petrov_2011 =========== I\. D\. Petrov, V\. L\. Sukhorukov, M\.\-W\. Ruf, D\. Klar and H\. Hotop, "Near\-threshold photoionization from the excited mp5\(m \+ 1\)p J = 0\-3 levels of Ar, Kr and Xe \(m = 3\-5\)", Eur\. Phys\. J\. D 62, 347\-359 \(2011\) `Source record `__ · :doc:`Catalogue ` · :doc:`Review register ` DOI: `10\.1140/epjd/e2011\-10667\-5 `__ **Source kind:** theory **Recorded technique:** Calculated one\-photon photoionisation cross sections of the ten levels mp5 \(m\+1\)p, J = 0\-3 \(Paschen 2p1\-2p10\) of Ar, Kr and Xe, total and partial \(into the 2P3/2 and 2P1/2 ion\), near threshold, including the autoionising mp5\(2P1/2\) ns', nd', ng' resonances between the two thresholds, in the configuration interaction Pauli\-Fock approach with core polarisation \(CIPFCP\)\: Pauli\-Fock orbitals with the relativistic compression of the core, initial\- and final\-state configuration interaction \(scheme \(2\)\: intershell 4p4 n/epsilon l, 4s 4p6 epsilon l, 4p5 p/f, and the coupling of the channels and resonances\) in second\-order perturbation theory, the Slater integrals scaled by the factors of Table 1\. Length and velocity gauges agree \(Fig\. 2\); the length gauge is shown\. Selected autoionisation spectra \(Ar, Kr\) are compared with atomic\-beam measurements \(cw two\-step laser excitation of metastables, ion detection\), convolved with the experiment's 0\.4\-1 cm\-1 resolution\. **Materials in structured entries:** Ar, Kr, Xe **Dataset quantities:** excited\_state\_photoionization\_cross\_section **Contents:** 120 datasets; 0 formulas. Curation notes -------------- Eur\. Phys\. J\. D 62\(3\), 347\-359 \(2011\) = PDF pages 1\-13 \(journal page = PDF page \+ 346\)\. Identity checked on the first page \(PDF p\. 1\: journal, volume, pages, DOI, title, authors, Rostov\-on\-Don and Kaiserslautern, received 22 November 2010, final form 4 February 2011, published online 17 May 2011\) on 2026\-10\-12\. Table 2 checked cell by cell against the table image; Figs\. 3\-5 read from the vector drawing and inspected as overlays \(below\)\. LEVELS\. The paper names each level by its Paschen label and its jK label \(pair\-coupling nl\[K\]J, a prime for the 2P1/2 core\); NIST's configuration, term and J follow from the jK label directly \(src/optmat/data/external/nist\_asd/\\_I\_levels\.tsv\), and each dataset's initial\_level gives both\. The figures' panels carry each gas's own Paschen label\: Kr 2p2 = 5p'\[3/2\]2 and 2p3 = 5p'\[1/2\]1, Xe 2p8 = 6p\[5/2\]3 and 2p9 = 6p\[5/2\]2, the reverse of Ar \(Table 2's footnote e\), as NIST's energies order them \(Kr 5p'\[3/2\]2 97945\.17 above 5p'\[1/2\]1 97919\.15 cm\-1; Xe 6p\[5/2\]3 78403\.06 above 6p\[5/2\]2 78119\.80\)\. Table 2's rows carry Ar's Paschen labels with one jK column, and its values for Kr and Xe belong to the jK label\: the curves at threshold match Table 2 by jK within 0\.06 Mb \(Kr \[3/2\]2' 15\.82 against 15\.81 and \[1/2\]1' 16\.13 against 16\.09; by the Paschen label they would miss by 0\.27 and 0\.32 Mb; Xe \[5/2\]3 6\.78 against 6\.77, \[5/2\]2 7\.58 against 7\.58, by Paschen 0\.8 Mb\), so the datasets are named by jK \(pp12\_0 = p'\[1/2\]0, p52\_3 = p\[5/2\]3 and so on\) and their rows keep Table 2's printed Paschen label\. ENERGY AXIS \(a decision of this record\)\. Figs\. 3\-5 and Table 2 give the cross sections against the 'relative \(photon\) energy' omega\_1/2 above the level's mp5 2P1/2 ionisation threshold \(pp\. 350\-351\), 0 to 6 eV; at omega\_1/2 = 0 the photoelectron of the 2P3/2 channel has Delta\_FS, that of the 2P1/2 channel none\. The quantity is held against the photon energy, so the scripts add the level's 2P1/2 threshold, E\(2P3/2 limit\) \+ Delta\_FS \- E\(level\), from NIST's levels \(the paper's energies are experimental, Fig\. 1's caption, ref\. 55\)\: Ar 2\.4572 \(4p'\[1/2\]0\) to 3\.0301 eV \(4p\[1/2\]1\), Kr 2\.4089 to 3\.3620, Xe 2\.2950 to 3\.8561 \(each dataset's notes\)\. Delta\_FS \(NIST, Ar\_II, Kr\_II, Xe\_II\_levels\.tsv\) is 0\.17749, 0\.66581 and 1\.30642 eV; the paper prints 0\.178, 0\.666 and 1\.306 \(p\. 349\) and 177\.5 meV for Ar \(p\. 353\) \(script check\)\. Nothing is shifted beyond this conversion; the printed omega\_1/2 of each vertex is kept in printed\. RANGE AGAINST OEP 8's DRIVES\. 0\-6 eV above the 2P1/2 threshold covers every drive\: Ar 4p'\[1/2\]0 at 184\.0 nm \(6\.738 eV\) is omega\_1/2 = 4\.28 eV, 4p\[1/2\]0 at 186\.8 nm 3\.97 eV, 4p\[3/2\]2 at 188\.3 nm 3\.82 eV, 4p\[5/2\]2 at 189\.4 nm 3\.70 eV \(the third photon of the two\-photon drive; photoelectron about 3\.9\-4\.1 eV above the 2P3/2 threshold\); Xe 6p\[1/2\]0 at 248 nm \(5\.0 eV\) 1\.50 eV; Kr 5p\[1/2\]0 at 212\.6 nm \(5\.83 eV\) 2\.83 eV\. Read off the curves \(linear interpolation of the vertices\)\: Ar 2p1 2\.39 Mb at 184\.0 nm, 2p5 2\.03 at 186\.8 nm, 2p6 2\.31 at 188\.3 nm, 2p8 2\.55 at 189\.4 nm; Xe 6p\[1/2\]0 3\.35 Mb at 248 nm and 1\.47 at 193 nm, 6p\[3/2\]2 2\.70 and 1\.21; Kr 5p\[1/2\]0 3\.03 Mb at 212\.6 nm\. These are bound\-free continuum values\: the autoionising resonances lie between the 2P3/2 and 2P1/2 thresholds \(omega\_1/2 \< 0\), below every drive\. WHAT IS TAKEN \(tools/extract/petrov\_2011\.py\)\. Per gas and level \(30 levels, 120 datasets\)\: \(1\) Table 2 \(p\. 