Abstract

The analysis of the spectrum of four-times-ionized yttrium, Y V, was extended to provide a large number of new spectrum lines and energy levels. The new analysis is based on spectrograms made with sliding-spark discharges on 10.7 m normal- and grazing-incidence spectrographs. The measurements cover the region 184–2549 Å. The results revise levels for this spectrum by Zahid-Ali et al. (1975) and by Ateqad et al. (1984). Five hundred and seventy lines were classified as transitions between 23 odd-parity and 90 even-parity levels. The 4s24p5, 4s4p6, 4s24p44d, 5s, 5p, 5d, 6s configurations are now complete. Results for the 4s24p46d and 7s configurations are tentative. Ritz-type wavelengths were determined from the optimized energy levels, with uncertainties as low as ±0.0004 Å. The observed configurations were interpreted with Hartree-Fock calculations and least-squares fits of the energy parameters to the observed levels. Oscillator strengths for all classified lines were calculated with the fitted parameters. The results are compared with values for the level energies, percentage compositions, and transition probabilities from recent ab initio theoretical calculations. The ionization energy was revised to 607,760 ± 300 cm−1 (75.353 ± 0.037 eV).

Highlights

  • The four-times ionized yttrium atom, Y V, has a Br-like electronic structure with ground configuration 4s2 4p5 and excited states 4s4p6 and 4s2 4p4 nl

  • The results are compared with values for the level energies, percentage compositions, and transition probabilities from recent ab initio theoretical calculations

  • The ionization energy was revised to 607,760 ± 300 cm−1 (75.353 ± 0.037 eV)

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Summary

Introduction

The four-times ionized yttrium atom, Y V, has a Br-like electronic structure with ground configuration 4s2 4p5 and excited states 4s4p6 and 4s2 4p4 nl. A start on this revision came in 1970, when Reader and Epstein [3] observed the true 4s2 4p5 2 P1/2,3/2 -4s4p6 2 S1/2 transitions, obtaining the position of 4s4p6 2 S1/2 and a revised value for the 2 P term splitting. Their splitting of 12,459.9 ± 3.0 cm−1 was close to the value predicted by Edlén. In 1972 Reader and Epstein [4] observed further transitions to the 4s2 4p5 2 P ground term and established most levels of the 4s2 4p4 4d and 5s configurations.

Experiment
Spectrum Analysis and Level Values
Structure
Structures
Odd Parity Configurations
Even Parity Configurations
Ritz Wavelengths
Oscillator Strengths
Ionization Energy
Comparison with ab Initio Calculations
Full Text
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