chan_1992#
W. F. Chan, G. Cooper, X. Guo, G. R. Burton, and C. E. Brion, Phys. Rev. A 46, 149 (1992)
Source record · Catalogue · Review register
Source kind: measurement
Recorded technique: Dipole (e,e) spectroscopy: fast-electron energy-loss spectra at zero scattering angle (optical limit) converted to relative optical oscillator strengths with the spectrometer’s Bethe-Born factor. Low resolution (about 1 eV FWHM, 8 keV impact energy): Ar 10-500, Kr 8-380, Xe 7-398 eV. High resolution (0.048 eV FWHM, 3 keV; also 0.072 and 0.098 eV): the discrete spectra and the ms autoionising resonances, peaks fitted where unresolved. Absolute scales by single-point normalisation to Samson and Yin’s (1989) photoabsorption cross sections at 21.218 eV (Ar, Kr) and 16.848 eV (Xe), in smooth continuum; no line-saturation effects (pp. 150-151). Energy scales calibrated on 11.828 eV (Ar), 10.033 eV (Kr), 8.437 eV (Xe) (low resolution) and the He 21.218 eV line admitted with the sample (high resolution).
Materials in structured entries: Ar, Kr, Xe
Dataset quantities: differential_oscillator_strength, oscillator_strength
Contents: 90 datasets; 0 formulas.
Curation notes#
Part III of the series (journal pages 149-171 = PDF pages 1-23) (He: Chan et al. 1991, Ne: Chan et al. 1992, Phys. Rev. A 45, 1420, curated as chan_1992_neon). Values per atom; no density or state involved.
Continuum (Tables I-III): df/dE in 10^-2 eV^-1 at photon energy E (eV), ‘uncertainties ... estimated to be ~5%’ (p. 151); sigma(Mb) = 109.75 df/dE(eV^-1) (table notes). The first rows (16.0 eV Ar, 14.7 eV Kr, 13.5 eV Xe) are just above the first ionisation potential; the 1 eV resolution smooths the autoionising structure (shown at high resolution in Figs. 14-16 only, not tabulated). Argon Table I (continued) prints ‘208.0’ for 308.0 eV (erratum).
Discrete lines (Tables IV-IX): the present oscillator strengths with their estimated uncertainties in parentheses (5 % for the resonance lines, 10 % for the others), and the literature values the tables compare, each extracted as a reproduced dataset per source and gas (one file per source combining the two tables of a gas; energies are the table headers’ transition energies from Moore’s tables). Resonance lines: Ar a_1 = 4s 11.624 eV, a_2 = 4s’ 11.828 eV; Kr b_1 = 5s 10.033, b_2 = 5s’ 10.644 eV; Xe c_1 = 6s 8.437, c_2 = 6s’ 9.570 eV. The ‘Oscillator strength ratio’ columns (a_1/a_2 etc.) are derived and not extracted; every printed ratio agrees with its row’s values to 0.001 except Lewis’s xenon row (see its dataset). Upper limits are not extracted: present work Xe ‘<0.001’ at 10.979, 11.495 and 11.583 eV; Geiger [83] Ar ‘<0.0025’ at 13.864 eV. Summed theory values (note b, a_1 + a_2 etc.) and the ‘Total to ionization’ column are separate datasets with an index abscissa. The text gives the present sums a_1 + a_2 = 0.331 and b_1 + b_2 = 0.407 (pp. 163, 166), and the totals 0.859 (Ar), 1.126 (Kr), 1.606 (Xe), compared with 0.82 (Lee), 0.827 (Natali et al.), 1.10 (Natali et al.), 1.640 (Geiger), and Eggarter’s (1975) 0.793 for Ar (pp. 165-168, text only, not extracted).
Transition labels: the header underlines distinguish nd[3/2] from nd[1/2] (Tables V, VII, IX note a); the library cells lose the underline, so labels such as ‘(2P3/2)6d’ repeat. The row ids are the energies, which are unique; the labels are kept in the printed column.
Erratum: the authors’ erratum, Phys. Rev. A 48, 858 (1993) (chan_1993_erratum), reprints Tables V, VII and IX whole because ‘some values ... were incorrectly positioned’: three rows printed one value for an unresolved group of lines under every line of the group (present work Ar 7s + 5d-underlined; Geiger [82] Kr 5d-underlined + 7s and 6d-underlined + 8s; Delage and Carette [81] Xe 9s + 5d’ and 8d + 8d-underlined + 10s). The files keep the 1992 printing; each group’s value is kept once, at the row of the group’s strongest line in the present work (for the unresolved Ar pair, in Natali et al.’s resolved values), and the repeats are excluded_rows (TC-710).
Sums of the discrete tables are not sum-rule checks: the tables stop below the 2P_3/2 threshold and omit higher members. Not extracted: the autoionising-region spectra (Figs. 14-16, figures only).
Recorded bibliographic identity status: VALIDATED_WITH_WARNINGS. This concerns identification of the source; it does not establish the scientific correctness of its contents.
Datasets#
chan_1992/continuum_Ar#
{
"id": "continuum_Ar",
"material": "Ar",
"file": "Ar/chan_1992__continuum_Ar.csv",
"table": "tbl_7266df86dba6, tbl_41f17cecf0c6",
"quantity": "differential_oscillator_strength",
"unit": "1/eV",
"scale": 0.01,
"abscissa_unit": "eV",
"use": "primary",
"uncertainty": {
"relative": 0.05,
"level": "not stated"
}
}
Table I and its continuation: df/dE (10^-2 eV^-1) at 16.0-500 eV, 450 points, rows numbered in reading order (column by column). Normalised to Samson and Yin at 21.218 eV (the 21.2 eV row, mark a). Row 333 prints 208.0 eV for 308.0 (erratum).
chan_1992/continuum_Kr#
{
"id": "continuum_Kr",
"material": "Kr",
"file": "Kr/chan_1992__continuum_Kr.csv",
"table": "tbl_bd52d819c303, tbl_5de368f90d0b",
"quantity": "differential_oscillator_strength",
"unit": "1/eV",
"scale": 0.01,
"abscissa_unit": "eV",
"use": "primary",
"uncertainty": {
"relative": 0.05,
"level": "not stated"
}
}
Table II and its continuation: df/dE (10^-2 eV^-1) at 14.7-380 eV, 287 points, rows numbered in reading order. Normalised to Samson and Yin at 21.218 eV (the 21.0 eV row carries mark a).
chan_1992/continuum_Xe#
{
"id": "continuum_Xe",
"material": "Xe",
"file": "Xe/chan_1992__continuum_Xe.csv",
"table": "tbl_70c8cd79d2c0, tbl_5469ba982e92",
"quantity": "differential_oscillator_strength",
"unit": "1/eV",
"scale": 0.01,
"abscissa_unit": "eV",
"use": "primary",
"uncertainty": {
"relative": 0.05,
"level": "not stated"
}
}
Table III and its continuation: df/dE (10^-2 eV^-1) at 13.5-398 eV, 251 points, rows numbered in reading order. Normalised to Samson and Yin at 16.848 eV (the 16.8 eV row, mark a).
chan_1992/present_Ar#
{
"id": "present_Ar",
"material": "Ar",
"file": "Ar/chan_1992__present_Ar.csv",
"table": "tbl_8988f801b4d2, tbl_699514709b3b",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "primary",
"excluded_rows": {
"15.186": "A repeat: the authors' erratum (Phys. Rev. A 48, 858 (1993), Table V(b)) prints 0.0426 once for the unresolved 7s (15.186 eV) and 5d-underlined (15.190 eV) pair; kept at 15.190 eV (TC-710)."