352\), sigma\_tot^0 \(tot\_\*\), sigma\_3/2^0 \(s32\_\*\) and sigma\_1/2^Delta\_FS \(s12\_\*\), one point each, channel total, '2P3/2 ion', '2P1/2 ion', use primary \(the paper's own calculation; no uncertainty stated\)\. No unit is printed in Table 2; it is Mb, the figures' unit, with which the totals agree\. The ratio column r\(Delta\_FS\) = sigma\_1/2^DFS / sigma\_3/2^0 is derived \(checked by the script for all 30 rows to the rounding\) and not taken\. \(2\) Figs\. 3\-5 \(p\. 351\), the total sigma\_tot against the photon energy, every vertex of the drawn line inside the frame \(42\-61 per level, omega\_1/2 from 0 or 0\.02\-0\.05 eV, where the drawn lines start, to 5\.5\-6\.0 eV, where the frame clips them\), fig\_\*, digitised vector, use check \(data rule 8\)\. The drawn lines begin at omega\_1/2 = \-0\.02 to 0\.05 eV and there equal Table 2's sigma\_tot^0 within 0\.06 Mb for all 30 levels \(script check\); the ticks lie on their scales within 0\.05 pt\. Uncertainty 0\.1 Mb absolute, not stated by the paper\: the drawing's reproduction of the printed threshold values \(0\.06 Mb\) with margin; the line is 0\.85 pt wide, 0\.23\-0\.34 Mb on the three y scales \(Ar 14\.5 pt per 4 Mb, Kr 12\.1, Xe 9\.9\)\. Overlays inspected\: the extracted vertices drawn back on the rendered page lie on the black lines of all 30 panels \(overlays made at curation, not archived\)\. NOT TAKEN\. The partial curves sigma\_3/2 \(blue\) and sigma\_1/2 \(dashed red\) of Figs\. 3\-5\: Table 2 prints their threshold values, the total is drawn and read, and several partial curves are drawn x10 \(marked by arrows\) and dashed\. Figs\. 2 and 6\-8 \(lineshapes of the autoionising resonances between the thresholds, against binding energy\) and Figs\. 9\-12 \(comparisons with experiment, relative units\)\: resonance structure below the 2P1/2 threshold, not near OEP 8's drives; nothing in them is printed as a number\. Table 1 \(scaling factors of the Slater integrals\)\: method parameters\. The text's reduced widths of the nd'\[5/2\]3 series \(81, 9501, 5955, 3796 cm\-1 for Ne, Ar, Kr, Xe, p\. 353\) and r\(J = 3\) of Ne\: no quantity\. FINDINGS \(comparison with the held excited\-state cross sections; Petrov read at the photon energy of each\)\. Ar 4p at 248 nm\: the \(2J\+1\)\-weighted mean of the ten levels 4\.72 Mb, 2p5 \(4p\[1/2\]0\) 4\.31, 2p1 4\.18; duzy\_1980 \(configuration average\) 5\.4, chang\_1982 \(4p 1S, J = 0\) 4\.8, hyman\_1977 \(J\-averaged, 248\.6 nm\) 4\.3 Mb\. payne\_1981's Ar 4p\[1/2\]0 '~1 x 10^\-18 cm2' at 157\.6 nm\: Petrov 1\.18 Mb\. Kr 5p at 248 nm\: mean 4\.51 Mb; duzy\_1980 5\.2, chang\_1982 4\.5\. payne\_1981's Kr 5p\[1/2\]0 '10^\-18 cm2' at 326\.2 nm\: Petrov 7\.02 Mb, seven times larger\. Xe 6p at 308 nm\: mean 5\.81 Mb; duzy\_1980 7\.6, chang\_1982 6\.9\. Xe 6p\[1/2\]0 \(2p5\)\: kroll\_1990 \(measured\) 4\.3 \+\- 0\.7 Mb at 248 nm and 1\.9 \+\- 0\.7 at 193 nm against Petrov 3\.35 and 1\.47 \(both within 1\.4 sigma, low\); pindzola\_1981 Dirac\-Fock length 3\.05 at 4\.97 eV and 1\.85 at 6\.20 eV against 3\.40 and 1\.71, Hartree\-Fock velocity 1\.32 at 4\.97 eV; payne\_1981's '3 x 10^\-18' at 249\.6 nm against 3\.41\. Xe 6p\[3/2\]2 \(2p6\)\: kroll\_1990 3\.7 \+\- 0\.7 and 1\.8 \+\- 0\.5 Mb against 2\.70 and 1\.21 \(1\.4 and 1\.2 sigma low\)\. The single\-electron calculations \(duzy\_1980, chang\_1982\) lie 0\-31 % above Petrov's level means; Petrov says its totals agree with them 'in general behaviour' \(p\. 352\)\. TWO\-PHOTON DATA CITED, NOT IN THE LIBRARY\: M\. Stellpflug, M\. Johnsson, I\. D\. Petrov, T\. Halfmann, Eur\. Phys\. J\. D 23, 35 \(2003\) \(ref\. 56\: Xe 2p1 and 2p5 two\-photon excited from the ground state, autoionisation spectra above them and the 5p6 admixture of the J = 0 levels\)\. The single\-electron calculations it compares with, Duzy and Hyman \(ref\. 65\) and Chang and Kim \(ref\. 66\), are duzy\_1980 and chang\_1982\. **Recorded bibliographic identity status:** VALIDATED. This concerns identification of the source; it does not establish the scientific correctness of its contents. Datasets -------- petrov\_2011/fig\_Ar\_pp12\_0 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Ar_pp12_0", "material": "Ar", "file": "Ar/petrov_2011__fig_Ar_pp12_0.csv", "table": "fig_cdcdef4cd679", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Ar 4p'[1/2]0 = 3s2.3p5.