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dc.contributor.authorDorney, Kevin M.
dc.contributor.authorEllis, Jennifer L.
dc.contributor.authorHernández-García, Carlos
dc.contributor.authorHickstein, Daniel D.
dc.contributor.authorMancuso, Christopher A.
dc.contributor.authorBrooks, Nathan J.
dc.contributor.authorFan, Tingting
dc.contributor.authorFan, Guangyu
dc.contributor.authorZusin, Dmitriy
dc.contributor.authorGentry, Christian
dc.contributor.authorGrychtol, Patrik
dc.contributor.authorKapteyn, Henry C.
dc.contributor.authorMurnane, Margaret M.
dc.date.accessioned2021-06-02T07:05:45Z
dc.date.available2021-06-02T07:05:45Z
dc.date.issued2017-08
dc.identifier.citationDorney, K. M., Ellis, J. L., Hernández-García, C., Hickstein, D. D., Mancuso, C. A., Brooks, N., Fan, T., Fan, G., Zusin, D., Gentry, C., Grychtol, P., Kapteyn, H. C., & Murnane, M. M. (2017). Helicity-Selective Enhancement and Polarization Control of Attosecond High Harmonic Waveforms Driven by Bichromatic Circularly Polarized Laser Fields. Phys. Rev. Lett., 119(6), 063201. https://doi.org/10.1103/PhysRevLett.119.063201es_ES
dc.identifier.issn0031-9007
dc.identifier.urihttp://hdl.handle.net/10366/146647
dc.description.abstractsource of bright, circularly polarized, extreme ultraviolet, and soft x-ray beams, where the individual harmonics themselves are completely circularly polarized. Here, we demonstrate the ability to preferentially select either the right or left circularly polarized harmonics simply by adjusting the relative intensity ratio of the bichromatic circularly polarized driving laser field. In the frequency domain, this significantly enhances the harmonic orders that rotate in the same direction as the higher-intensity driving laser. In the time domain, this helicity-dependent enhancement corresponds to control over the polarization of the resulting attosecond waveforms. This helicity control enables the generation of circularly polarized high harmonics with a user-defined polarization of the underlying attosecond bursts. In the future, this technique should allow for the production of bright highly elliptical harmonic supercontinua as well as the generation of isolated elliptically polarized attosecond pulses.es_ES
dc.description.sponsorshipH. K. and M. M. graciously acknowledge support from the Department of Energy BES Award No. DE-FG02- 99ER14982 for the experimental implementation, as well as a MURI grant from the Air Force Office of Scientific Research under Award No. FA9550-16-1-0121 for the theory. J. E. and C. M. acknowledge support from National Science Foundation Graduate Research Fellowships (Grant No. DGE-1144083). C. H.-G. acknowl- edges support from the Marie Curie International Outgoing Fellowship within the EU Seventh Framework Programme for Research and Technological Development (2007-2013), under REA Grant No. 328334, from Junta de Castilla y León (Project No. SA046U16) and Spanish Ministerio de Economía y Competitividad, MINECO (Projects No. FIS2013-44174-P and No. FIS2016-75652-P). Part of this work utilized the Janus supercomputer, which is sup- ported by the U.S. National Science Foundation (Grant No. CNS-0821794) and the University of Colorado Boulder.es_ES
dc.format.mimetypeapplication/pdf
dc.language.isoenges_ES
dc.rightsAttribution-NonCommercial-NoDerivatives 4.0 Internacional*
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/4.0/*
dc.titleHelicity-Selective Enhancement and Polarization Control of Attosecond High Harmonic Waveforms Driven by Bichromatic Circularly Polarized Laser Fieldses_ES
dc.typeinfo:eu-repo/semantics/articlees_ES
dc.identifier.doi10.1103/PhysRevLett.119.063201
dc.relation.projectIDREA Grant No. 328334es_ES
dc.relation.projectIDSA046U16es_ES
dc.relation.projectIDFIS2013-44174-Pes_ES
dc.relation.projectIDFIS2016-75652-Pes_ES
dc.rights.accessRightsinfo:eu-repo/semantics/openAccesses_ES
dc.identifier.essn1079-7114
dc.journal.titlePhysical Review Letterses_ES
dc.volume.number119es_ES
dc.issue.number6es_ES
dc.type.hasVersioninfo:eu-repo/semantics/publishedVersiones_ES


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