},
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table IV and Table V: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); the present high-resolution dipole (e,e) measurement (0.048 eV FWHM), normalised to Samson and Yin at 21.218 eV (Ar, Kr) or 16.848 eV (Xe). Sub-table V(b) prints 0.0426(0.0043) under both 7s (15.186 eV) and 5d(underlined) (15.190 eV), 4 meV apart (image checked; TC-68). The authors’ erratum (chan_1993_erratum, Table V(b)) reprints it once, under a brace spanning both lines, with uncertainty 0.0063: one value for the unresolved pair. Kept once, at 15.190 eV (the stronger of the pair in Natali et al.’s resolved 0.0139 and 0.0234), with the erratum’s uncertainty; the 15.186 eV repeat is excluded (TC-710).
chan_1992/present_total_Ar#
{
"id": "present_total_Ar",
"material": "Ar",
"file": "Ar/chan_1992__present_total_Ar.csv",
"table": "tbl_699514709b3b",
"quantity": "oscillator_strength",
"abscissa": "label",
"use": "check",
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table V: ‘Total to ionization’: the discrete oscillator-strength sum up to the 2P_3/2 threshold, index abscissa; the present high-resolution dipole (e,e) measurement (0.048 eV FWHM), normalised to Samson and Yin at 21.218 eV (Ar, Kr) or 16.848 eV (Xe). A sum over the lines of the present-work line dataset and the unlisted higher members: a check, not fitted beside them. Its uncertainty is misprinted (0.0043) (erratum).
chan_1992/albat_1975_Ar#
{
"id": "albat_1975_Ar",
"material": "Ar",
"file": "Ar/chan_1992__albat_1975_Ar.csv",
"table": "tbl_8988f801b4d2",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"R. Albat, N. Gruen, and B. Wirsam, J. Phys. B 8, L82 (1975)"
]
}
Table IV: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); theory.
chan_1992/amusya_1990_sum_Ar#
{
"id": "amusya_1990_sum_Ar",
"material": "Ar",
"file": "Ar/chan_1992__amusya_1990_sum_Ar.csv",
"table": "tbl_8988f801b4d2",
"quantity": "oscillator_strength",
"abscissa": "label",
"use": "reproduced",
"reproduced_from": [
"M. Ya. Amus'ya, Atomic Photoeffect (Plenum, New York, 1990), p. 170"
]
}
Table IV: summed oscillator strength of the two resonance lines (note b; printed between the columns), index abscissa; theory, RPAE.
chan_1992/aymar_1970_length_Ar#
{
"id": "aymar_1970_length_Ar",
"material": "Ar",
"file": "Ar/chan_1992__aymar_1970_length_Ar.csv",
"table": "tbl_8988f801b4d2",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"M. Aymar, S. Feneuille, and M. Klapisch, Nucl. Instrum. Methods 90, 137 (1970)"
]
}
Table IV: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); theory, dipole length.
chan_1992/aymar_1970_velocity_Ar#
{
"id": "aymar_1970_velocity_Ar",
"material": "Ar",
"file": "Ar/chan_1992__aymar_1970_velocity_Ar.csv",
"table": "tbl_8988f801b4d2",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"M. Aymar, S. Feneuille, and M. Klapisch, Nucl. Instrum. Methods 90, 137 (1970)"
]
}
Table IV: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); theory, dipole velocity.
chan_1992/chamberlain_1965_Ar#
{
"id": "chamberlain_1965_Ar",
"material": "Ar",
"file": "Ar/chan_1992__chamberlain_1965_Ar.csv",
"table": "tbl_8988f801b4d2",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"G. E. Chamberlain, J. G. M. Heideman, J. A. Simpson, and C. E. Kuyatt, Abstracts, Fourth International Conference on the Physics of Electronic and Atomic Collisions, Quebec, 1965 (Science Bookcrafters, 1968)"
]
}
Table IV: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); electron impact.
chan_1992/chornay_1984_Ar#
{
"id": "chornay_1984_Ar",
"material": "Ar",
"file": "Ar/chan_1992__chornay_1984_Ar.csv",
"table": "tbl_8988f801b4d2",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"D. J. Chornay, G. C. King, and S. J. Buckman, J. Phys. B 17, 3173 (1984)"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table IV: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); lifetime, electron-photon coincidence.
chan_1992/cooper_1962_sum_Ar#
{
"id": "cooper_1962_sum_Ar",
"material": "Ar",
"file": "Ar/chan_1992__cooper_1962_sum_Ar.csv",
"table": "tbl_8988f801b4d2",
"quantity": "oscillator_strength",
"abscissa": "label",
"use": "reproduced",
"reproduced_from": [
"J. W. Cooper, Phys. Rev. 128, 681 (1962)"
]
}
Table IV: summed oscillator strength of the two resonance lines (note b; printed between the columns), index abscissa; theory, one-electron central potential.
chan_1992/copley_1974_Ar#
{
"id": "copley_1974_Ar",
"material": "Ar",
"file": "Ar/chan_1992__copley_1974_Ar.csv",
"table": "tbl_8988f801b4d2",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"G. H. Copley and D. M. Camm, J. Quant. Spectrosc. Radiat. Transfer 14, 899 (1974)"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table IV: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); pressure-broadening profile.
chan_1992/de_jongh_1971_Ar#
{
"id": "de_jongh_1971_Ar",
"material": "Ar",
"file": "Ar/chan_1992__de_jongh_1971_Ar.csv",
"table": "tbl_8988f801b4d2",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"J. P. De Jongh and J. Van Eck, Physica 51, 104 (1971)"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table IV: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); relative self-absorption.
