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Generation of shape-invariant flat-top laser beams

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dc.contributor.author Ait-Ameur, K
dc.contributor.author Naidoo, Darryl
dc.contributor.author Ngcobo, Sandile
dc.contributor.author Fromager, M
dc.contributor.author Litvin, I
dc.contributor.author Hasnaoui, A
dc.contributor.author Harfouche, A
dc.contributor.author Forbes, A
dc.date.accessioned 2016-04-22T07:27:23Z
dc.date.available 2016-04-22T07:27:23Z
dc.date.issued 2015-02
dc.identifier.citation Ait-Ameur, K, Naidoo, S, Ngcobo, S, Fromager, M, Litvin, I, Hasnaoui, A, Harfouche, A, and Forbes, A. 2015. Generation of shape-invariant flat-top laser beams. In: 2015 Proceedings of SPIE 9434, Laser Resonators, Microresonators, and Beam Control XVII, San Francisco, California, United States, 7 February 2015. en_US
dc.identifier.uri http://proceedings.spiedigitallibrary.org/mobile/proceeding.aspx?articleid=2194908
dc.identifier.uri http://hdl.handle.net/10204/8511
dc.description 2015 Proceedings of SPIE 9434, Laser Resonators, Microresonators, and Beam Control XVII, San Francisco, California, United States, 7 February 2015. Due to copyright restrictions, the attached PDF file only contains the abstract of the full text item. en_US
dc.description.abstract A great number of laser applications need in place of the usual Gaussian beam a flat-top intensity profile in the focal plane of a focusing lens. In general the transformation of the laser beam from the Gaussian to the flat-top shape is made by a diffractive beam shaping technique. It is worthwhile to note that this transformation occurs in the vicinity of the focal plane. If a flat top laser beam keeping its shape during propagation is needed then this can be obtained by a weighted incoherent mixing of LG(sub0)0 and LG(sub01) eigenmodes. Here, we consider the generation of these two transverse modes by a solid-state laser axially pumped by a laser diode. The idea is to design the laser cavity so as to make identical the losses of LG(sub00) and LG(sub01) modes. To reach this objective we have used two techniques. The first one called as diffractive lies to insert an adequate amplitude mask inside the cavity. The second one called as interferometric consisted to couple the laser to an external cavity. It is important to note that LG(sub00) and LG(sub01) modes are not spatially in concurrence, i.e. the peak of the LG(sub00) appears in the dip of the LG(sub01) mode. As a result, the energy extraction from the amplifying medium is improved increasing thus the laser slope efficiency. Theory and experimental verifications have been done for the diffractive and interferometric techniques allowing the generation of a flat-top laser beam keeping its shape from the near-field to the far-field. en_US
dc.language.iso en en_US
dc.publisher SPIE en_US
dc.relation.ispartofseries Worklist;14888
dc.subject Diffractive optics en_US
dc.subject Intra-cavity laser beam shaping en_US
dc.subject High order transverse modes en_US
dc.subject Optical feedback en_US
dc.title Generation of shape-invariant flat-top laser beams en_US
dc.type Conference Presentation en_US
dc.identifier.apacitation Ait-Ameur, K., Naidoo, D., Ngcobo, S., Fromager, M., Litvin, I., Hasnaoui, A., ... Forbes, A. (2015). Generation of shape-invariant flat-top laser beams. SPIE. http://hdl.handle.net/10204/8511 en_ZA
dc.identifier.chicagocitation Ait-Ameur, K, Darryl Naidoo, Sandile Ngcobo, M Fromager, I Litvin, A Hasnaoui, A Harfouche, and A Forbes. "Generation of shape-invariant flat-top laser beams." (2015): http://hdl.handle.net/10204/8511 en_ZA
dc.identifier.vancouvercitation Ait-Ameur K, Naidoo D, Ngcobo S, Fromager M, Litvin I, Hasnaoui A, et al, Generation of shape-invariant flat-top laser beams; SPIE; 2015. http://hdl.handle.net/10204/8511 . en_ZA
dc.identifier.ris TY - Conference Presentation AU - Ait-Ameur, K AU - Naidoo, Darryl AU - Ngcobo, Sandile AU - Fromager, M AU - Litvin, I AU - Hasnaoui, A AU - Harfouche, A AU - Forbes, A AB - A great number of laser applications need in place of the usual Gaussian beam a flat-top intensity profile in the focal plane of a focusing lens. In general the transformation of the laser beam from the Gaussian to the flat-top shape is made by a diffractive beam shaping technique. It is worthwhile to note that this transformation occurs in the vicinity of the focal plane. If a flat top laser beam keeping its shape during propagation is needed then this can be obtained by a weighted incoherent mixing of LG(sub0)0 and LG(sub01) eigenmodes. Here, we consider the generation of these two transverse modes by a solid-state laser axially pumped by a laser diode. The idea is to design the laser cavity so as to make identical the losses of LG(sub00) and LG(sub01) modes. To reach this objective we have used two techniques. The first one called as diffractive lies to insert an adequate amplitude mask inside the cavity. The second one called as interferometric consisted to couple the laser to an external cavity. It is important to note that LG(sub00) and LG(sub01) modes are not spatially in concurrence, i.e. the peak of the LG(sub00) appears in the dip of the LG(sub01) mode. As a result, the energy extraction from the amplifying medium is improved increasing thus the laser slope efficiency. Theory and experimental verifications have been done for the diffractive and interferometric techniques allowing the generation of a flat-top laser beam keeping its shape from the near-field to the far-field. DA - 2015-02 DB - ResearchSpace DP - CSIR KW - Diffractive optics KW - Intra-cavity laser beam shaping KW - High order transverse modes KW - Optical feedback LK - https://researchspace.csir.co.za PY - 2015 T1 - Generation of shape-invariant flat-top laser beams TI - Generation of shape-invariant flat-top laser beams UR - http://hdl.handle.net/10204/8511 ER - en_ZA


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