Thermal effects in a gain medium of a high-power laser can cause significant power losses through depolarization, if a gain medium without intrinsic birefringence is used and the laser resonator contains an element with high losses for one of the polarization directions (e.g. a Brewster plate). The reason for this is that the temperature gradients in the gain medium induce mechanical stress and thus some amount of birefringence, with the direction of the local axis varying over the beam cross-section. (The birefringence axes are often oriented in the radial and tangential direction.) As a result, an originally linear polarization state is distorted, so that losses can occur at a polarizing intracavity element.
Thermally induced depolarization is suppressed if the gain medium has a sufficiently strong natural birefringence, so that the birefringent axis can not be significantly rotated by thermal effects. This is the case, e.g., in Nd:YVO4 lasers. For optically isotropic gain media such as Nd:YAG, thermal depolarization loss can be minimized, e.g. by using a Faraday rotator , a λ/4 plate in the laser resonator , or by arranging the laser resonator for a Gouy phase shift of suitable magnitude . The basic idea behind such compensation methods is to create a situation where depolarization from different passes through a gain medium cancel each other at least partially. Depolarization losses can also be reduced by using a YAG crystal with optimized cut direction [6, 8].
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|||W. C. Scott and M. de Wit, “Birefringence compensation and TEM00 mode enhancement in a Nd:YAG laser”, Appl. Phys. Lett. 18, 3 (1971), doi:10.1063/1.1653466|
|||H. J. Eichler et al., “Thermal lensing and depolarization in a highly pumped Nd:YAG laser amplifier”, J. Phys. D: Appl. Phys. 26, 1884 (1993), doi:10.1088/0022-3727/26/11/008|
|||M. P. Murdough and C. A. Denman, “Mode-volume and pump-power limitations in injection-locked TEM00 Nd:YAG rod lasers”, Appl. Opt. 35 (30), 5925 (1996), doi:10.1364/AO.35.005925|
|||W. A. Clarkson et al., “Simple method for reducing the depolarization loss resulting from thermally induced birefringence in solid-state lasers”, Opt. Lett. 24 (12), 820 (1999), doi:10.1364/OL.24.000820|
|||R. Fluck et al., “Birefringence compensation in single solid-state rods”, Appl. Phys. Lett. 76 (12), 1513 (2000), doi:10.1063/1.126080|
|||I. Shoji and T. Taira, “Intrinsic reduction of the depolarization loss in solid state lasers by use of a (110)-cut Y3Al5O12 crystal”, Appl. Phys. Lett. 80 (17), 3048 (2002), doi:10.1063/1.1475365|
|||J. J. Morehead, “Compensation of laser thermal depolarization using free space”, JSTQE 13 (3), 498 (2007), doi:10.1109/JSTQE.2007.896616|
|||O. Puncken et al., “Intrinsic reduction of the depolarization in Nd:YAG crystals”, Opt. Express 18 (19), 20461 (2010), doi:10.1364/OE.18.020461|
|||M. De Video et al., “Modelling and measurement of thermal stress-induced depolarisation in high energy, high repetition rate diode-pumped Yb:YAG lasers”, Opt. Express 29 (4), 5607 (2021), doi:10.1364/OE.417152|
|||W. Koechner, Solid-State Laser Engineering, 6th edn., Springer, Berlin (2006)|