chan_1992/geiger_1970_Ar#
{
"id": "geiger_1970_Ar",
"material": "Ar",
"file": "Ar/chan_1992__geiger_1970_Ar.csv",
"table": "tbl_8988f801b4d2",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"J. Geiger, Phys. Lett. 33A, 351 (1970)"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table IV: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); electron impact.
chan_1992/geiger_unpublished_Ar#
{
"id": "geiger_unpublished_Ar",
"material": "Ar",
"file": "Ar/chan_1992__geiger_unpublished_Ar.csv",
"table": "tbl_8988f801b4d2, tbl_699514709b3b",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"J. Geiger, unpublished, as quoted in W. B. Westerveld et al. (1979) and J. Berkowitz, Photoabsorption, Photoionization and Photoelectron Spectroscopy (Academic, 1979), p. 80"
]
}
Table IV and Table V: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); electron impact (Ref. [83]).
chan_1992/gruzdev_1967_Ar#
{
"id": "gruzdev_1967_Ar",
"material": "Ar",
"file": "Ar/chan_1992__gruzdev_1967_Ar.csv",
"table": "tbl_8988f801b4d2",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"P. F. Gruzdev, Opt. Spectrosc. 22, 170 (1967)"
]
}
Table IV: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); theory.
chan_1992/gruzdev_loginov_1975a_Ar#
{
"id": "gruzdev_loginov_1975a_Ar",
"material": "Ar",
"file": "Ar/chan_1992__gruzdev_loginov_1975a_Ar.csv",
"table": "tbl_8988f801b4d2",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"P. F. Gruzdev and A. V. Loginov, Opt. Spektrosk. 38, 411 (1975) [Opt. Spectrosc. 38, 234 (1975)]"
]
}
Table IV: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); theory.
chan_1992/irwin_1973_Ar#
{
"id": "irwin_1973_Ar",
"material": "Ar",
"file": "Ar/chan_1992__irwin_1973_Ar.csv",
"table": "tbl_8988f801b4d2",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"D. Irwin, A. E. Livingston, and J. A. Kernahan, Nucl. Instrum. Methods 110, 111 (1973)"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table IV: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); lifetime, beam foil.
chan_1992/knox_1958_semiempirical_Ar#
{
"id": "knox_1958_semiempirical_Ar",
"material": "Ar",
"file": "Ar/chan_1992__knox_1958_semiempirical_Ar.csv",
"table": "tbl_8988f801b4d2",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"R. S. Knox, Phys. Rev. 110, 375 (1958)"
]
}
Table IV: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); theory, semiempirical.
chan_1992/knox_1958_wave_function_Ar#
{
"id": "knox_1958_wave_function_Ar",
"material": "Ar",
"file": "Ar/chan_1992__knox_1958_wave_function_Ar.csv",
"table": "tbl_8988f801b4d2",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"R. S. Knox, Phys. Rev. 110, 375 (1958)"
]
}
Table IV: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); theory, wave function.
chan_1992/kuyatt_1975_Ar#
{
"id": "kuyatt_1975_Ar",
"material": "Ar",
"file": "Ar/chan_1992__kuyatt_1975_Ar.csv",
"table": "tbl_8988f801b4d2",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"C. E. Kuyatt, private communication quoted in E. Eggarter, J. Chem. Phys. 62, 833 (1975)"
]
}
Table IV: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); electron impact (Ref. [96]).
chan_1992/lawrence_1968_Ar#
{
"id": "lawrence_1968_Ar",
"material": "Ar",
"file": "Ar/chan_1992__lawrence_1968_Ar.csv",
"table": "tbl_8988f801b4d2, tbl_699514709b3b",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"G. M. Lawrence, Phys. Rev. 175, 40 (1968)"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table IV and Table V: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); lifetime, delayed coincidence.
chan_1992/lee_1974_Ar#
{
"id": "lee_1974_Ar",
"material": "Ar",
"file": "Ar/chan_1992__lee_1974_Ar.csv",
"table": "tbl_8988f801b4d2, tbl_699514709b3b",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"C. M. Lee, Phys. Rev. A 10, 584 (1974)"
]
}
Table IV and Table V: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); theory.
chan_1992/lee_1974_total_Ar#
{
"id": "lee_1974_total_Ar",
"material": "Ar",
"file": "Ar/chan_1992__lee_1974_total_Ar.csv",
"table": "tbl_699514709b3b",
"quantity": "oscillator_strength",
"abscissa": "label",
"use": "reproduced",
"reproduced_from": [
"C. M. Lee, Phys. Rev. A 10, 584 (1974)"
]
}
Table V: ‘Total to ionization’: the discrete oscillator-strength sum up to the 2P_3/2 threshold, index abscissa; theory.
chan_1992/lee_lu_1973_Ar#
{
"id": "lee_lu_1973_Ar",
"material": "Ar",
"file": "Ar/chan_1992__lee_lu_1973_Ar.csv",
"table": "tbl_8988f801b4d2, tbl_699514709b3b",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"C. M. Lee and K. T. Lu, Phys. Rev. A 8, 1241 (1973)"
]
}
Table IV and Table V: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); theory.
chan_1992/lewis_1967_Ar#
{
"id": "lewis_1967_Ar",
"material": "Ar",
"file": "Ar/chan_1992__lewis_1967_Ar.csv",
"table": "tbl_8988f801b4d2",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"E. L. Lewis, Proc. Phys. Soc. 92, 817 (1967)"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table IV: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); pressure-broadening profile. The 4s’ uncertainty is printed (0.002), 0.7 %, against (0.004) on 4s; possibly (0.02). Kept as printed.
chan_1992/li_1988_Ar#
{
"id": "li_1988_Ar",
"material": "Ar",
"file": "Ar/chan_1992__li_1988_Ar.csv",
"table": "tbl_8988f801b4d2",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"G. P. Li, T. Takayanagi, K. Wakiya, H. Suzuki, T. Ajiro, S. Yagi, S. S. Kano, and H. Takuma, Phys. Rev. A 38, 1240 (1988)"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table IV: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); electron impact.
chan_1992/mcconkey_1973_Ar#
{
"id": "mcconkey_1973_Ar",
"material": "Ar",
"file": "Ar/chan_1992__mcconkey_1973_Ar.csv",
"table": "tbl_8988f801b4d2",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"J. W. McConkey and F. G. Donaldson, Can. J. Phys. 51, 914 (1973)"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table IV: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); electron excitation function.
chan_1992/morack_1967_Ar#
{
"id": "morack_1967_Ar",
"material": "Ar",
"file": "Ar/chan_1992__morack_1967_Ar.csv",
"table": "tbl_8988f801b4d2",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"J. L. Morack and C. E. Fairchild, Phys. Rev. 163, 125 (1967)"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table IV: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); lifetime, delayed coincidence.
