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Date: 17-3-2016
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Date: 31-1-2021
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Date: 10-3-2016
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Laser action caused by molecular oscillations
The most important example is provided by the CO2 gas laser. In these molecules the individual atoms can perform oscillations. The three fundamental kinds of oscillations are shown in fig. 1.1. According to quantum theory the different kinds of oscillations must be quantized so that discrete energy levels result. The energy level diagram belonging to some low lying oscillation levels of CO2 is represented in fig. 1.2. One of the laser processes rests on the optical transition between the levels which are denoted in fig. 1.2 by 00'1 and 10'0. The excitation of the uppermost level is usually achieved in a plasma discharge in which N2 and He participate in addition to CO2. In the plasma discharge a large fraction of the two-atomic N2 molecules is excited to make vibrations, whereby the molecules accumulate in the excited state with the vibration quantum number n = 1 of the harmonic oscillator. Collisions with CO2 molecules in their ground states make a transfer of the energy from the excited state of N2 to an excited state of CO2 possible. The remaining small energy difference is transformed into kinetic energy of the molecules after their collisions. The efficiency of CO2 lasers is very high and lies at about 30%. In order to achieve high power emission, lasers with a length up to several hundred meters have been built. According to quantum theory, besides the vibrational levels of CO2 molecules also discrete rotational levels are possible which may also participate in the laser process. If the gas pressure is increased above 5 Torr, due to the numerous collisions a line-broadening occurs which exceeds the usual