(2P*<1/2>).4p 2[1/2] J = 0 (NIST, 108722.619 cm-1); Paschen 2p1 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 3 \(p\. 351\), panel 2p1 4p'\[1/2\]0\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 2\.4572 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Ar\_pp12\_0 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Ar_pp12_0", "material": "Ar", "file": "Ar/petrov_2011__tot_Ar_pp12_0.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p'[1/2]0 = 3s2.3p5.(2P*<1/2>).4p 2[1/2] J = 0 (NIST, 108722.619 cm-1); Paschen 2p1 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p1 \[1/2\]0' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 2\.4572 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Ar\_pp12\_0 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Ar_pp12_0", "material": "Ar", "file": "Ar/petrov_2011__s32_Ar_pp12_0.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p'[1/2]0 = 3s2.3p5.(2P*<1/2>).4p 2[1/2] J = 0 (NIST, 108722.619 cm-1); Paschen 2p1 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p1 \[1/2\]0' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 2\.4572 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Ar\_pp12\_0 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Ar_pp12_0", "material": "Ar", "file": "Ar/petrov_2011__s12_Ar_pp12_0.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p'[1/2]0 = 3s2.3p5.(2P*<1/2>).4p 2[1/2] J = 0 (NIST, 108722.619 cm-1); Paschen 2p1 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p1 \[1/2\]0' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 2\.6347 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Ar\_pp12\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Ar_pp12_1", "material": "Ar", "file": "Ar/petrov_2011__fig_Ar_pp12_1.csv", "table": "fig_cdcdef4cd679", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Ar 4p'[1/2]1 = 3s2.3p5.(2P*<1/2>).4p 2[1/2] J = 1 (NIST, 107496.417 cm-1); Paschen 2p2 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 3 \(p\. 351\), panel 2p2 4p'\[1/2\]1\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 2\.6092 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Ar\_pp12\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Ar_pp12_1", "material": "Ar", "file": "Ar/petrov_2011__tot_Ar_pp12_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p'[1/2]1 = 3s2.3p5.(2P*<1/2>).4p 2[1/2] J = 1 (NIST, 107496.417 cm-1); Paschen 2p2 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p2 \[1/2\]1' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 2\.6092 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Ar\_pp12\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Ar_pp12_1", "material": "Ar", "file": "Ar/petrov_2011__s32_Ar_pp12_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p'[1/2]1 = 3s2.3p5.(2P*<1/2>).4p 2[1/2] J = 1 (NIST, 107496.417 cm-1); Paschen 2p2 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p2 \[1/2\]1' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 2\.6092 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Ar\_pp12\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Ar_pp12_1", "material": "Ar", "file": "Ar/petrov_2011__s12_Ar_pp12_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p'[1/2]1 = 3s2.3p5.(2P*<1/2>).4p 2[1/2] J = 1 (NIST, 107496.417 cm-1); Paschen 2p2 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p2 \[1/2\]1' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 2\.7867 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Ar\_pp32\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Ar_pp32_2", "material": "Ar", "file": "Ar/petrov_2011__fig_Ar_pp32_2.csv", "table": "fig_cdcdef4cd679", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Ar 4p'[3/2]2 = 3s2.3p5.(2P*<1/2>).4p 2[3/2] J = 2 (NIST, 107289.700 cm-1); Paschen 2p3 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 3 \(p\. 351\), panel 2p3 4p'\[3/2\]2\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 2\.6349 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Ar\_pp32\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Ar_pp32_2", "material": "Ar", "file": "Ar/petrov_2011__tot_Ar_pp32_2.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p'[3/2]2 = 3s2.3p5.(2P*<1/2>).4p 2[3/2] J = 2 (NIST, 107289.700 cm-1); Paschen 2p3 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p3 \[3/2\]2' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 2\.6349 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Ar\_pp32\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Ar_pp32_2", "material": "Ar", "file": "Ar/petrov_2011__s32_Ar_pp32_2.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p'[3/2]2 = 3s2.3p5.