chan_1992/natali_unpublished_Ar#
{
"id": "natali_unpublished_Ar",
"material": "Ar",
"file": "Ar/chan_1992__natali_unpublished_Ar.csv",
"table": "tbl_8988f801b4d2, tbl_699514709b3b",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"S. Natali, C. E. Kuyatt, and S. R. Miekzarek, unpublished, as quoted in Chan et al.'s Refs. [53,83,88]"
]
}
Table IV and Table V: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); electron impact (Ref. [87]).
chan_1992/natali_unpublished_total_Ar#
{
"id": "natali_unpublished_total_Ar",
"material": "Ar",
"file": "Ar/chan_1992__natali_unpublished_total_Ar.csv",
"table": "tbl_699514709b3b",
"quantity": "oscillator_strength",
"abscissa": "label",
"use": "reproduced",
"reproduced_from": [
"S. Natali, C. E. Kuyatt, and S. R. Miekzarek, unpublished, as quoted in Chan et al.'s Refs. [53,83,88]"
]
}
Table V: ‘Total to ionization’: the discrete oscillator-strength sum up to the 2P_3/2 threshold, index abscissa; electron impact (Ref. [87]).
chan_1992/stewart_1975_Ar#
{
"id": "stewart_1975_Ar",
"material": "Ar",
"file": "Ar/chan_1992__stewart_1975_Ar.csv",
"table": "tbl_8988f801b4d2",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"R. F. Stewart, Mol. Phys. 30, 745 (1975)"
]
}
Table IV: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); theory.
chan_1992/tsurubuchi_1990_Ar#
{
"id": "tsurubuchi_1990_Ar",
"material": "Ar",
"file": "Ar/chan_1992__tsurubuchi_1990_Ar.csv",
"table": "tbl_8988f801b4d2",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"S. Tsurubuchi, K. Watanabe, and T. Arikawa, J. Phys. Soc. Jpn. 59, 497 (1990)"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table IV: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); absolute self-absorption.
chan_1992/vallee_1977_Ar#
{
"id": "vallee_1977_Ar",
"material": "Ar",
"file": "Ar/chan_1992__vallee_1977_Ar.csv",
"table": "tbl_8988f801b4d2",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"O. Vallee, P. Ranson, and J. Chapelle, J. Quant. Spectrosc. Radiat. Transfer 18, 327 (1977)"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table IV: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); pressure-broadening profile.
chan_1992/westerveld_1979_Ar#
{
"id": "westerveld_1979_Ar",
"material": "Ar",
"file": "Ar/chan_1992__westerveld_1979_Ar.csv",
"table": "tbl_8988f801b4d2, tbl_699514709b3b",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"W. B. Westerveld, Th. F. A. Mulder, and J. Van Eck, J. Quant. Spectrosc. Radiat. Transfer 21, 533 (1979)"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table IV and Table V: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); absolute self-absorption.
chan_1992/wiese_1969_Ar#
{
"id": "wiese_1969_Ar",
"material": "Ar",
"file": "Ar/chan_1992__wiese_1969_Ar.csv",
"table": "tbl_699514709b3b",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"W. L. Wiese, M. W. Smith, and B. M. Miles, Atomic Transition Probabilities: Sodium through Calcium, NSRDS-NBS 22, Vol. II (U.S. GPO, Washington, D.C., 1969)"
]
}
Table V: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); reanalysis of Lawrence’s lifetime data (note c). The 14.304 eV (3d’) value is misprinted 0.0106 (erratum).
chan_1992/present_Kr#
{
"id": "present_Kr",
"material": "Kr",
"file": "Kr/chan_1992__present_Kr.csv",
"table": "tbl_85dda44edbca, tbl_0dd5fa4f52b5",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "primary",
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table VI and Table VII: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); the present high-resolution dipole (e,e) measurement (0.048 eV FWHM), normalised to Samson and Yin at 21.218 eV (Ar, Kr) or 16.848 eV (Xe).
chan_1992/present_total_Kr#
{
"id": "present_total_Kr",
"material": "Kr",
"file": "Kr/chan_1992__present_total_Kr.csv",
"table": "tbl_0dd5fa4f52b5",
"quantity": "oscillator_strength",
"abscissa": "label",
"use": "check",
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table VII: ‘Total to ionization’: the discrete oscillator-strength sum up to the 2P_3/2 threshold, index abscissa; the present high-resolution dipole (e,e) measurement (0.048 eV FWHM), normalised to Samson and Yin at 21.218 eV (Ar, Kr) or 16.848 eV (Xe). A sum over the lines of the present-work line dataset and the unlisted higher members: a check, not fitted beside them.
chan_1992/amusya_1990_sum_Kr#
{
"id": "amusya_1990_sum_Kr",
"material": "Kr",
"file": "Kr/chan_1992__amusya_1990_sum_Kr.csv",
"table": "tbl_85dda44edbca",
"quantity": "oscillator_strength",
"abscissa": "label",
"use": "reproduced",
"reproduced_from": [
"M. Ya. Amus'ya, Atomic Photoeffect (Plenum, New York, 1990), p. 170"
]
}
Table VI: summed oscillator strength of the two resonance lines (note b; printed between the columns), index abscissa; theory, RPAE.
chan_1992/aymar_1970_length_Kr#
{
"id": "aymar_1970_length_Kr",
"material": "Kr",
"file": "Kr/chan_1992__aymar_1970_length_Kr.csv",
"table": "tbl_85dda44edbca",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"M. Aymar, S. Feneuille, and M. Klapisch, Nucl. Instrum. Methods 90, 137 (1970)"
]
}
Table VI: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); theory, dipole length.
chan_1992/aymar_1970_velocity_Kr#
{
"id": "aymar_1970_velocity_Kr",
"material": "Kr",
"file": "Kr/chan_1992__aymar_1970_velocity_Kr.csv",
"table": "tbl_85dda44edbca",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"M. Aymar, S. Feneuille, and M. Klapisch, Nucl. Instrum. Methods 90, 137 (1970)"
]
}
Table VI: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); theory, dipole velocity.
chan_1992/aymar_coulombe_1978_length_Kr#
{
"id": "aymar_coulombe_1978_length_Kr",
"material": "Kr",
"file": "Kr/chan_1992__aymar_coulombe_1978_length_Kr.csv",
"table": "tbl_85dda44edbca",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"M. Aymar and M. Coulombe, At. Data Nucl. Data Tables 21, 537 (1978)"
]
}
Table VI: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); theory, dipole length.
