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dc.contributor.authorNorris, Barnaby
dc.contributor.authorWei, Jin
dc.contributor.authorBetters, Christopher H.
dc.contributor.authorLeon-Saval, Sergio G.
dc.contributor.authorXin, Yinzi
dc.contributor.authorLin, Jonathan
dc.contributor.authorKim, Yoo Jung
dc.contributor.authorSallum, Steph
dc.contributor.authorLozi, Julien
dc.contributor.authorVievard, Sebastian
dc.contributor.authorGuyon, Olivier
dc.contributor.authorGatkine, Pradip
dc.contributor.authorJovanovic, Nemanja
dc.contributor.authorMawet, Dimitri
dc.contributor.authorFitzgerald, Michael P.
dc.date.accessioned2025-12-10T00:08:13Z
dc.date.available2025-12-10T00:08:13Z
dc.date.issued2022en
dc.identifier.citationBarnaby R. M. Norris, Sergio G. Leon-Saval, Jin Wei, Christopher H. Betters, Adam Taras, Jonathan Lin, Yinzi Xin, Yoo Jung Kim, Michael Fitzgerald, Steph Sallum, Aditya Sengupta, Pradip Gatkine, Nemanja Jovanovic, Dimitri Mawet, Julien Lozi, Sebastian Vievard, Vincent Deo, Manon Lallement, Daniel Levinstein, and Olivier Guyon "The photonic lantern wavefront sensor and imager: focal plane wavefront sensing and optimal imaging at the diffraction limit and beyond", Proc. SPIE 13097, Adaptive Optics Systems IX, 130971I (27 August 2024); https://doi.org/10.1117/12.3019643
dc.identifier.urihttps://hdl.handle.net/2123/34598
dc.description.abstractA focal plane wavefront sensor offers major advantages to adaptive optics, including removal of non-commonpath error and providing sensitivity to blind modes (such as petalling). But simply using the observed point spread function (PSF) is not sufficient for wavefront correction, as only the intensity, not phase, is measured. Here we demonstrate the use of a multimode fiber mode converter (photonic lantern) to directly measure the wavefront phase and amplitude at the focal plane. Starlight is injected into a multimode fiber at the image plane, with the combination of modes excited within the fiber a function of the phase and amplitude of the incident wavefront. The fiber undergoes an adiabatic transition into a set of multiple, single-mode outputs, such that the distribution of intensities between them encodes the incident wavefront. The mapping (which may be strongly non-linear) between spatial modes in the PSF and the outputs is stable but must be learned. This is done by a deep neural network, trained by applying random combinations of spatial modes to the deformable mirror. Once trained, the neural network can instantaneously predict the incident wavefront for any set of output intensities. We demonstrate the successful reconstruction of wavefronts produced in the laboratory with low-wind-effect, and an on-sky demonstration of reconstruction of low-order modes consistent with those measured by the existing pyramid wavefront sensor, using SCExAO observations at the Subaru Telescope.en
dc.language.isoenen
dc.publisherSociety of Photo‑Optical Instrumentation Engineers (SPIE)en
dc.relation.ispartofSPIE Astronomical Telescopes + Instrumentationen
dc.rightsCopyright All Rights Reserveden
dc.titleDemonstration of a photonic-lantern focal-plane wavefront sensor using fiber mode conversion and deep learningen
dc.typeConference paperen
dc.subject.asrc510102en
dc.identifier.doi10.1117/12.2629852
dc.type.pubtypeAuthor accepted manuscripten
dc.relation.arcDE210100953
dc.rights.otherCopyright 2024 Society of Photo‑Optical Instrumentation Engineers (SPIE). One print or electronic copy may be made for personal use only. Systematic reproduction and distribution, duplication of any material in this publication for a fee or for commercial purposes, and modification of the contents of the publication are prohibited.en
usyd.facultySeS faculties schools::Faculty of Science::School of Physicsen
workflow.metadata.onlyNoen


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