(2P*<1/2>).4p 2[3/2] J = 2 (NIST, 107289.700 cm-1); Paschen 2p3 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p3 \[3/2\]2' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 2\.6349 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Ar\_pp32\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Ar_pp32_2", "material": "Ar", "file": "Ar/petrov_2011__s12_Ar_pp32_2.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p'[3/2]2 = 3s2.3p5.(2P*<1/2>).4p 2[3/2] J = 2 (NIST, 107289.700 cm-1); Paschen 2p3 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p3 \[3/2\]2' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 2\.8124 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Ar\_pp32\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Ar_pp32_1", "material": "Ar", "file": "Ar/petrov_2011__fig_Ar_pp32_1.csv", "table": "fig_cdcdef4cd679", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Ar 4p'[3/2]1 = 3s2.3p5.(2P*<1/2>).4p 2[3/2] J = 1 (NIST, 107131.709 cm-1); Paschen 2p4 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 3 \(p\. 351\), panel 2p4 4p'\[3/2\]1\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 2\.6545 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Ar\_pp32\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Ar_pp32_1", "material": "Ar", "file": "Ar/petrov_2011__tot_Ar_pp32_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p'[3/2]1 = 3s2.3p5.(2P*<1/2>).4p 2[3/2] J = 1 (NIST, 107131.709 cm-1); Paschen 2p4 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p4 \[3/2\]1' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 2\.6545 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Ar\_pp32\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Ar_pp32_1", "material": "Ar", "file": "Ar/petrov_2011__s32_Ar_pp32_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p'[3/2]1 = 3s2.3p5.(2P*<1/2>).4p 2[3/2] J = 1 (NIST, 107131.709 cm-1); Paschen 2p4 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p4 \[3/2\]1' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 2\.6545 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Ar\_pp32\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Ar_pp32_1", "material": "Ar", "file": "Ar/petrov_2011__s12_Ar_pp32_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p'[3/2]1 = 3s2.3p5.(2P*<1/2>).4p 2[3/2] J = 1 (NIST, 107131.709 cm-1); Paschen 2p4 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p4 \[3/2\]1' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 2\.8320 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Ar\_p12\_0 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Ar_p12_0", "material": "Ar", "file": "Ar/petrov_2011__fig_Ar_p12_0.csv", "table": "fig_cdcdef4cd679", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Ar 4p[1/2]0 = 3s2.3p5.(2P*<3/2>).4p 2[1/2] J = 0 (NIST, 107054.272 cm-1); Paschen 2p5 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 3 \(p\. 351\), panel 2p5 4p\[1/2\]0\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 2\.6641 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Ar\_p12\_0 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Ar_p12_0", "material": "Ar", "file": "Ar/petrov_2011__tot_Ar_p12_0.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p[1/2]0 = 3s2.3p5.(2P*<3/2>).4p 2[1/2] J = 0 (NIST, 107054.272 cm-1); Paschen 2p5 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p5 \[1/2\]0 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 2\.6641 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Ar\_p12\_0 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Ar_p12_0", "material": "Ar", "file": "Ar/petrov_2011__s32_Ar_p12_0.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p[1/2]0 = 3s2.3p5.(2P*<3/2>).4p 2[1/2] J = 0 (NIST, 107054.272 cm-1); Paschen 2p5 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p5 \[1/2\]0 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 2\.6641 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Ar\_p12\_0 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Ar_p12_0", "material": "Ar", "file": "Ar/petrov_2011__s12_Ar_p12_0.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p[1/2]0 = 3s2.3p5.(2P*<3/2>).4p 2[1/2] J = 0 (NIST, 107054.272 cm-1); Paschen 2p5 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p5 \[1/2\]0 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 2\.8416 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Ar\_p32\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Ar_p32_2", "material": "Ar", "file": "Ar/petrov_2011__fig_Ar_p32_2.csv", "table": "fig_cdcdef4cd679", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Ar 4p[3/2]2 = 3s2.3p5.(2P*<3/2>).4p 2[3/2] J = 2 (NIST, 106237.552 cm-1); Paschen 2p6 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 3 \(p\. 351\), panel 2p6 4p\[3/2\]2\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 2\.7653 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Ar\_p32\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Ar_p32_2", "material": "Ar", "file": "Ar/petrov_2011__tot_Ar_p32_2.