Abstract:
We report detailed experimental studies on the spectra of barium using the two-step
excitation scheme to measure the absolute photoionization cross section from excited
states and the optical oscillator strengths of the Rydberg transitions. In addition, the line
shapes of the autoionizing resonances have been studied using various channels
approached by different intermediate levels and extensive new measurements of the
highly excited even parity autoionizing resonances is presented. Furthermore, the proper
line shape of the 6p2 1S0 autoionizing resonance has been reported experimentally for the
first time.
In the first set of experiments, the photoionization cross section from the 6s6p
1,3
P1
excited states have been measured in the energy region from the first ionization threshold
up to 1.69 eV excess energy. The experiments have been performed using a thermionic
diode ion detector in conjunction with a Nd: YAG laser system. The absolute values of
the photoionization cross section from the 6s6p 1P1 and 3P1 excited states at the first
ionization threshold have been determined as 90 ± 14 Mb and 102 ± 15 Mb respectively.
The studies have been extended to determine the measurements of the oscillator strengths
of the 6s6p 1P1 → 6snd 1D2 (20 ≤ n ≤ 76) and 6s6p 3P1 → 6snd 3D2 (20 ≤ n ≤ 63) Rydberg
transitions. The measured absolute photoionization cross-sections from the 6s6p 1P1 and
6s6p 3P1 states have been used to calibrate the f-values of the Rydberg transitions. The
oscillator strength densities in the continuum corresponding to the 6s6p 3P1 excited state
have also been determined.
In the next set of experiments, we have investigated how the line shape and width of an
autoionizing resonance varies by choosing different excitation paths and a systematic line
shape analysis of the 6p7p configuration based 1P1, 3D1 and 3P1 autoionizing resonances
are presented. These even parity isolated autoionizing resonances have been accessed via
four different intermediate states 6snp 1P1 (6 ≤ n ≤ 8) and 5d6p 1P1. A comparison of the
Fano parameters of the resonance profiles reveals that the width of an autoionizing
resonance remains constant while the line profile parameter changes with the selection of
different intermediate states.