rejected it; it appeared instead as a half-page note in Nature.

Why it mattered

A laser is a tap of pure, controllable light. Because the beam is one colour and one direction, you can focus it to a pinpoint hot enough to cut steel, send it for thousands of miles down a glass fibre thinner than a hair, or use its waves as a ruler accurate to a fraction of their own length. At first almost nobody knew what it was good for — it was joked about as "a solution looking for a problem." Within a generation the problems came flooding in.

An analogy

Think of pushing a child on a swing. A shove at a random moment does little, and can even fight the motion. But push exactly in time with the swing — again, and again, and again — and the arc grows huge from small efforts. Stimulated emission is light pushing atoms in time: each photon nudges an excited atom to release another photon in perfect step, so the wave reinforces itself and the beam swells.

Raise the pump slider and the ruby rod fills with excited atoms; below the threshold line it merely glows, but above it a bright red beam suddenly shoots out of the front mirror and a graph of output rises in a straight line.

Where it sits

The laser grew straight out of quantum physics — the quantized energy rungs of Planck (planck-1900) and Bohr (bohr-1913), and Einstein's 1917 insight about stimulated emission. It is the optical cousin of the microwave maser that came a few years earlier. And it turned around to serve the rest of science: the exquisitely stable lasers that steady the mirrors of LIGO, listening for gravitational waves (ligo-2016), are direct descendants of Maiman's red flash.

The original document
Original source text
T. H. Maiman · Hughes Research Laboratories, Malibu, California · Nature 187, 493–494 · 6 August 1960
The proposal it answered
Schawlow and Townes have proposed a technique for the generation of very monochromatic radiation in the infra-red optical region of the spectrum using an alkali vapour as the active medium.
Maiman opens by naming the 1958 theory he is about to realise — and then quietly departs from its recipe. Where Schawlow and Townes pictured a gas, he reaches for a solid: a small synthetic ruby. (Paraphrase of the body of the note.)
The result
an optical pumping technique has been successfully applied to a fluorescent solid resulting in the attainment of negative temperatures and stimulated optical emission at a wave-length of 6943 Å.; the active material used was ruby (chromium in corundum).
The apparatus, as the note describes it: a ruby cylinder, its two ends silvered to form a resonator, pumped by a helical xenon flashlamp coiled around it. "Negative temperature" is Maiman's term for a population inversion — more chromium ions sitting in the excited level than in the ground state. (Description, not a quotation.)
The threshold
Below a certain flash energy the ruby only fluoresces; above it, the note reports, the emission on the 6943 Å line narrows and intensifies sharply — the signature of stimulated emission building up between the mirrors. (Description of the reported observation.)
[ … ]
The whole communication runs to little more than half a page; the figures, the energy-level diagram, and the discussion are in the original at the source below.
Hughes Research Laboratories, Malibu · 1960