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p[3/2]2 = 3s2.3p5.(2P*<3/2>).4p 2[3/2] J = 2 (NIST, 106237.552 cm-1); Paschen 2p6 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p6 \[3/2\]2 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 2\.7653 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Ar\_p32\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Ar_p32_2", "material": "Ar", "file": "Ar/petrov_2011__s32_Ar_p32_2.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p[3/2]2 = 3s2.3p5.(2P*<3/2>).4p 2[3/2] J = 2 (NIST, 106237.552 cm-1); Paschen 2p6 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p6 \[3/2\]2 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 2\.7653 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Ar\_p32\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Ar_p32_2", "material": "Ar", "file": "Ar/petrov_2011__s12_Ar_p32_2.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p[3/2]2 = 3s2.3p5.(2P*<3/2>).4p 2[3/2] J = 2 (NIST, 106237.552 cm-1); Paschen 2p6 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p6 \[3/2\]2 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 2\.9428 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Ar\_p32\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Ar_p32_1", "material": "Ar", "file": "Ar/petrov_2011__fig_Ar_p32_1.csv", "table": "fig_cdcdef4cd679", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Ar 4p[3/2]1 = 3s2.3p5.(2P*<3/2>).4p 2[3/2] J = 1 (NIST, 106087.260 cm-1); Paschen 2p7 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 3 \(p\. 351\), panel 2p7 4p\[3/2\]1\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 2\.7840 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Ar\_p32\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Ar_p32_1", "material": "Ar", "file": "Ar/petrov_2011__tot_Ar_p32_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p[3/2]1 = 3s2.3p5.(2P*<3/2>).4p 2[3/2] J = 1 (NIST, 106087.260 cm-1); Paschen 2p7 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p7 \[3/2\]1 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 2\.7840 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Ar\_p32\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Ar_p32_1", "material": "Ar", "file": "Ar/petrov_2011__s32_Ar_p32_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p[3/2]1 = 3s2.3p5.(2P*<3/2>).4p 2[3/2] J = 1 (NIST, 106087.260 cm-1); Paschen 2p7 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p7 \[3/2\]1 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 2\.7840 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Ar\_p32\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Ar_p32_1", "material": "Ar", "file": "Ar/petrov_2011__s12_Ar_p32_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p[3/2]1 = 3s2.3p5.(2P*<3/2>).4p 2[3/2] J = 1 (NIST, 106087.260 cm-1); Paschen 2p7 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p7 \[3/2\]1 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 2\.9615 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Ar\_p52\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Ar_p52_2", "material": "Ar", "file": "Ar/petrov_2011__fig_Ar_p52_2.csv", "table": "fig_cdcdef4cd679", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Ar 4p[5/2]2 = 3s2.3p5.(2P*<3/2>).4p 2[5/2] J = 2 (NIST, 105617.270 cm-1); Paschen 2p8 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 3 \(p\. 351\), panel 2p8 4p\[5/2\]2\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 2\.8422 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Ar\_p52\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Ar_p52_2", "material": "Ar", "file": "Ar/petrov_2011__tot_Ar_p52_2.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p[5/2]2 = 3s2.3p5.(2P*<3/2>).4p 2[5/2] J = 2 (NIST, 105617.270 cm-1); Paschen 2p8 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p8 \[5/2\]2 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 2\.8422 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Ar\_p52\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Ar_p52_2", "material": "Ar", "file": "Ar/petrov_2011__s32_Ar_p52_2.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p[5/2]2 = 3s2.3p5.(2P*<3/2>).4p 2[5/2] J = 2 (NIST, 105617.270 cm-1); Paschen 2p8 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p8 \[5/2\]2 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 2\.8422 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Ar\_p52\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Ar_p52_2", "material": "Ar", "file": "Ar/petrov_2011__s12_Ar_p52_2.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p[5/2]2 = 3s2.3p5.