{"id":195140,"date":"2024-08-24T19:24:46","date_gmt":"2024-08-25T00:24:46","guid":{"rendered":"https:\/\/lifeboat.com\/blog\/2024\/08\/chiral-topological-light-for-detection-of-robust-enantiosensitive-observables"},"modified":"2024-08-24T19:24:46","modified_gmt":"2024-08-25T00:24:46","slug":"chiral-topological-light-for-detection-of-robust-enantiosensitive-observables","status":"publish","type":"post","link":"https:\/\/lifeboat.com\/blog\/2024\/08\/chiral-topological-light-for-detection-of-robust-enantiosensitive-observables","title":{"rendered":"Chiral topological light for detection of robust enantiosensitive observables"},"content":{"rendered":"<p><a class=\"aligncenter blog-photo\" href=\"https:\/\/lifeboat.com\/blog.images\/chiral-topological-light-for-detection-of-robust-enantiosensitive-observables.jpg\"><\/a><\/p>\n<p>Figure <a data-track=\"click\" data-track-label=\"link\" data-track-action=\"figure anchor\" href=\"https:\/\/www.nature.com\/articles\/s41566-024-01499-8#Fig5\">5<\/a> is the second key result of our work. It demonstrates a robust route to decomposing the contributions to the overall chiral optical signal, originating from interfering pathways encoding different topological charge. The decomposition relies on straightforward Fourier analysis of the far-field image. Given the ability to precisely control the orientation of the polarization ellipse of the incident infrared light, chiral topological light generated by such infrared drivers stands out as a robust probe of molecular chirality, capable of inducing strongly enantiosensitive total intensity signals as well as giant rotations of intense spectral features.<\/p>\n<p>The concept of chiral topological light introduced here is not limited to vortex beams: other members of the larger family of structured light beams<sup><a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" title=\"Angelsky, O. V. et al. Structured light: ideas and concepts. Front. Phys. 8, 00114 (2020).\" href=\"https:\/\/www.nature.com\/articles\/s41566-024-01499-8#ref-CR32\" id=\"ref-link-section-d187175793e2778\">32<\/a>,<a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" title=\"Forbes, A., de Oliveira, M. & Dennis, M. R. Structured light. Nat. Photon. 15253&ndash;262 (2021).\" href=\"https:\/\/www.nature.com\/articles\/s41566-024-01499-8#ref-CR33\" id=\"ref-link-section-d187175793e2778_1\">33<\/a>,<a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" aria-label=\"Reference 34\" title=\"Rubinsztein-Dunlop, H. et al. Roadmap on structured light. J. Opt. 19, 013001 (2017).\" href=\"https:\/\/www.nature.com\/articles\/s41566-024-01499-8#ref-CR34\" id=\"ref-link-section-d187175793e2781\">34<\/a><\/sup> can be used to create locally and globally chiral topological light. We envision using tightly focused radially polarized beams, which are known to posses strong longitudinal components<sup><a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" aria-label=\"Reference 35\" title=\"Dorn, R., Quabis, S. & Leuchs, G. Sharper focus for a radially polarized light beam. Phys. Rev. Lett. 91, 233901 (2003).\" href=\"https:\/\/www.nature.com\/articles\/s41566-024-01499-8#ref-CR35\" id=\"ref-link-section-d187175793e2785\">35<\/a><\/sup>, central to the concept of local chirality. Skyrmionic beams<sup><a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" aria-label=\"Reference 36\" title=\"Guti\u00e9rrez-Cuevas, R. & Pisanty, E. Optical polarization skyrmionic fields in free space. J. Opt. 23, 024004 (2021).\" href=\"https:\/\/www.nature.com\/articles\/s41566-024-01499-8#ref-CR36\" id=\"ref-link-section-d187175793e2789\">36<\/a>,<a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" aria-label=\"Reference 37\" title=\"Du, L., Yang, A., Zayats, A. V. & Yuan, X. Deep-subwavelength features of photonic skyrmions in a confined electromagnetic field with orbital angular momentum. Nat. Phys. 15650&ndash;654 (2019).\" href=\"https:\/\/www.nature.com\/articles\/s41566-024-01499-8#ref-CR37\" id=\"ref-link-section-d187175793e2792\">37<\/a><\/sup> could also be used, for example to induce topological distributions with radially dependent topological charges. From the perspective of structured light<sup><a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" title=\"Angelsky, O. V. et al. Structured light: ideas and concepts. Front. Phys. 8, 00114 (2020).\" href=\"https:\/\/www.nature.com\/articles\/s41566-024-01499-8#ref-CR32\" id=\"ref-link-section-d187175793e2796\">32<\/a>,<a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" title=\"Forbes, A., de Oliveira, M. & Dennis, M. R. Structured light. Nat. Photon. 15253&ndash;262 (2021).\" href=\"https:\/\/www.nature.com\/articles\/s41566-024-01499-8#ref-CR33\" id=\"ref-link-section-d187175793e2796_1\">33<\/a>,<a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" aria-label=\"Reference 34\" title=\"Rubinsztein-Dunlop, H. et al. Roadmap on structured light. J. Opt. 19, 013001 (2017).\" href=\"https:\/\/www.nature.com\/articles\/s41566-024-01499-8#ref-CR34\" id=\"ref-link-section-d187175793e2799\">34<\/a>,<a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" aria-label=\"Reference 38\" title=\"Bliokh, K. Y. et al. Roadmap on structured waves. J. Opt. 25, 103001 (2023).