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dc.contributor.authorHernández García, Carlos 
dc.contributor.authorDurfee, Charles G.
dc.contributor.authorHickstein, Daniel D.
dc.contributor.authorPopmintchev, T.
dc.contributor.authorMeier, A.
dc.contributor.authorMurnane, Margaret M.
dc.contributor.authorKapteyn, Henry C.
dc.contributor.authorSola Larrañaga, Iñigo Juan 
dc.contributor.authorJaron-Becker, Agnieszka
dc.contributor.authorBecker, Andreas
dc.date.accessioned2021-06-03T10:31:55Z
dc.date.available2021-06-03T10:31:55Z
dc.date.issued2016-04
dc.identifier.citationHernández-García, C., Durfee, C. G., Hickstein, D. D., Popmintchev, T., Meier, A., Murnane, M. M., Kapteyn, H. C., Sola, I. J., Jaron-Becker, A., & Becker, A. (2016). Schemes for generation of isolated attosecond pulses of pure circular polarization. Physical Review A, 93(4), 043855. https://doi.org/10.1103/PhysRevA.93.043855es_ES
dc.identifier.issn2469-9926
dc.identifier.urihttp://hdl.handle.net/10366/146682
dc.description.abstractWe propose and analyze two schemes capable of generating isolated attosecond pulses of pure circular polarization, based on results of numerical simulations. Both schemes utilize the generation of circularly polarized high-order-harmonics by crossing two circularly polarized counter-rotating pulses in a noncollinear geometry. Our results show that in this setup isolation of a single attosecond pulse can be achieved either by restricting the driver pulse duration to a few cycles or by temporally delaying the two crossed driver pulses. We further propose to compensate the temporal walk-off between the pulses across the focal spot and increasing the conversion efficiency by using angular spatial chirp to provide perfectly matched pulse fronts. The isolation of pure circularly polarized attosecond pulses, along with the opportunity to select their central energy and helicity in the noncollinear technique, opens new perspectives from which to study ultrafast dynamics in chiral systems and magnetic materials.es_ES
dc.description.sponsorshipThe authors acknowledge Luis Plaja for valuable discussions. C.H.-G. acknowledges support from the Marie Curie International Outgoing Fellowship within the EU Seventh Framework Programme for Research and Technological Development (2007–2013), under REA Grant Agreement No. 328334. C.H.-G. and I.J.S. acknowledge support from Junta de Castilla y León (Project SA116U13, UIC016) and MINECO (Grants No. FIS2013-44174-P and No. FIS2015-71933-REDT). A.J.-B. was supported by grants from the U.S. National Science Foundation (Grants No. PHY-1125844 and No. PHY-1068706). D.H. was supported via a grant from the Department of Energy. M.M.M., H.C.K., C.G.D., and A.B. acknowledge support by a MURI grant from Air Force Office of Scientific Research under Award Number FA9550-16-1- 0121. This work utilized the Janus supercomputer, which is supported 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.subjecthigh-order harmonic generationes_ES
dc.subjectUltrafast phenomenaes_ES
dc.subjectX-ray beams & opticses_ES
dc.subjectAtomic gaseses_ES
dc.subjectX-ray laserses_ES
dc.subjectAtomic orbitales_ES
dc.subjectBound stateses_ES
dc.subjectDipole approximationes_ES
dc.subjectNonperturbative methodses_ES
dc.subjectPlane wavees_ES
dc.subjectSchroedinger equationes_ES
dc.subjectStrong-field approximationes_ES
dc.titleSchemes for generation of isolated attosecond pulses of pure circular polarizationes_ES
dc.typeinfo:eu-repo/semantics/articlees_ES
dc.identifier.doi10.1103/PhysRevA.93.043855
dc.relation.projectIDREA Grant Agreement No. 328334es_ES
dc.relation.projectIDSA116U13 - UIC016es_ES
dc.relation.projectIDFIS2013-44174-Pes_ES
dc.relation.projectIDFIS2015-71933-REDTes_ES
dc.rights.accessRightsinfo:eu-repo/semantics/openAccesses_ES
dc.identifier.essn2469-9934
dc.journal.titlePhysical Review Aes_ES
dc.volume.number93es_ES
dc.issue.number4es_ES
dc.type.hasVersioninfo:eu-repo/semantics/publishedVersiones_ES


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