(2P*<3/2>).4p 2[5/2] J = 2 (NIST, 105617.270 cm-1); Paschen 2p8 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p8 \[5/2\]2 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 3\.0197 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Ar\_p52\_3 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Ar_p52_3", "material": "Ar", "file": "Ar/petrov_2011__fig_Ar_p52_3.csv", "table": "fig_cdcdef4cd679", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Ar 4p[5/2]3 = 3s2.3p5.(2P*<3/2>).4p 2[5/2] J = 3 (NIST, 105462.760 cm-1); Paschen 2p9 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 3 \(p\. 351\), panel 2p9 4p\[5/2\]3\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 2\.8614 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Ar\_p52\_3 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Ar_p52_3", "material": "Ar", "file": "Ar/petrov_2011__tot_Ar_p52_3.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p[5/2]3 = 3s2.3p5.(2P*<3/2>).4p 2[5/2] J = 3 (NIST, 105462.760 cm-1); Paschen 2p9 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p9 \[5/2\]3 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 2\.8614 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Ar\_p52\_3 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Ar_p52_3", "material": "Ar", "file": "Ar/petrov_2011__s32_Ar_p52_3.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p[5/2]3 = 3s2.3p5.(2P*<3/2>).4p 2[5/2] J = 3 (NIST, 105462.760 cm-1); Paschen 2p9 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p9 \[5/2\]3 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 2\.8614 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Ar\_p52\_3 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Ar_p52_3", "material": "Ar", "file": "Ar/petrov_2011__s12_Ar_p52_3.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p[5/2]3 = 3s2.3p5.(2P*<3/2>).4p 2[5/2] J = 3 (NIST, 105462.760 cm-1); Paschen 2p9 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p9 \[5/2\]3 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 3\.0389 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Ar\_p12\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Ar_p12_1", "material": "Ar", "file": "Ar/petrov_2011__fig_Ar_p12_1.csv", "table": "fig_cdcdef4cd679", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Ar 4p[1/2]1 = 3s2.3p5.(2P*<3/2>).4p 2[1/2] J = 1 (NIST, 104102.099 cm-1); Paschen 2p10 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 3 \(p\. 351\), panel 2p10 4p\[1/2\]1\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 3\.0301 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Ar\_p12\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Ar_p12_1", "material": "Ar", "file": "Ar/petrov_2011__tot_Ar_p12_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p[1/2]1 = 3s2.3p5.(2P*<3/2>).4p 2[1/2] J = 1 (NIST, 104102.099 cm-1); Paschen 2p10 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p10 \[1/2\]1 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 3\.0301 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Ar\_p12\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Ar_p12_1", "material": "Ar", "file": "Ar/petrov_2011__s32_Ar_p12_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p[1/2]1 = 3s2.3p5.(2P*<3/2>).4p 2[1/2] J = 1 (NIST, 104102.099 cm-1); Paschen 2p10 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p10 \[1/2\]1 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 3\.0301 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Ar\_p12\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Ar_p12_1", "material": "Ar", "file": "Ar/petrov_2011__s12_Ar_p12_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Ar 4p[1/2]1 = 3s2.3p5.(2P*<3/2>).4p 2[1/2] J = 1 (NIST, 104102.099 cm-1); Paschen 2p10 of Ar", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p10 \[1/2\]1 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Ar\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 3\.2076 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Kr\_pp12\_0 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Kr_pp12_0", "material": "Kr", "file": "Kr/petrov_2011__fig_Kr_pp12_0.csv", "table": "fig_c5f6d8609180", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Kr 5p'[1/2]0 = 4s2.4p5.(2P*<1/2>).5p 2[1/2] J = 0 (NIST, 98855.070 cm-1); Paschen 2p1 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 4 \(p\. 351\), panel 2p1 5p'\[1/2\]0\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 2\.4089 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Kr\_pp12\_0 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Kr_pp12_0", "material": "Kr", "file": "Kr/petrov_2011__tot_Kr_pp12_0.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p'[1/2]0 = 4s2.4p5.