dc.contributor.author |
Ngcobo, Sandile
|
|
dc.contributor.author |
Ait-Ameur, K
|
|
dc.contributor.author |
Forbes, A
|
|
dc.date.accessioned |
2012-11-02T07:59:51Z |
|
dc.date.available |
2012-11-02T07:59:51Z |
|
dc.date.issued |
2011-11 |
|
dc.identifier.citation |
Ngcobo, S, Ait-Ameur, K and Forbes, A. Superresolution beams. African Laser Centre Workshop, Cape Town, November 2011 |
en_US |
dc.identifier.uri |
http://hdl.handle.net/10204/6279
|
|
dc.description |
African Laser Centre Workshop, Cape Town, November 2011 |
en_US |
dc.description.abstract |
The transformation of a Gaussian beam (GB) into a symmetrical higher order TEMp0 Laguerre Gaussian beam (LGB) intensity distribution of which is further rectified and transformed into a Gaussian intensity distribution in the plane of a converging lens will produce a sharper focused beam which has transverse high resolution properties. The generated high resolution beam is very useful in improving the spatial resolution of optical imaging microscopes by making the central diffractive spot smaller than the Airy spot. The intracavity beam shaping of the GB is achieved by using an annular binary Diffractive Optical Element (DOE) whose geometry is in connection with the location of the Laguerre polynomial zeros. The DOE imposes positions of p zeros of intensity distributions on the GB, resulting to a generation of TEMp0 beams where there are minimum losses. The focused high resolution beams will then be achieved by shaping the generated higher order LG TEMp0 beams using a binary DOE which has annular zones capable of introducing a phase shift of zero or p on the alternately out of phase rings of the TEMp0 beams into a unified phase and then focusing the rectified beam to generate a high resolution beam which has a Gaussian beam intensity distribution at the focus. |
en_US |
dc.language.iso |
en |
en_US |
dc.relation.ispartofseries |
Workflow;9672 |
|
dc.subject |
Superresolution beams |
en_US |
dc.subject |
Gaussian beams |
en_US |
dc.subject |
Laguerre Gaussian beams |
en_US |
dc.subject |
Diffractive optical element |
en_US |
dc.subject |
Beam shaping |
en_US |
dc.title |
Superresolution beams |
en_US |
dc.type |
Conference Presentation |
en_US |
dc.identifier.apacitation |
Ngcobo, S., Ait-Ameur, K., & Forbes, A. (2011). Superresolution beams. http://hdl.handle.net/10204/6279 |
en_ZA |
dc.identifier.chicagocitation |
Ngcobo, Sandile, K Ait-Ameur, and A Forbes. "Superresolution beams." (2011): http://hdl.handle.net/10204/6279 |
en_ZA |
dc.identifier.vancouvercitation |
Ngcobo S, Ait-Ameur K, Forbes A, Superresolution beams; 2011. http://hdl.handle.net/10204/6279 . |
en_ZA |
dc.identifier.ris |
TY - Conference Presentation
AU - Ngcobo, Sandile
AU - Ait-Ameur, K
AU - Forbes, A
AB - The transformation of a Gaussian beam (GB) into a symmetrical higher order TEMp0 Laguerre Gaussian beam (LGB) intensity distribution of which is further rectified and transformed into a Gaussian intensity distribution in the plane of a converging lens will produce a sharper focused beam which has transverse high resolution properties. The generated high resolution beam is very useful in improving the spatial resolution of optical imaging microscopes by making the central diffractive spot smaller than the Airy spot. The intracavity beam shaping of the GB is achieved by using an annular binary Diffractive Optical Element (DOE) whose geometry is in connection with the location of the Laguerre polynomial zeros. The DOE imposes positions of p zeros of intensity distributions on the GB, resulting to a generation of TEMp0 beams where there are minimum losses. The focused high resolution beams will then be achieved by shaping the generated higher order LG TEMp0 beams using a binary DOE which has annular zones capable of introducing a phase shift of zero or p on the alternately out of phase rings of the TEMp0 beams into a unified phase and then focusing the rectified beam to generate a high resolution beam which has a Gaussian beam intensity distribution at the focus.
DA - 2011-11
DB - ResearchSpace
DP - CSIR
KW - Superresolution beams
KW - Gaussian beams
KW - Laguerre Gaussian beams
KW - Diffractive optical element
KW - Beam shaping
LK - https://researchspace.csir.co.za
PY - 2011
T1 - Superresolution beams
TI - Superresolution beams
UR - http://hdl.handle.net/10204/6279
ER -
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en_ZA |