1993
DOI: 10.1051/jp4:1993621
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First observation of a Fano profile following one step autoionization into a double photoionization continuum

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Cited by 16 publications
(22 citation statements)
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References 20 publications
(26 reference statements)
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“…(18)]. For this reason, for each partial cross section, we will fix the parameters already obtained from the fit of the total cross section (E r , , and q) and will only leave three free parameters: Re(α μ ), Im(α μ ), (17), by introducing the new parameters C 1μ and C 2μ [87] defined as…”
Section: Photoionization Of Ne At XCI Levelmentioning
confidence: 99%
“…(18)]. For this reason, for each partial cross section, we will fix the parameters already obtained from the fit of the total cross section (E r , , and q) and will only leave three free parameters: Re(α μ ), Im(α μ ), (17), by introducing the new parameters C 1μ and C 2μ [87] defined as…”
Section: Photoionization Of Ne At XCI Levelmentioning
confidence: 99%
“…This effect is referred to as the presence of Fano zeros that do not depend on the optical-field strength. Experimental evidence of the Fano zeros has been brought, e.g., in [4]. In general, there exist N Fano zeros in a system with N discrete levels [1].…”
Section: Introductionmentioning
confidence: 99%
“…In this approximation, just two reduced E1 matrix elements J f = 1/2 m α m a 1 1 (r m ) J = 1/2, 3/2 need to be calculated in order to obtain the transition amplitude (4), where we have omitted the electron configurations for the sake of brevity. The two |J = 1/2, 3/2 resonances overlap each other and cannot be resolved spectroscopically [40][41][42][43]. In the computations, we use the experimentally known data 0.199 eV and 66.41 eV for the total linewidth Γ tot and the central excitation energy E exc [43].…”
Section: Resultsmentioning
confidence: 99%