chan_1992/aymar_coulombe_1978_velocity_Kr#
{
"id": "aymar_coulombe_1978_velocity_Kr",
"material": "Kr",
"file": "Kr/chan_1992__aymar_coulombe_1978_velocity_Kr.csv",
"table": "tbl_85dda44edbca",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"M. Aymar and M. Coulombe, At. Data Nucl. Data Tables 21, 537 (1978)"
]
}
Table VI: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); theory, dipole velocity.
chan_1992/chashchina_1967_Kr#
{
"id": "chashchina_1967_Kr",
"material": "Kr",
"file": "Kr/chan_1992__chashchina_1967_Kr.csv",
"table": "tbl_85dda44edbca",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"G. I. Chashchina and E. Ya. Shreider, Opt. Spectrosc. 22, 284 (1967)"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table VI: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); linear absorption.
chan_1992/cooper_1962_sum_Kr#
{
"id": "cooper_1962_sum_Kr",
"material": "Kr",
"file": "Kr/chan_1992__cooper_1962_sum_Kr.csv",
"table": "tbl_85dda44edbca",
"quantity": "oscillator_strength",
"abscissa": "label",
"use": "reproduced",
"reproduced_from": [
"J. W. Cooper, Phys. Rev. 128, 681 (1962)"
]
}
Table VI: summed oscillator strength of the two resonance lines (note b; printed between the columns), index abscissa; theory, one-electron central potential.
chan_1992/de_jongh_1971_Kr#
{
"id": "de_jongh_1971_Kr",
"material": "Kr",
"file": "Kr/chan_1992__de_jongh_1971_Kr.csv",
"table": "tbl_85dda44edbca",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"J. P. De Jongh and J. Van Eck, Physica 51, 104 (1971)"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table VI: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); relative self-absorption.
chan_1992/dow_knox_1966_semiempirical_Kr#
{
"id": "dow_knox_1966_semiempirical_Kr",
"material": "Kr",
"file": "Kr/chan_1992__dow_knox_1966_semiempirical_Kr.csv",
"table": "tbl_85dda44edbca",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"J. D. Dow and R. S. Knox, Phys. Rev. 152, 50 (1966)"
]
}
Table VI: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); theory, semiempirical.
chan_1992/dow_knox_1966_wave_function_Kr#
{
"id": "dow_knox_1966_wave_function_Kr",
"material": "Kr",
"file": "Kr/chan_1992__dow_knox_1966_wave_function_Kr.csv",
"table": "tbl_85dda44edbca",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"J. D. Dow and R. S. Knox, Phys. Rev. 152, 50 (1966)"
]
}
Table VI: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); theory, wave function.
chan_1992/ferrell_1987_Kr#
{
"id": "ferrell_1987_Kr",
"material": "Kr",
"file": "Kr/chan_1992__ferrell_1987_Kr.csv",
"table": "tbl_85dda44edbca",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"ferrell_1987"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table VI: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); phase matching.
chan_1992/geiger_1970_Kr#
{
"id": "geiger_1970_Kr",
"material": "Kr",
"file": "Kr/chan_1992__geiger_1970_Kr.csv",
"table": "tbl_85dda44edbca",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"J. Geiger, Phys. Lett. 33A, 351 (1970)"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table VI: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); electron impact.
chan_1992/geiger_1977_Kr#
{
"id": "geiger_1977_Kr",
"material": "Kr",
"file": "Kr/chan_1992__geiger_1977_Kr.csv",
"table": "tbl_85dda44edbca, tbl_0dd5fa4f52b5",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"J. Geiger, Z. Phys. A 282, 129 (1977)"
],
"excluded_rows": {
"13.099": "A repeat: the authors' erratum (Phys. Rev. A 48, 858 (1993), Table VII(b)) prints 0.187 once for the 5d-underlined (13.099 eV) and 7s (13.114 eV) blend; kept at 13.114 eV (TC-710).",
"13.437": "A repeat: the authors' erratum (Table VII(b)) prints 0.054 once for the 6d-underlined (13.423 eV) and 8s (13.437 eV) blend; kept at 13.423 eV (TC-710)."
}
}
Table VI and Table VII: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); electron impact. Sub-table (b) prints 0.187 under both 5d(underlined) and 7s and 0.054 under both 6d(underlined) and 8s (image checked). The authors’ erratum (chan_1993_erratum, Table VII(b)) prints each once under a brace: blends. Kept at the group’s strongest line in the present work (7s, 13.114 eV: 0.113 against 0.0610; 6d(underlined), 13.423 eV: 0.0439 against 0.0203); the repeats are excluded (TC-710).
chan_1992/geiger_1977_theory_Kr#
{
"id": "geiger_1977_theory_Kr",
"material": "Kr",
"file": "Kr/chan_1992__geiger_1977_theory_Kr.csv",
"table": "tbl_85dda44edbca, tbl_0dd5fa4f52b5",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"J. Geiger, Z. Phys. A 282, 129 (1977)"
]
}
Table VI and Table VII: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); semiempirical calculation (listed under Theory).
chan_1992/griffin_1969_Kr#
{
"id": "griffin_1969_Kr",
"material": "Kr",
"file": "Kr/chan_1992__griffin_1969_Kr.csv",
"table": "tbl_85dda44edbca",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"P. M. Griffin and J. W. Hutchson, J. Opt. Soc. Am. 59, 1607 (1969)"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table VI: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); total absorption.
chan_1992/gruzdev_1967_Kr#
{
"id": "gruzdev_1967_Kr",
"material": "Kr",
"file": "Kr/chan_1992__gruzdev_1967_Kr.csv",
"table": "tbl_85dda44edbca",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"P. F. Gruzdev, Opt. Spectrosc. 22, 170 (1967)"
]
}
Table VI: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); theory.
chan_1992/gruzdev_loginov_1975b_Kr#
{
"id": "gruzdev_loginov_1975b_Kr",
"material": "Kr",
"file": "Kr/chan_1992__gruzdev_loginov_1975b_Kr.csv",
"table": "tbl_85dda44edbca",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"P. F. Gruzdev and A. V. Loginov, Opt. Spektrosk. 38, 1065 (1975) [Opt. Spectrosc. 38, 611 (1975)]"
]
}
Table VI: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); theory.
chan_1992/lewis_1967_Kr#
{
"id": "lewis_1967_Kr",
"material": "Kr",
"file": "Kr/chan_1992__lewis_1967_Kr.csv",
"table": "tbl_85dda44edbca",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"E. L. Lewis, Proc. Phys. Soc. 92, 817 (1967)"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table VI: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); pressure-broadening profile.
chan_1992/matthias_1977_Kr#
{
"id": "matthias_1977_Kr",
"material": "Kr",
"file": "Kr/chan_1992__matthias_1977_Kr.csv",
"table": "tbl_85dda44edbca",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"E. Matthias, R. A. Rosenberg, E. D. Poliakoff, M. G. White, S. T. Lee, and D. A. Shirley, Chem. Phys. Lett. 52, 239 (1977)"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table VI: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); lifetime, resonance fluorescence.
