مرکز منطقه ای اطلاع رساني علوم و فناوري

Abstract :

The self locking behavior of 6328 Å He-Ne gas lasers has been investigated at various mirror separations by controlling the oscillation intensity with the aid of an intracavity modulator. The results indicate that the self-locked gas laser with $m$ light pulses bouncing back and forth between both the mirrors oscillates ordinarily at mfpmode interval (fpis the fundamental axial mode interval) and exceptionally at $1f_{p}$ mode interval. The ordinary self locking, that is, mfplocking, easily occurs around a certain curve plotted as a function of internal oscillation power and of pulse repetition rate or oscillating mode interval regardless of the multiplicity $m$ . This optimum curve of self locking is related to the minimum spread of oscillating mode intervals which results from the frequency pulling, dependent on excitation level only, and from the hole repulsion, dependent on both mode intensity and oscillating mode interval. Accordingly, the repetition rate of the output laser pulse increases with the oscillation intensity on the optimum curve of self locking. The mode quenching, which is a necessary condition of mfplocking ( $m \\neq 1$ ), is associated with the axial mode interval and the effective damping constant representing half the hole width. In consequence, the mfplocking with large $m$ occurs in long cavities and becomes difficult with the increase of $m$ . The power-dependent transition from $1f_{p}$ to $2f_{p}$ self locking is illustrated by the power-dependence of the effective damping constant. In order to realize mfpself locking, the relative positions of the discharge tube and both the mirrors must be chosen so as to make the $2m$ th spatial Fourier component of the excitation density predominant over the other components. The pulse repetition rate of the output light from a locked gas laser is limited mainly by the damping constant of the laser medium. For this reason, the technique of mfplocking is desirable rather to get high output power pulse using a long tube and cavity than to realize high speed pulse using a short tube and cavity.