(2P*<1/2>).5p 2[1/2] J = 0 (NIST, 98855.070 cm-1); Paschen 2p1 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p1 \[1/2\]0' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 2\.4089 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Kr\_pp12\_0 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Kr_pp12_0", "material": "Kr", "file": "Kr/petrov_2011__s32_Kr_pp12_0.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p'[1/2]0 = 4s2.4p5.(2P*<1/2>).5p 2[1/2] J = 0 (NIST, 98855.070 cm-1); Paschen 2p1 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p1 \[1/2\]0' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 2\.4089 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Kr\_pp12\_0 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Kr_pp12_0", "material": "Kr", "file": "Kr/petrov_2011__s12_Kr_pp12_0.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p'[1/2]0 = 4s2.4p5.(2P*<1/2>).5p 2[1/2] J = 0 (NIST, 98855.070 cm-1); Paschen 2p1 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p1 \[1/2\]0' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 3\.0748 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Kr\_pp32\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Kr_pp32_2", "material": "Kr", "file": "Kr/petrov_2011__fig_Kr_pp32_2.csv", "table": "fig_c5f6d8609180", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Kr 5p'[3/2]2 = 4s2.4p5.(2P*<1/2>).5p 2[3/2] J = 2 (NIST, 97945.166 cm-1); Paschen 2p2 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 4 \(p\. 351\), panel 2p2 5p'\[3/2\]2\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 2\.5218 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Kr\_pp32\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Kr_pp32_2", "material": "Kr", "file": "Kr/petrov_2011__tot_Kr_pp32_2.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p'[3/2]2 = 4s2.4p5.(2P*<1/2>).5p 2[3/2] J = 2 (NIST, 97945.166 cm-1); Paschen 2p2 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p3 \[3/2\]2' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 2\.5218 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Kr\_pp32\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Kr_pp32_2", "material": "Kr", "file": "Kr/petrov_2011__s32_Kr_pp32_2.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p'[3/2]2 = 4s2.4p5.(2P*<1/2>).5p 2[3/2] J = 2 (NIST, 97945.166 cm-1); Paschen 2p2 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p3 \[3/2\]2' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 2\.5218 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Kr\_pp32\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Kr_pp32_2", "material": "Kr", "file": "Kr/petrov_2011__s12_Kr_pp32_2.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p'[3/2]2 = 4s2.4p5.(2P*<1/2>).5p 2[3/2] J = 2 (NIST, 97945.166 cm-1); Paschen 2p2 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p3 \[3/2\]2' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 3\.1876 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Kr\_pp12\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Kr_pp12_1", "material": "Kr", "file": "Kr/petrov_2011__fig_Kr_pp12_1.csv", "table": "fig_c5f6d8609180", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Kr 5p'[1/2]1 = 4s2.4p5.(2P*<1/2>).5p 2[1/2] J = 1 (NIST, 97919.147 cm-1); Paschen 2p3 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 4 \(p\. 351\), panel 2p3 5p'\[1/2\]1\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 2\.5250 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Kr\_pp12\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Kr_pp12_1", "material": "Kr", "file": "Kr/petrov_2011__tot_Kr_pp12_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p'[1/2]1 = 4s2.4p5.(2P*<1/2>).5p 2[1/2] J = 1 (NIST, 97919.147 cm-1); Paschen 2p3 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p2 \[1/2\]1' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 2\.5250 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Kr\_pp12\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Kr_pp12_1", "material": "Kr", "file": "Kr/petrov_2011__s32_Kr_pp12_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p'[1/2]1 = 4s2.4p5.(2P*<1/2>).5p 2[1/2] J = 1 (NIST, 97919.147 cm-1); Paschen 2p3 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p2 \[1/2\]1' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 2\.5250 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Kr\_pp12\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Kr_pp12_1", "material": "Kr", "file": "Kr/petrov_2011__s12_Kr_pp12_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p'[1/2]1 = 4s2.4p5.(2P*<1/2>).5p 2[1/2] J = 1 (NIST, 97919.147 cm-1); Paschen 2p3 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p2 \[1/2\]1' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 3\.1908 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Kr\_pp32\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Kr_pp32_1", "material": "Kr", "file": "Kr/petrov_2011__fig_Kr_pp32_1.csv", "table": "fig_c5f6d8609180", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Kr 5p'[3/2]1 = 4s2.4p5.