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Stimulating stuff — the first laser

After demonstration in 1954 of the 'maser' principle (microwave amplification by stimulated emission of radiation), systems were sought in which the effect occurred in the infrared and visible spectrum. This goal was reached in 1960 when Theodore Maiman achieved optical laser action in ruby.
Nature 187, 493-494 (1960)
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Stimulated optical radiation in ruby

Schawlow and Townes1 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. Javan2 and Sanders3 have discussed proposals involving electron-excited gaseous systems. In this laboratory 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).

A simplified energy-level diagram for triply ionized chromium in this crystal is shown in Fig. 1. When this material is irradiated with energy at a wave-length of about 5500 Å., chromium ions are excited to the 4F2 state and then quickly lose some of their excitation energy through non-radiative transitions to the 2E state4. This state then slowly decays by spontaneously emitting a sharp doublet the components of which at 300° K. are at 6943 Å. and 6929 Å. (Fig. 2a). Under very intense excitation the population of this metastable state (2E) can become greater than that of the ground-state; this is the condition for negative temperatures and consequently amplification via stimulated emission.

Figure 1
Energy-level diagram of Cr3+ in corundum, showing pertinent processes

high-resolution version

To demonstrate the above effect a ruby crystal of 1-cm. dimensions coated on two parallel faces with silver was irradiated by a high-power flash lamp; the emission spectrum obtained under these conditions is shown in Fig. 2b. These results can be explained on the basis that negative temperatures were produced and regenerative amplification ensued. I expect, in principle, a considerably greater (~108) reduction in line width when mode selection techniques are used1.

Figure 2
Emission spectrum of ruby: a, low-power excitation; b, high-power excitation

high-resolution version

I gratefully acknowledge helpful discussions with G. Birnbaum, R. W. Hellwarth, L. C. Levitt, and R. A. Satten and am indebted to I. J. D'Haenens and C. K. Asawa for technical assistance in obtaining the measurements.

T. H. MAIMAN

Hughes Research Laboratories, A Division of Hughes Aircraft Co., Malibu, California.

  1. Schawlow, A. L., and Townes, C. H., Phys. Rev., 112, 1940 (1958).
  2. Javan, A., Phys. Rev. Letters, 3, 87 (1959).
  3. Sanders, J. H., Phys. Rev. Letters, 3, 86 (1959).
  4. Maiman, T. H., Phys. Rev. Letters, 4, 564 (1960).

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