chan_1992/natali_unpublished_Kr#
{
"id": "natali_unpublished_Kr",
"material": "Kr",
"file": "Kr/chan_1992__natali_unpublished_Kr.csv",
"table": "tbl_85dda44edbca, tbl_0dd5fa4f52b5",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"S. Natali, C. E. Kuyatt, and S. R. Miekzarek, unpublished, as quoted in Chan et al.'s Refs. [53,83,88]"
]
}
Table VI and Table VII: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); electron impact (Ref. [87]).
chan_1992/natali_unpublished_total_Kr#
{
"id": "natali_unpublished_total_Kr",
"material": "Kr",
"file": "Kr/chan_1992__natali_unpublished_total_Kr.csv",
"table": "tbl_0dd5fa4f52b5",
"quantity": "oscillator_strength",
"abscissa": "label",
"use": "reproduced",
"reproduced_from": [
"S. Natali, C. E. Kuyatt, and S. R. Miekzarek, unpublished, as quoted in Chan et al.'s Refs. [53,83,88]"
]
}
Table VII: ‘Total to ionization’: the discrete oscillator-strength sum up to the 2P_3/2 threshold, index abscissa; electron impact (Ref. [87]).
chan_1992/takayanagi_1990_Kr#
{
"id": "takayanagi_1990_Kr",
"material": "Kr",
"file": "Kr/chan_1992__takayanagi_1990_Kr.csv",
"table": "tbl_85dda44edbca",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"T. Takayanagi, G. P. Li, K. Wakiya, H. Suzuki, T. Ajiro, T. Inaba, S. S. Kano, and H. Takuma, Phys. Rev. A 41, 5948 (1990)"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table VI: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); electron impact.
chan_1992/tsurubuchi_1990_Kr#
{
"id": "tsurubuchi_1990_Kr",
"material": "Kr",
"file": "Kr/chan_1992__tsurubuchi_1990_Kr.csv",
"table": "tbl_85dda44edbca",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"S. Tsurubuchi, K. Watanabe, and T. Arikawa, J. Phys. Soc. Jpn. 59, 497 (1990)"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table VI: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); absolute self-absorption.
chan_1992/turner_1965_Kr#
{
"id": "turner_1965_Kr",
"material": "Kr",
"file": "Kr/chan_1992__turner_1965_Kr.csv",
"table": "tbl_85dda44edbca",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"R. Turner, Phys. Rev. 140, A426 (1965)"
]
}
Table VI: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); lifetime, resonance imprisonment.
chan_1992/wilkinson_1965_Kr#
{
"id": "wilkinson_1965_Kr",
"material": "Kr",
"file": "Kr/chan_1992__wilkinson_1965_Kr.csv",
"table": "tbl_85dda44edbca",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"P. G. Wilkinson, J. Quant. Spectrosc. Radiat. Transfer 5, 503 (1965)"
]
}
Table VI: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); total absorption.
chan_1992/present_Xe#
{
"id": "present_Xe",
"material": "Xe",
"file": "Xe/chan_1992__present_Xe.csv",
"table": "tbl_ae92208a90e7, tbl_1dbc4809ef5a",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "primary",
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table VIII and Table IX: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); the present high-resolution dipole (e,e) measurement (0.048 eV FWHM), normalised to Samson and Yin at 21.218 eV (Ar, Kr) or 16.848 eV (Xe).
chan_1992/present_total_Xe#
{
"id": "present_total_Xe",
"material": "Xe",
"file": "Xe/chan_1992__present_total_Xe.csv",
"table": "tbl_1dbc4809ef5a",
"quantity": "oscillator_strength",
"abscissa": "label",
"use": "check",
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table IX: ‘Total to ionization’: the discrete oscillator-strength sum up to the 2P_3/2 threshold, index abscissa; the present high-resolution dipole (e,e) measurement (0.048 eV FWHM), normalised to Samson and Yin at 21.218 eV (Ar, Kr) or 16.848 eV (Xe). A sum over the lines of the present-work line dataset and the unlisted higher members: a check, not fitted beside them.
chan_1992/amusya_1990_sum_Xe#
{
"id": "amusya_1990_sum_Xe",
"material": "Xe",
"file": "Xe/chan_1992__amusya_1990_sum_Xe.csv",
"table": "tbl_ae92208a90e7",
"quantity": "oscillator_strength",
"abscissa": "label",
"use": "reproduced",
"reproduced_from": [
"M. Ya. Amus'ya, Atomic Photoeffect (Plenum, New York, 1990), p. 170"
]
}
Table VIII: summed oscillator strength of the two resonance lines (note b; printed between the columns), index abscissa; theory, RPAE.
chan_1992/anderson_1965_Xe#
{
"id": "anderson_1965_Xe",
"material": "Xe",
"file": "Xe/chan_1992__anderson_1965_Xe.csv",
"table": "tbl_ae92208a90e7",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"D. K. Anderson, Phys. Rev. 137, A21 (1965)"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table VIII: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); lifetime, level crossing.
chan_1992/aymar_1970_length_Xe#
{
"id": "aymar_1970_length_Xe",
"material": "Xe",
"file": "Xe/chan_1992__aymar_1970_length_Xe.csv",
"table": "tbl_ae92208a90e7",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"M. Aymar, S. Feneuille, and M. Klapisch, Nucl. Instrum. Methods 90, 137 (1970)"
]
}
Table VIII: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); theory, dipole length.
chan_1992/aymar_1970_velocity_Xe#
{
"id": "aymar_1970_velocity_Xe",
"material": "Xe",
"file": "Xe/chan_1992__aymar_1970_velocity_Xe.csv",
"table": "tbl_ae92208a90e7",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"M. Aymar, S. Feneuille, and M. Klapisch, Nucl. Instrum. Methods 90, 137 (1970)"
]
}
Table VIII: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); theory, dipole velocity.
chan_1992/aymar_coulombe_1978_length_Xe#
{
"id": "aymar_coulombe_1978_length_Xe",
"material": "Xe",
"file": "Xe/chan_1992__aymar_coulombe_1978_length_Xe.csv",
"table": "tbl_ae92208a90e7",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"M. Aymar and M. Coulombe, At. Data Nucl. Data Tables 21, 537 (1978)"
]
}
Table VIII: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); theory, dipole length.
chan_1992/aymar_coulombe_1978_velocity_Xe#
{
"id": "aymar_coulombe_1978_velocity_Xe",
"material": "Xe",
"file": "Xe/chan_1992__aymar_coulombe_1978_velocity_Xe.csv",
"table": "tbl_ae92208a90e7",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"M. Aymar and M. Coulombe, At. Data Nucl. Data Tables 21, 537 (1978)"
]
}
Table VIII: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); theory, dipole velocity.
