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Introduction
The laser is a device for producing electromagnetic waves of the same nature
as light waves, radio waves and X-rays but which have characteristics not
present in any other natural or man-made radiation available at present.
The characteristics of laser light are essentially coherence which is the
coincidence of phases both in time, in which case we speak of monofrequency
or monochromaticity, and in space for which it is possible to obtain
extremely concentrated light beams even for paths kilometres long or to
focalize the beams or make them diverge in an extremely controlled manner.
The difference between sunlight or normal incandescent light used for
domestic illumination and laser light is that the sun or the lamp emit
radiation or quanta in a random fashion, like people leaving a stadium or
cinema, while the laser emits extremely orderly quanta of energy, like a
platoon of soldiers or robots, all exactly alike, that march perfectly
aligned in rows and columns.
With a rhetorical figure of synecdoche, the word laser has come to identify
the apparatus in which the physical laser process occurs in a controlled
form.
Historical notes
The first applications in the field of medicine were in ophthalmic
pathology, while in 1962 Goldman applied the laser in field of dermatology.
G.L. Jako used a CO2 laser with a microscope for surgical applications on
the vocal chords. The first Authors to report results of surgical
applications of a CO2 laser in gynaecology are I. Goldman, I. Kaplan, R. Ger.
The assumptions for the discovery of the laser were proposed by the
development of quantum physics. The bases of this theory date back to the
early 1900s, from Plancks's studies of radiation of the black body and
developed through the atom model with discrete energy levels attributed to
Bohr, Einstein's theory (1917) of stimulated emission of photons and to
Einstein and Bose's data on photons.
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In 1950 Lamb and Rutherford performed the first
important experimental verification of a mechanism essential for laser
function: the population inversion in the energy levels in an atomic or
molecular system. Block theoretically predicted such a mechanism during his
work in 1945. In 1955 Lamb received the Nobel Prize in Physics for his
important work in this field. In 1964 the Nobel Prize for Physics was again
awarded to researchers who contributed to the birth of the laser: an
American, Towens, and two Russians, Basov and Prochorov, who since 1951 had
been involved in research to create quantum amplifiers by means of systems
placed in a condition of energy state population inversion.
Important research on this topic was also performed by the American, Weber
during the same period. The first working apparatus was constructed by the
Towens group at Columbia University in 1954. For the first time they were
able to obtain radio waves at a microwave frequency without the use of the
usual electronic tube. The waves, little more than a centimetre in length,
were generated in a small metal box that contained only ammonia gas. The
"Maser", antecedent of the laser, was born. "Maser" is
the abbreviation of "Microwave Amplification by Stimulated Emission of
Radiation". Following this, (1958) the principle was extended by Towens
and Schawlow to the field of optical frequencies, and the letter
"M" came to indicate "molecular", while
"amplification" at optical frequencies became known as
"laser" from the acronym of "Light Amplification by
Stimulated Emission of Radiation".
In mid-1960, T.H. Maiman, of Hughes Aircraft Co. USA, constructed the first
optical Maser, or ruby laser, the first solid state laser. At the end of
1960, A. Javan and collaborators constructed the first gas laser using a
mixture of helium and neon (He-Ne). In 1965 Patel created the first
molecular gas (CO2) laser.
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