\" href=\"https:\/\/www.nature.com\/articles\/s41566-024-01499-8#ref-CR38\" id=\"ref-link-section-d187175793e2802\">38<\/a><\/sup> the temporally chiral vortex introduced here represents a new kind of polarization singularity, which could be analysed by extending the current framework from monochromatic 3D fields<sup><a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" aria-label=\"Reference 39\" title=\"Bliokh, K. Y., Alonso, M. A. & Dennis, M. R. Geometric phases in 2D and 3D polarized fields: geometrical, dynamical, and topological aspects. Rep. Prog. Phys. 82, 122401 (2019).\" href=\"https:\/\/www.nature.com\/articles\/s41566-024-01499-8#ref-CR39\" id=\"ref-link-section-d187175793e2806\">39<\/a>,<a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" aria-label=\"Reference 40\" title=\"Alonso, M. A. Geometric descriptions for the polarization of nonparaxial light: a tutorial. Adv. Opt. Photon. 15176&ndash;235 (2023).\" href=\"https:\/\/www.nature.com\/articles\/s41566-024-01499-8#ref-CR40\" id=\"ref-link-section-d187175793e2809\">40<\/a><\/sup> to polychromatic 3D fields<sup><a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" aria-label=\"Reference 13\" title=\"Pisanty, E. et al. Knotting fractional-order knots with the polarization state of light. Nat. Photon. 13569&ndash;574 (2019).\" href=\"https:\/\/www.nature.com\/articles\/s41566-024-01499-8#ref-CR13\" id=\"ref-link-section-d187175793e2814\">13<\/a>,<a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" aria-label=\"Reference 41\" title=\"Sugic, D., Dennis, M. R., Nori, F. & Bliokh, K. Y. Knotted polarizations and spin in three-dimensional polychromatic waves. Phys. Rev. Res. 2, 042045 (2020).\" href=\"https:\/\/www.nature.com\/articles\/s41566-024-01499-8#ref-CR41\" id=\"ref-link-section-d187175793e2817\">41<\/a>,<a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" aria-label=\"Reference 42\" title=\"Kessler, D. A. & Freund, I. Lissajous singularities. Opt. Lett. 28111&ndash;113 (2003).\" href=\"https:\/\/www.nature.com\/articles\/s41566-024-01499-8#ref-CR42\" id=\"ref-link-section-d187175793e2820\">42<\/a><\/sup>.<\/p>\n<p>Our method is not limited to high harmonics. Its extension to low-order parametric processes such as chiral sum-frequency generation<sup><a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" aria-label=\"Reference 43\" title=\"Vogwell, J., Rego, L., Smirnova, O. & Ayuso, D. Ultrafast control over chiral sum-frequency generation. Sci. Adv. 9, eadj1429 (2023).\" href=\"https:\/\/www.nature.com\/articles\/s41566-024-01499-8#ref-CR43\" id=\"ref-link-section-d187175793e2827\">43<\/a><\/sup> has potential for non-destructive enantiosensitive imaging in the ultraviolet region and for exploiting intrinsically low-order nonlinearities for enantiosensitive detection in the X-ray domain<sup><a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" aria-label=\"Reference 16\" title=\"Rouxel, J. R. et al. Hard X-ray helica dichroism of disordered molecular media. Nat. Photon. 16570&ndash;574 (2022).\" href=\"https:\/\/www.nature.com\/articles\/s41566-024-01499-8#ref-CR16\" id=\"ref-link-section-d187175793e2831\">16<\/a>,<a data-track=\"click\" data-track-action=\"reference anchor\" data-track-label=\"link\" data-test=\"citation-ref\" aria-label=\"Reference 17\" title=\"Rouxel, J. R. & Mukamel, S. Molecular chirality and Its monitoring by ultrafast X-ray pulses. Chem. Rev. 122, 16802&ndash;16838 (2022).\" href=\"https:\/\/www.nature.com\/articles\/s41566-024-01499-8#ref-CR17\" id=\"ref-link-section-d187175793e2834\">17<\/a><\/sup>.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Figure 5 is the second key result of our work. It demonstrates a robust route to decomposing the contributions to the overall chiral optical signal, originating from interfering pathways encoding different topological charge. The decomposition relies on straightforward Fourier analysis of the far-field image. Given the ability to precisely control the orientation of the polarization [\u2026]<\/p>\n","protected":false},"author":427,"featured_media":0,"comment_status":"open","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[64],"tags":[],"class_list":["post-195140","post","type-post","status-publish","format-standard","hentry","category-singularity"],"_links":{"self":[{"href":"https:\/\/lifeboat.com\/blog\/wp-json\/wp\/v2\/posts\/195140","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/lifeboat.com\/blog\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/lifeboat.com\/blog\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/lifeboat.com\/blog\/wp-json\/wp\/v2\/users\/427"}],"replies":[{"embeddable":true,"href":"https:\/\/lifeboat.com\/blog\/wp-json\/wp\/v2\/comments?post=195140"}],"version-history":[{"count":0,"href":"https:\/\/lifeboat.com\/blog\/wp-json\/wp\/v2\/posts\/195140\/revisions"}],"wp:attachment":[{"href":"https:\/\/lifeboat.com\/blog\/wp-json\/wp\/v2\/media?parent=195140"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/lifeboat.com\/blog\/wp-json\/wp\/v2\/categories?post=195140"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/lifeboat.com\/blog\/wp-json\/wp\/v2\/tags?post=195140"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}