chan_1992/delage_1976_Xe#
{
"id": "delage_1976_Xe",
"material": "Xe",
"file": "Xe/chan_1992__delage_1976_Xe.csv",
"table": "tbl_ae92208a90e7, tbl_1dbc4809ef5a",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"A. Delage and J. D. Carette, Phys. Rev. A 14, 1345 (1976)"
],
"excluded_rows": {
"10.401": "Note c: normalized to the experimental value of Geiger [82], not an independent measurement.",
"11.583": "A repeat: the authors' erratum (Phys. Rev. A 48, 858 (1993), Table IX(b)) prints 0.251 once for the 9s (11.583 eV) and 5d' (11.607 eV) blend; kept at 11.607 eV (TC-710).",
"11.683": "A repeat: the authors' erratum (Table IX(b)) prints 0.171 once for the 8d (11.683), 8d-underlined (11.740) and 10s (11.752 eV) blend; kept at 11.740 eV (TC-710).",
"11.752": "A repeat of the 0.171 blend (see 11.683); kept at 11.740 eV (TC-710)."
}
}
Table VIII and Table IX: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); electron impact. Normalised on the 5d line of Geiger [82] (p. 168); the 10.401 eV value carries note c, ‘normalized to the experimental value of Geiger’, and is excluded. The (b) sub-table prints 0.251 under both 9s and 5d’ and 0.171 under 8d, 8d(underlined) and 10s (image checked). The authors’ erratum (chan_1993_erratum, Table IX(b)) prints each once under a brace: blends. Kept at the group’s strongest line in the present work (5d’, 11.607 eV; 8d(underlined), 11.740 eV); the repeats are excluded (TC-710).
chan_1992/dow_knox_1966_semiempirical_Xe#
{
"id": "dow_knox_1966_semiempirical_Xe",
"material": "Xe",
"file": "Xe/chan_1992__dow_knox_1966_semiempirical_Xe.csv",
"table": "tbl_ae92208a90e7",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"J. D. Dow and R. S. Knox, Phys. Rev. 152, 50 (1966)"
]
}
Table VIII: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); theory, semiempirical.
chan_1992/dow_knox_1966_wave_function_Xe#
{
"id": "dow_knox_1966_wave_function_Xe",
"material": "Xe",
"file": "Xe/chan_1992__dow_knox_1966_wave_function_Xe.csv",
"table": "tbl_ae92208a90e7",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"J. D. Dow and R. S. Knox, Phys. Rev. 152, 50 (1966)"
]
}
Table VIII: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); theory, wave function.
chan_1992/ferrell_1987_Xe#
{
"id": "ferrell_1987_Xe",
"material": "Xe",
"file": "Xe/chan_1992__ferrell_1987_Xe.csv",
"table": "tbl_ae92208a90e7, tbl_1dbc4809ef5a",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"ferrell_1987"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table VIII and Table IX: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); phase matching.
chan_1992/geiger_1970_Xe#
{
"id": "geiger_1970_Xe",
"material": "Xe",
"file": "Xe/chan_1992__geiger_1970_Xe.csv",
"table": "tbl_ae92208a90e7",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"J. Geiger, Phys. Lett. 33A, 351 (1970)"
]
}
Table VIII: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); electron impact.
chan_1992/geiger_1977_Xe#
{
"id": "geiger_1977_Xe",
"material": "Xe",
"file": "Xe/chan_1992__geiger_1977_Xe.csv",
"table": "tbl_ae92208a90e7, tbl_1dbc4809ef5a",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"J. Geiger, Z. Phys. A 282, 129 (1977)"
]
}
Table VIII and Table IX: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); electron impact.
chan_1992/geiger_1977_theory_Xe#
{
"id": "geiger_1977_theory_Xe",
"material": "Xe",
"file": "Xe/chan_1992__geiger_1977_theory_Xe.csv",
"table": "tbl_ae92208a90e7, tbl_1dbc4809ef5a",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"J. Geiger, Z. Phys. A 282, 129 (1977)"
]
}
Table VIII and Table IX: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); semiempirical calculation (listed under Theory).
chan_1992/geiger_1977_total_Xe#
{
"id": "geiger_1977_total_Xe",
"material": "Xe",
"file": "Xe/chan_1992__geiger_1977_total_Xe.csv",
"table": "tbl_1dbc4809ef5a",
"quantity": "oscillator_strength",
"abscissa": "label",
"use": "reproduced",
"reproduced_from": [
"J. Geiger, Z. Phys. A 282, 129 (1977)"
]
}
Table IX: ‘Total to ionization’: the discrete oscillator-strength sum up to the 2P_3/2 threshold, index abscissa; electron impact. Note d: ‘This value is quoted in Ref. [88]’ (Berkowitz 1979).
chan_1992/griffin_1969_Xe#
{
"id": "griffin_1969_Xe",
"material": "Xe",
"file": "Xe/chan_1992__griffin_1969_Xe.csv",
"table": "tbl_ae92208a90e7",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"P. M. Griffin and J. W. Hutchson, J. Opt. Soc. Am. 59, 1607 (1969)"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table VIII: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); total absorption.
chan_1992/gruzdev_1967_Xe#
{
"id": "gruzdev_1967_Xe",
"material": "Xe",
"file": "Xe/chan_1992__gruzdev_1967_Xe.csv",
"table": "tbl_ae92208a90e7",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"P. F. Gruzdev, Opt. Spectrosc. 22, 170 (1967)"
]
}
Table VIII: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); theory.
chan_1992/kim_1968_Xe#
{
"id": "kim_1968_Xe",
"material": "Xe",
"file": "Xe/chan_1992__kim_1968_Xe.csv",
"table": "tbl_ae92208a90e7",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"Y. K. Kim, M. Inokuti, G. E. Chamberlain, and S. R. Mielczarek, Phys. Rev. Lett. 21, 1146 (1968)"
]
}
Table VIII: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); theory.
chan_1992/kramer_1984_Xe#
{
"id": "kramer_1984_Xe",
"material": "Xe",
"file": "Xe/chan_1992__kramer_1984_Xe.csv",
"table": "tbl_1dbc4809ef5a",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"S. D. Kramer, C. H. Chen, and M. G. Payne, Opt. Lett. 9, 347 (1984)"
]
}
Table IX: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); phase matching.
