Optical damage thresholds of single-mode fiber-tip spintronic terahertz emitters

dc.contributor.authorParies, Felix
dc.contributor.authorSelz, Felix
dc.contributor.authorSantos, Cristiane N.
dc.contributor.authorLampin, Jean-Francois
dc.contributor.authorKoleják, Pierre
dc.contributor.authorLezier, Geoffrey
dc.contributor.authorTroadec, David
dc.contributor.authorTiercelin, Nicolas
dc.contributor.authorVanwolleghem, Mathias
dc.contributor.authorAddda, Ahmed
dc.contributor.authorKampfrath, Tobias
dc.contributor.authorSeifert, Tom S.
dc.contributor.authorVon Freymann, Georg
dc.contributor.authorMolter, Daniel
dc.date.accessioned2026-05-13T07:31:45Z
dc.date.available2026-05-13T07:31:45Z
dc.date.issued2024
dc.description.abstractSpintronic terahertz emitters (STEs) are gapless, ultrabroadband terahertz sources that can be driven within a wide pump-wavelength and repetition-rate range. While STEs driven by strong pump lasers operating at kilohertz repetition rates excel in generating high electric field strengths for terahertz spectroscopy or ellipsometry, newly advancing technologies such as ultrafast modulation of terahertz polarization, scanning tunneling microscopy, laser terahertz emission nanoscopy, and fully fiber-coupled integrated systems demand an STE pumping at megahertz repetition rates. In all these applications the available terahertz power is ultimately limited by the STE's optical damage threshold. However, to date, only very few publications have targeted this crucial topic and investigations beyond the kilohertz repetition-rate regime are missing. Here, we present a complete study of our single-mode fiber-tip STEs' optical damage thresholds covering the kilohertz, megahertz, and gigahertz repetition-rate regimes as well as continuous-wave irradiation. As a very important finding, we introduce the necessity of classifying the optical damage threshold into two regimes: a low-repetition-rate regime characterized by a nearly constant fluence threshold, and a high-repetition-rate regime characterized by an antiproportional fluence dependence ("average-power threshold"). For our single-mode fiber-tip STEs, the transition between these regimes occurs around 4 MHz. Moreover, we present a cohesive theory of the damaging thermodynamical processes at play and identify temperature-driven inter-layer diffusion as the primary cause of the STE failure. These findings are substantiated by atomic force microscopy, infrared scattering-type scanning near-field optical microscopy, and scanning of spintronic terahertz emission.
dc.description.firstpage24826
dc.description.issue14
dc.description.lastpage24838
dc.description.sourceWeb of Science
dc.description.volume32
dc.identifier.citationOptics Express. 2024, vol. 32, issue 14, p. 24826-24838.
dc.identifier.doi10.1364/OE.525747
dc.identifier.issn1094-4087
dc.identifier.urihttp://hdl.handle.net/10084/158613
dc.identifier.wos001278801500010
dc.language.isoen
dc.publisherOptica Publishing Group
dc.relation.ispartofseriesOptics Express
dc.relation.urihttps://doi.org/10.1364/OE.525747
dc.rights© 2024 Optica Publishing Group
dc.rights.accessopenAccess
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/
dc.titleOptical damage thresholds of single-mode fiber-tip spintronic terahertz emitters
dc.typearticle
dc.type.statusPeer-reviewed
dc.type.versionpublishedVersion
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local.files.size3377985
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