TY - JOUR
T1 - Transverse profile shaping of laser beams by means of aspherical mirror resonators
AU - Ruschin, S.
N1 - Publisher Copyright:
© 1993 SPIE. All rights reserved.
PY - 1993/4/22
Y1 - 1993/4/22
N2 - Two main approaches exist in order to generate laser beams with transverse profiles which depart from the common Gaussian shape: The use of graded transmission resonator mirrors and the use of aspheric mirrors. Aspheric, fully reflecting mirrors have the advantage of better power and energy handling and availability of reflecting surfaces at wavelengths where transparent materials are inconvenient to handle and eventually nonexisting. A beam synthesis method was developed by means of which it can be proven that any pre-required beam profile can be supported by a resonator based on either variable transmission mirrors or aspheric mirrors, in the empty-cavity approximation. The cavity will not however necessarily support the pre-required mode as the lowest-loss mode, and the gain profile of the amplifying medium has to be taken into account. Examples will be presented in which cavity design improves the efficiency of the laser by coupling between the mode profile to the gain profile of the medium. Additional applications of aspheric mirror resonators include the matching of free-space modes to waveguide modes and shaping of beams according to subsequent beam' handling requirements like focusing to preferred spot shapes for materials processing.
AB - Two main approaches exist in order to generate laser beams with transverse profiles which depart from the common Gaussian shape: The use of graded transmission resonator mirrors and the use of aspheric mirrors. Aspheric, fully reflecting mirrors have the advantage of better power and energy handling and availability of reflecting surfaces at wavelengths where transparent materials are inconvenient to handle and eventually nonexisting. A beam synthesis method was developed by means of which it can be proven that any pre-required beam profile can be supported by a resonator based on either variable transmission mirrors or aspheric mirrors, in the empty-cavity approximation. The cavity will not however necessarily support the pre-required mode as the lowest-loss mode, and the gain profile of the amplifying medium has to be taken into account. Examples will be presented in which cavity design improves the efficiency of the laser by coupling between the mode profile to the gain profile of the medium. Additional applications of aspheric mirror resonators include the matching of free-space modes to waveguide modes and shaping of beams according to subsequent beam' handling requirements like focusing to preferred spot shapes for materials processing.
UR - http://www.scopus.com/inward/record.url?scp=85075798582&partnerID=8YFLogxK
U2 - 10.1117/12.143850
DO - 10.1117/12.143850
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AN - SCOPUS:85075798582
SN - 0277-786X
VL - 1834
SP - 169
EP - 175
JO - Proceedings of SPIE - The International Society for Optical Engineering
JF - Proceedings of SPIE - The International Society for Optical Engineering
T2 - Laser Energy Distribution Profiles: Measurement and Applications 1992
Y2 - 16 November 1992
ER -