000585148 001__ 585148 000585148 005__ 20251014093403.0 000585148 0247_ $$2doi$$a10.1038/s41467-024-53788-z 000585148 0247_ $$2datacite_doi$$a10.3204/PUBDB-2023-03421 000585148 0247_ $$2altmetric$$aaltmetric:171002738 000585148 0247_ $$2pmid$$apmid:39580474 000585148 0247_ $$2WOS$$aWOS:001362684200007 000585148 0247_ $$2openalex$$aopenalex:W4404645458 000585148 037__ $$aPUBDB-2023-03421 000585148 041__ $$aEnglish 000585148 082__ $$a500 000585148 1001_ $$0P:(DE-H253)PIP1085492$$aRitzkowsky, Felix$$b0$$eCorresponding author 000585148 245__ $$aOn-Chip Petahertz Electronics for Single-Shot Phase Detection 000585148 260__ $$a[London]$$bNature Publishing Group UK$$c2024 000585148 3367_ $$2DRIVER$$aarticle 000585148 3367_ $$2DataCite$$aOutput Types/Journal article 000585148 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1734604972_44243 000585148 3367_ $$2BibTeX$$aARTICLE 000585148 3367_ $$2ORCID$$aJOURNAL_ARTICLE 000585148 3367_ $$00$$2EndNote$$aJournal Article 000585148 520__ $$aAttosecond science has demonstrated that electrons can be controlled on the sub-cycle time scale of an optical waveform, paving the way towards optical frequency electronics. However, these experiments historically relied on high-energy laser pulses and detection not suitable for microelectronic integration. For practical optical frequency electronics, a system suitable for integration and capable of generating detectable signals with low pulse energies is needed. While current from plasmonic nanoantenna emitters can be driven at optical frequencies, low charge yields have been a significant limitation. In this work we demonstrate that large-scale electrically connected plasmonic nanoantenna networks, when driven in concert, enable charge yields sufficient for single-shot carrier-envelope phase detection at repetition rates exceeding tens of kilohertz. We not only show that limitations in single-shot CEP detection techniques can be overcome, but also demonstrate a flexible approach to optical frequency electronics in general, enabling future applications such as high sensitivity petahertz-bandwidth electric field sampling or logic-circuits. 000585148 536__ $$0G:(DE-HGF)POF4-631$$a631 - Matter – Dynamics, Mechanisms and Control (POF4-631)$$cPOF4-631$$fPOF IV$$x0 000585148 536__ $$0G:(EU-Grant)609920$$aAXSIS - Frontiers in Attosecond X-ray Science: Imaging and Spectroscopy (609920)$$c609920$$fERC-2013-SyG$$x1 000585148 536__ $$0G:(GEPRIS)390715994$$aDFG project G:(GEPRIS)390715994 - EXC 2056: CUI: Advanced Imaging of Matter (390715994)$$c390715994$$x2 000585148 536__ $$0G:(GEPRIS)453615464$$aDFG project G:(GEPRIS)453615464 - Dielektrischer Laserbeschleuniger im mittleren Infrarotbereich (453615464)$$c453615464$$x3 000585148 542__ $$2Crossref$$i2024-11-23$$uhttps://creativecommons.org/licenses/by/4.0 000585148 542__ 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