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Putting light in a spin

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dc.contributor.author Dudley, Angela L
dc.contributor.author Rop, R
dc.contributor.author Litvin, IA
dc.contributor.author Lopez-Mariscal, C
dc.contributor.author Roux, FS
dc.contributor.author Forbes, A
dc.date.accessioned 2012-10-25T10:21:30Z
dc.date.available 2012-10-25T10:21:30Z
dc.date.issued 2012-08
dc.identifier.citation Dudley, A, Rop, R, Litvin, IA, Lopez-Mariscal, C, Roux, FS and Forbes, A. Putting light in a spin. Proc. SPIE 8490, Laser Beam Shaping XIII, 849006 (October 15, 2012); doi:10.1117/12.932224 en_US
dc.identifier.isbn 9780819492074
dc.identifier.uri http://proceedings.spiedigitallibrary.org/proceeding.aspx?articleid=1380172
dc.identifier.uri http://hdl.handle.net/10204/6220
dc.description Copyright: 2012 SPIE. Dudley, A, Rop, R, Litvin, IA, Lopez-Mariscal, C, Roux, FS and Forbes, A. Putting light in a spin. Proc. SPIE 8490, Laser Beam Shaping XIII, 849006 (October 15, 2012); doi:10.1117/12.932224. One print or electronic copy may be made for personal use only. Systematic electronic or print reproduction and distribution, duplication of any material in this paper for a fee or for commercial purposes, or modification of the content of the paper are prohibited. en_US
dc.description.abstract We experimentally generated superpositions of higher-order Bessel beams that possess no global orbital angular momentum (OAM), yet exhibit an angular rotation in their intensity profile as the field propagates. The digital holograms encoded on a spatial light modulator (SLM), used for generating such fields, consist of two annular rings of unequal radial wave-vectors where each ring is encoded with an azimuthal mode of equal order but opposite charge. We present experimentally measured angular rotation rates for some example superposition fields, which are shown to be in good agreement with that predicted theoretically. Introducing a second SLM and a Fourier transforming lens, we demonstrate a simple approach to perform an azimuthal decomposition of our generated optical fields. Bounding the match-filter to an annular ring, of varying radius, we are able to perform a scale-independent azimuthal decomposition of our initial field. From the measured weightings of the azimuthally decomposed modes we show reconstruction of the cross-sectional intensity profile and OAM density of our initial field. en_US
dc.language.iso en en_US
dc.publisher SPIE en_US
dc.relation.ispartofseries Workflow;9715
dc.subject Bessel beams en_US
dc.subject Angular rotation en_US
dc.subject Azimuthal decomposition en_US
dc.subject Orbital angular momentum density en_US
dc.title Putting light in a spin en_US
dc.type Conference Presentation en_US
dc.identifier.apacitation Dudley, A. L., Rop, R., Litvin, I., Lopez-Mariscal, C., Roux, F., & Forbes, A. (2012). Putting light in a spin. SPIE. http://hdl.handle.net/10204/6220 en_ZA
dc.identifier.chicagocitation Dudley, Angela L, R Rop, IA Litvin, C Lopez-Mariscal, FS Roux, and A Forbes. "Putting light in a spin." (2012): http://hdl.handle.net/10204/6220 en_ZA
dc.identifier.vancouvercitation Dudley AL, Rop R, Litvin I, Lopez-Mariscal C, Roux F, Forbes A, Putting light in a spin; SPIE; 2012. http://hdl.handle.net/10204/6220 . en_ZA
dc.identifier.ris TY - Conference Presentation AU - Dudley, Angela L AU - Rop, R AU - Litvin, IA AU - Lopez-Mariscal, C AU - Roux, FS AU - Forbes, A AB - We experimentally generated superpositions of higher-order Bessel beams that possess no global orbital angular momentum (OAM), yet exhibit an angular rotation in their intensity profile as the field propagates. The digital holograms encoded on a spatial light modulator (SLM), used for generating such fields, consist of two annular rings of unequal radial wave-vectors where each ring is encoded with an azimuthal mode of equal order but opposite charge. We present experimentally measured angular rotation rates for some example superposition fields, which are shown to be in good agreement with that predicted theoretically. Introducing a second SLM and a Fourier transforming lens, we demonstrate a simple approach to perform an azimuthal decomposition of our generated optical fields. Bounding the match-filter to an annular ring, of varying radius, we are able to perform a scale-independent azimuthal decomposition of our initial field. From the measured weightings of the azimuthally decomposed modes we show reconstruction of the cross-sectional intensity profile and OAM density of our initial field. DA - 2012-08 DB - ResearchSpace DP - CSIR KW - Bessel beams KW - Angular rotation KW - Azimuthal decomposition KW - Orbital angular momentum density LK - https://researchspace.csir.co.za PY - 2012 SM - 9780819492074 T1 - Putting light in a spin TI - Putting light in a spin UR - http://hdl.handle.net/10204/6220 ER - en_ZA


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