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dc.contributor.authorSchmidt, David D.
dc.contributor.authorPablos Marín, José Miguel 
dc.contributor.authorClarke, Cameron
dc.contributor.authorBarolak, Jonathan
dc.contributor.authorWestlake, Nathaniel
dc.contributor.authorHeras, Alba de las
dc.contributor.authorSerrano, Javier
dc.contributor.authorShevtsov, Sergei
dc.contributor.authorKazansky, Peter
dc.contributor.authorAdams, Daniel
dc.contributor.authorHernández García, Carlos 
dc.contributor.authorDurfee, Charles G.
dc.date.accessioned2026-01-09T08:46:09Z
dc.date.available2026-01-09T08:46:09Z
dc.date.issued2025-06
dc.identifier.citationDavid D. Schmidt, José Miguel Pablos-Marín, Cameron Clarke, Jonathan Barolak, Nathaniel Westlake, Alba de las Heras, Javier Serrano, Sergei Shevtsov, Peter Kazansky, Daniel Adams, Carlos Hernández-García, Charles G. Durfee; Self-interfering high harmonic beam arrays driven by Hermite–Gaussian beams. APL Photonics 1 June 2025; 10 (6): 060801.es_ES
dc.identifier.urihttp://hdl.handle.net/10366/168570
dc.description.abstract[EN]The use of structured light to drive highly nonlinear processes in matter not only enables the imprinting of spatially resolved properties onto short-wavelength radiation but also opens alternative avenues for exploring the dynamics of nonlinear laser–matter interactions. In this work, we experimentally and theoretically explore the unique properties of driving high-order harmonic generation (HHG) with Hermite–Gaussian beams. HHG driven by Laguerre–Gauss modes results in harmonics that inherit the azimuthal Laguerre–Gauss modal structure, with their topological charge scaling according to orbital angular momentum conservation. In contrast, when HHG is driven by Hermite–Gauss beams, the harmonic modes do not show a direct correspondence to the driving modal profile. Our experimental measurements using HG0,1 and HG1,1 modes, which are in excellent agreement with our numerical simulations, show that the lobes of the Hermite–Gauss driving beams effectively produce a set of separate phase-locked harmonic beamlets that can interfere downstream. This self-interference, which can be adjusted through the relative position between the gas target and the driving beam focus, can be exploited for precision extreme-ultraviolet interferometry. We demonstrate a simple application to calibrate the dispersion of an extreme-ultraviolet diffraction grating. In addition, we show through simulations that the array of harmonic beamlets can be used as an illumination source for single-shot extreme-ultraviolet ptychography.es_ES
dc.format.mimetypeapplication/pdf
dc.language.isoenges_ES
dc.publisherAmerican Institute of Physicses_ES
dc.subjectPtychographyes_ES
dc.subjectArtificial neural networkses_ES
dc.subjectModal analysises_ES
dc.subjectNonlinear optical processeses_ES
dc.subjectGratingses_ES
dc.subjectInterferometryes_ES
dc.subjectOptical interferencees_ES
dc.subjectOptical phase matchinges_ES
dc.subjectOptical harmonic generationes_ES
dc.subjectGaussian beames_ES
dc.titleSelf-interfering high harmonic beam arrays driven by Hermite–Gaussian beamses_ES
dc.typeinfo:eu-repo/semantics/articlees_ES
dc.relation.publishversionhttps://doi.org/10.1063/5.0255843es_ES
dc.identifier.doi10.1063/5.0255843
dc.relation.projectIDinfo:eu-repo/grantAgreement/EC/H2020/851201/EUes_ES
dc.relation.projectIDPID2022-142340NB-I00es_ES
dc.relation.projectIDSA108P24es_ES
dc.relation.projectIDCLU-2023-1-02es_ES
dc.rights.accessRightsinfo:eu-repo/semantics/openAccesses_ES
dc.identifier.essn2378-0967
dc.journal.titleAPL Photonicses_ES
dc.volume.number10es_ES
dc.issue.number6es_ES
dc.type.hasVersioninfo:eu-repo/semantics/publishedVersiones_ES


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