chan_1992/lewis_1967_Xe#
{
"id": "lewis_1967_Xe",
"material": "Xe",
"file": "Xe/chan_1992__lewis_1967_Xe.csv",
"table": "tbl_ae92208a90e7",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"E. L. Lewis, Proc. Phys. Soc. 92, 817 (1967)"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table VIII: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); pressure-broadening profile. DOUBT: the printed values 0.256(0.008), 0.238(0.015) are identical to Anderson’s [61] row below, but the printed ratio is 1.071 (Anderson 1.076, which those values give); Lewis’s own values may have been replaced by Anderson’s in the table. Kept as printed.
chan_1992/matthias_1977_Xe#
{
"id": "matthias_1977_Xe",
"material": "Xe",
"file": "Xe/chan_1992__matthias_1977_Xe.csv",
"table": "tbl_ae92208a90e7",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"E. Matthias, R. A. Rosenberg, E. D. Poliakoff, M. G. White, S. T. Lee, and D. A. Shirley, Chem. Phys. Lett. 52, 239 (1977)"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table VIII: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); lifetime, resonance fluorescence.
chan_1992/natali_unpublished_Xe#
{
"id": "natali_unpublished_Xe",
"material": "Xe",
"file": "Xe/chan_1992__natali_unpublished_Xe.csv",
"table": "tbl_ae92208a90e7, tbl_1dbc4809ef5a",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"S. Natali, C. E. Kuyatt, and S. R. Miekzarek, unpublished, as quoted in Chan et al.'s Refs. [53,83,88]"
]
}
Table VIII and Table IX: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); electron impact (Ref. [87]). Table IX(b) labels this row ‘Natali, Kuyatt, and Garrett [87]’ (sic).
chan_1992/suzuki_1991_Xe#
{
"id": "suzuki_1991_Xe",
"material": "Xe",
"file": "Xe/chan_1992__suzuki_1991_Xe.csv",
"table": "tbl_ae92208a90e7",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"T. Y. Suzuki, Y. Sakai, B. S. Min, T. Takayanagi, K. Wakiya, H. Suzuki, T. Inaba, and H. Takuma, Phys. Rev. A 43, 5867 (1991)"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table VIII: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); electron impact.
chan_1992/wieme_1973_Xe#
{
"id": "wieme_1973_Xe",
"material": "Xe",
"file": "Xe/chan_1992__wieme_1973_Xe.csv",
"table": "tbl_ae92208a90e7",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"W. Wieme and P. Mortier, Physica 65, 198 (1973)"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table VIII: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); lifetime, resonance imprisonment.
chan_1992/wilkinson_1966_Xe#
{
"id": "wilkinson_1966_Xe",
"material": "Xe",
"file": "Xe/chan_1992__wilkinson_1966_Xe.csv",
"table": "tbl_ae92208a90e7",
"quantity": "oscillator_strength",
"abscissa_unit": "eV",
"use": "reproduced",
"reproduced_from": [
"P. G. Wilkinson, J. Quant. Spectrosc. Radiat. Transfer 6, 823 (1966)"
],
"uncertainty": {
"column": true,
"level": "not stated"
}
}
Table VIII: oscillator strengths of the discrete lines, rows by transition energy (eV, from Moore’s tables, Ref. [95]); total absorption.
Formulas#
No formulas are recorded.
Corrections#
[
{
"dataset": "continuum_Ar",
"row": "333",
"column": "x",
"printed": "208.0",
"corrected": "308.0",
"reason": "The energy column of the second column pair of Table I (continued) runs 270.0 ... 307.0, '208.0', 309.0 ... 315.0 in 1 eV steps; 208.0 breaks the sequence and duplicates the 208.0 eV row of the first page (df/dE 0.514 there, 2.64 here, between 2.67 at 307 and 2.62 at 309 eV).",
"evidence": "Table image tbl_41f17cecf0c6.jpg prints 208.0 between 307.0 and 309.0 (checked 2026-09-24)."
},
{
"dataset": "present_total_Ar",
"row": "total",
"column": "sigma",
"printed": "0.0043",
"corrected": "0.043",
"reason": "The uncertainty of the argon total discrete oscillator strength 0.859 is printed (0.0043), 0.5 %; the krypton and xenon totals carry exactly 5 % (1.126(0.056), 1.606(0.080)), as do the resonance lines, and 5 % of 0.859 is 0.043. A dropped digit.",
"evidence": "Table image tbl_699514709b3b.jpg prints 0.859 (0.0043); Tables VII and IX print 1.126 (0.056) and 1.606 (0.080). Checked 2026-09-24. Confirmed by the authors' erratum, Phys. Rev. A 48, 858 (1993) (chan_1993_erratum), whose reprinted Table V(b) (tbl_73d8dcfe47d0, p. 858, image checked 2026-09-29) prints 0.859 (0.043)."
},
{
"dataset": "wiese_1969_Ar",
"row": "14.304",
"column": "value",
"printed": "0.0106",
"corrected": "0.106",
"reason": "Wiese, Smith and Miles's value for the 3d' line (14.304 eV) is 'obtained by reanalyzing the lifetime data of Lawrence' (note c), and Lawrence's value is 0.107(0.015); the present work gives 0.106 and Natali et al. 0.110. The printed 0.0106 is ten times smaller, a misplaced zero (Wiese et al.'s other three values agree with Lawrence's to 10 %).",
"evidence": "Table image tbl_699514709b3b.jpg prints 0.0106 in the Wiese, Smith, and Miles row under (2P1/2)3d' (14.304 eV), beside Lawrence's 0.107. The original compilation is not in the library. Checked 2026-09-24. The authors' erratum (chan_1993_erratum, Table V(a), p. 858) reprints 0.0106 unchanged, so this correction rests on the table's own evidence (checked 2026-09-29)."
},
{
"dataset": "present_Ar",
"row": "15.190",
"column": "sigma",
"printed": "0.0043",
"corrected": "0.0063",
"reason": "The authors' erratum: Table V(b)'s 0.0426 is one value for the unresolved 7s (15.186 eV) and 5d-underlined (15.190 eV) pair, printed in 1992 under both lines with (0.0043) each; the reprint prints it once, under a brace spanning the pair, with uncertainty 0.0063 (15 %, printed without parentheses). The repeat at 15.186 eV is an excluded row (TC-710).",
"evidence": "Erratum, Phys. Rev. A 48, 858 (1993) (chan_1993_erratum), reprinted Table V(b), p. 858 (library table tbl_73d8dcfe47d0, image checked 2026-09-29): '0.0426' over '0.0063', centred under the brace spanning the 7s and 5d-underlined columns. The 1992 table image tbl_699514709b3b.jpg prints 0.0426 (0.0043) in both columns."
}
]
Formula corrections, where recorded, appear with their formulas above. Curation notes may also discuss corrections or unresolved interpretation. Consult the review register for the checks and decisions.