Matches in SemOpenAlex for { <https://semopenalex.org/work/W2892902900> ?p ?o ?g. }
- W2892902900 abstract "The higher-order Poincare (HOP) sphere beam generalizes optical vortices and vector beams, vividly illustrating their higher-order polarization states. However, its doughnutlike intensity profile varies significantly with topological charge, restricting its application in optics. The authors study a perfect HOP sphere, whose annular intensity profile is $iphantom{rule{0}{0ex}}nphantom{rule{0}{0ex}}dphantom{rule{0}{0ex}}ephantom{rule{0}{0ex}}pphantom{rule{0}{0ex}}ephantom{rule{0}{0ex}}nphantom{rule{0}{0ex}}dphantom{rule{0}{0ex}}ephantom{rule{0}{0ex}}nphantom{rule{0}{0ex}}t$ of topological charge. Single- and multiringed beams are produced in anisotropic medium, by exploiting a spiral geometric phase and aptly designed gratings. This work provides an exciting technique for manipulating the angular momentum of light, to improve $e.g.$ optical tweezers, or multiplexing in optical communication." @default.
- W2892902900 created "2018-10-05" @default.
- W2892902900 creator A5009164839 @default.
- W2892902900 creator A5017033890 @default.
- W2892902900 creator A5022039557 @default.
- W2892902900 creator A5026700421 @default.
- W2892902900 creator A5036887046 @default.
- W2892902900 creator A5040527685 @default.
- W2892902900 creator A5046383891 @default.
- W2892902900 creator A5047135289 @default.
- W2892902900 creator A5081600599 @default.
- W2892902900 date "2018-09-27" @default.
- W2892902900 modified "2023-10-12" @default.
- W2892902900 title "Perfect Higher-Order Poincaré Sphere Beams from Digitalized Geometric Phases" @default.
- W2892902900 cites W1571898161 @default.
- W2892902900 cites W1964064791 @default.
- W2892902900 cites W1991262999 @default.
- W2892902900 cites W1994944040 @default.
- W2892902900 cites W1998478798 @default.
- W2892902900 cites W2038629562 @default.
- W2892902900 cites W2045420711 @default.
- W2892902900 cites W2063516315 @default.
- W2892902900 cites W2066446967 @default.
- W2892902900 cites W2071006676 @default.
- W2892902900 cites W2079956247 @default.
- W2892902900 cites W2088665655 @default.
- W2892902900 cites W2094055587 @default.
- W2892902900 cites W2094575623 @default.
- W2892902900 cites W2104751855 @default.
- W2892902900 cites W2111163802 @default.
- W2892902900 cites W2111540554 @default.
- W2892902900 cites W2120583949 @default.
- W2892902900 cites W2144065779 @default.
- W2892902900 cites W2172222388 @default.
- W2892902900 cites W2183565235 @default.
- W2892902900 cites W2278245471 @default.
- W2892902900 cites W2332210027 @default.
- W2892902900 cites W2337752353 @default.
- W2892902900 cites W2345960861 @default.
- W2892902900 cites W2346786121 @default.
- W2892902900 cites W2407195782 @default.
- W2892902900 cites W2487378917 @default.
- W2892902900 cites W2514982746 @default.
- W2892902900 cites W2527553265 @default.
- W2892902900 cites W255611753 @default.
- W2892902900 cites W2588634987 @default.
- W2892902900 cites W2598793818 @default.
- W2892902900 cites W2599094379 @default.
- W2892902900 cites W2616248175 @default.
- W2892902900 cites W2748148539 @default.
- W2892902900 cites W2766309801 @default.
- W2892902900 cites W2771079598 @default.
- W2892902900 cites W2781990698 @default.
- W2892902900 cites W2783246905 @default.
- W2892902900 cites W2784032369 @default.
- W2892902900 cites W2792217460 @default.
- W2892902900 cites W2964192178 @default.
- W2892902900 doi "https://doi.org/10.1103/physrevapplied.10.034061" @default.
- W2892902900 hasPublicationYear "2018" @default.
- W2892902900 type Work @default.
- W2892902900 sameAs 2892902900 @default.
- W2892902900 citedByCount "31" @default.
- W2892902900 countsByYear W28929029002019 @default.
- W2892902900 countsByYear W28929029002020 @default.
- W2892902900 countsByYear W28929029002021 @default.
- W2892902900 countsByYear W28929029002022 @default.
- W2892902900 countsByYear W28929029002023 @default.
- W2892902900 crossrefType "journal-article" @default.
- W2892902900 hasAuthorship W2892902900A5009164839 @default.
- W2892902900 hasAuthorship W2892902900A5017033890 @default.
- W2892902900 hasAuthorship W2892902900A5022039557 @default.
- W2892902900 hasAuthorship W2892902900A5026700421 @default.
- W2892902900 hasAuthorship W2892902900A5036887046 @default.
- W2892902900 hasAuthorship W2892902900A5040527685 @default.
- W2892902900 hasAuthorship W2892902900A5046383891 @default.
- W2892902900 hasAuthorship W2892902900A5047135289 @default.
- W2892902900 hasAuthorship W2892902900A5081600599 @default.
- W2892902900 hasConcept C10138342 @default.
- W2892902900 hasConcept C104293457 @default.
- W2892902900 hasConcept C114614502 @default.
- W2892902900 hasConcept C120665830 @default.
- W2892902900 hasConcept C121332964 @default.
- W2892902900 hasConcept C130404759 @default.
- W2892902900 hasConcept C147789679 @default.
- W2892902900 hasConcept C162324750 @default.
- W2892902900 hasConcept C168834538 @default.
- W2892902900 hasConcept C182306322 @default.
- W2892902900 hasConcept C184720557 @default.
- W2892902900 hasConcept C184779094 @default.
- W2892902900 hasConcept C185592680 @default.
- W2892902900 hasConcept C20198109 @default.
- W2892902900 hasConcept C205049153 @default.
- W2892902900 hasConcept C33923547 @default.
- W2892902900 hasConcept C37914503 @default.
- W2892902900 hasConcept C62520636 @default.
- W2892902900 hasConcept C77223115 @default.
- W2892902900 hasConcept C88221313 @default.
- W2892902900 hasConceptScore W2892902900C10138342 @default.
- W2892902900 hasConceptScore W2892902900C104293457 @default.
- W2892902900 hasConceptScore W2892902900C114614502 @default.