Single and double ionization of strontium in the vicinity of four-photon excitation of the 5p(2) (1)S(0) doubly excited state

dc.contributor.authorLiontos, I.en
dc.contributor.authorCohen, S.en
dc.contributor.authorBolovinos, A.en
dc.date.accessioned2015-11-24T18:35:28Z
dc.date.available2015-11-24T18:35:28Z
dc.identifier.issn0953-4075-
dc.identifier.urihttps://olympias.lib.uoi.gr/jspui/handle/123456789/17100
dc.rightsDefault Licence-
dc.subjectmultiphoton double ionizationen
dc.subjectlaser optogalvanic spectroscopyen
dc.subjectabove-threshold ionizationen
dc.subjectmulti-photon ionizationen
dc.subjectautoionizing statesen
dc.subjecteven-parityen
dc.subjecttheoretical-analysisen
dc.subjectpicosecond pulsesen
dc.subjectcharged ionsen
dc.subjectba atomsen
dc.titleSingle and double ionization of strontium in the vicinity of four-photon excitation of the 5p(2) (1)S(0) doubly excited stateen
heal.abstractWe report on the single and double multiphoton ionization of ground state Sr atoms observed in an atomic beam experiment with laser pulses of similar to 5 ns duration, maximum intensity similar to 4 x 10(11) W cm(-2) and within the 710-740 nm wavelength range. The Sr(+) spectrum consists of two strong lines originating from three-photon resonant four-photon ionization of bound states, a number of weak autoionizing resonances and a broad line due to four-photon excitation of the doubly excited 5p(2) (1)S(0) state. The latter, along with a strong, broad and structured spectral feature, is also evident in the wavelength dependence of the doubly charged Sr(2+) ion. A weakly evident but reproducible inflection point ('knee' structure) appears in the intensity dependence of the Sr(2+) yield at the location of the 5p2 1S0 resonance. A complementary fluorescence experiment revealed the accumulation of population in the 5p(1/2,3/2), 6s(1/2) and 5d(3/2,5/2) excited Sr(+) states during the laser pulse. All fluorescence signals depend on laser wavelength in a manner similar to the recorded Sr(+) spectrum. The population accumulation in the 5p(1/2,3/2) ionic states unambiguously proves the absorption of two photons above the first 5s(1/2) atomic threshold while that of the 5d(3/2),(5/2) and 6s(1/2) ones suggest the absorption of at least two more. Since under our laser pulse duration and intensity the absorption of such a number of photons in an unstructured continuum is highly improbable, it may be concluded that the process is mediated by dense manifolds of near-resonant doubly excited states, their role in the dynamics of laser - atom interaction under our conditions being far more crucial than in studies conducted using intense ultrashort pulses.en
heal.accesscampus-
heal.fullTextAvailabilityTRUE-
heal.identifier.primaryDoi 10.1088/0953-4075/41/4/045601-
heal.identifier.secondary<Go to ISI>://000253547600025-
heal.identifier.secondaryhttp://iopscience.iop.org/0953-4075/41/4/045601/pdf/0953-4075_41_4_045601.pdf-
heal.journalNameJournal of Physics B-Atomic Molecular and Optical Physicsen
heal.journalTypepeer reviewed-
heal.languageen-
heal.publicationDate2008-
heal.recordProviderΠανεπιστήμιο Ιωαννίνων. Σχολή Επιστημών και Τεχνολογιών. Τμήμα Βιολογικών Εφαρμογών και Τεχνολογιώνel
heal.typejournalArticle-
heal.type.elΆρθρο Περιοδικούel
heal.type.enJournal articleen

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