Utilize este identificador para referenciar este registo: http://hdl.handle.net/10071/7099
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dc.contributor.authorPathak, V. B.-
dc.contributor.authorVieira, J.-
dc.contributor.authorFonseca, R. A.-
dc.contributor.authorSilva, L. O.-
dc.date.accessioned2014-05-06T14:22:30Z-
dc.date.available2014-05-06T14:22:30Z-
dc.date.issued2012-
dc.identifier.issn1367-2630por
dc.identifier.urihttps://ciencia.iscte-iul.pt/public/pub/id/11212en_US
dc.identifier.urihttp://hdl.handle.net/10071/7099-
dc.descriptionWOS:000302310200002 (Nº de Acesso Web of Science)-
dc.description“Prémio Científico ISCTE-IUL 2013”-
dc.description.abstractThe role of laser frequency chirps in the laser wakefield accelerator is examined. We show that in the linear regime, the evolution of the laser pulse length is affected by the frequency chirp, and that positive (negative) chirp compresses (stretches) the laser pulse, thereby increasing (decreasing) the peak vector potential and wakefield amplitude. In the blowout regime, the frequency chirp can be used to fine-tune the localized etching rates at the front of the laser. In our simulations, chirped laser pulses can lead to 15% higher self-trapped electrons and 10% higher peak energies as compared to the transform-limited pulse. Chirps may be used to control the phase velocity of the wake and to relax the self-guiding conditions at the front of the laser. Our predictions are confirmed by multi-dimensional particle-in-cell simulations with OSIRIS.por
dc.language.isoengpor
dc.publisherIOP Publishing Ltdpor
dc.rightsopenAccesspor
dc.titleEffect of the frequency chirp on laser wakefield accelerationpor
dc.typearticleen_US
dc.pagination23057por
dc.publicationstatusPublicadopor
dc.peerreviewedSimpor
dc.relation.publisherversionThe definitive version is available at: http://dx.doi.org/10.1088/1367-2630/14/2/023057por
dc.journalNew Journal of Physicspor
dc.distributionInternacionalpor
dc.volume14por
degois.publication.firstPage23057por
degois.publication.titleNew Journal of Physicspor
dc.date.updated2014-05-06T14:19:55Z-
dc.identifier.doi10.1088/1367-2630/14/2/023057-
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