(2P*<1/2>).5p 2[3/2] J = 1 (NIST, 97595.915 cm-1); Paschen 2p4 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 4 \(p\. 351\), panel 2p4 5p'\[3/2\]1\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 2\.5651 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Kr\_pp32\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Kr_pp32_1", "material": "Kr", "file": "Kr/petrov_2011__tot_Kr_pp32_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p'[3/2]1 = 4s2.4p5.(2P*<1/2>).5p 2[3/2] J = 1 (NIST, 97595.915 cm-1); Paschen 2p4 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p4 \[3/2\]1' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 2\.5651 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Kr\_pp32\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Kr_pp32_1", "material": "Kr", "file": "Kr/petrov_2011__s32_Kr_pp32_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p'[3/2]1 = 4s2.4p5.(2P*<1/2>).5p 2[3/2] J = 1 (NIST, 97595.915 cm-1); Paschen 2p4 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p4 \[3/2\]1' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 2\.5651 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Kr\_pp32\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Kr_pp32_1", "material": "Kr", "file": "Kr/petrov_2011__s12_Kr_pp32_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p'[3/2]1 = 4s2.4p5.(2P*<1/2>).5p 2[3/2] J = 1 (NIST, 97595.915 cm-1); Paschen 2p4 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p4 \[3/2\]1' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 3\.2309 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Kr\_p12\_0 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Kr_p12_0", "material": "Kr", "file": "Kr/petrov_2011__fig_Kr_p12_0.csv", "table": "fig_c5f6d8609180", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Kr 5p[1/2]0 = 4s2.4p5.(2P*<3/2>).5p 2[1/2] J = 0 (NIST, 94092.863 cm-1); Paschen 2p5 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 4 \(p\. 351\), panel 2p5 5p\[1/2\]0\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 2\.9994 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Kr\_p12\_0 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Kr_p12_0", "material": "Kr", "file": "Kr/petrov_2011__tot_Kr_p12_0.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p[1/2]0 = 4s2.4p5.(2P*<3/2>).5p 2[1/2] J = 0 (NIST, 94092.863 cm-1); Paschen 2p5 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p5 \[1/2\]0 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 2\.9994 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Kr\_p12\_0 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Kr_p12_0", "material": "Kr", "file": "Kr/petrov_2011__s32_Kr_p12_0.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p[1/2]0 = 4s2.4p5.(2P*<3/2>).5p 2[1/2] J = 0 (NIST, 94092.863 cm-1); Paschen 2p5 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p5 \[1/2\]0 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 2\.9994 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Kr\_p12\_0 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Kr_p12_0", "material": "Kr", "file": "Kr/petrov_2011__s12_Kr_p12_0.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p[1/2]0 = 4s2.4p5.(2P*<3/2>).5p 2[1/2] J = 0 (NIST, 94092.863 cm-1); Paschen 2p5 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p5 \[1/2\]0 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 3\.6652 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Kr\_p32\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Kr_p32_2", "material": "Kr", "file": "Kr/petrov_2011__fig_Kr_p32_2.csv", "table": "fig_c5f6d8609180", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Kr 5p[3/2]2 = 4s2.4p5.(2P*<3/2>).5p 2[3/2] J = 2 (NIST, 93123.341 cm-1); Paschen 2p6 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 4 \(p\. 351\), panel 2p6 5p\[3/2\]2\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 3\.1196 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Kr\_p32\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Kr_p32_2", "material": "Kr", "file": "Kr/petrov_2011__tot_Kr_p32_2.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p[3/2]2 = 4s2.4p5.(2P*<3/2>).5p 2[3/2] J = 2 (NIST, 93123.341 cm-1); Paschen 2p6 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p6 \[3/2\]2 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 3\.1196 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Kr\_p32\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Kr_p32_2", "material": "Kr", "file": "Kr/petrov_2011__s32_Kr_p32_2.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p[3/2]2 = 4s2.4p5.(2P*<3/2>).5p 2[3/2] J = 2 (NIST, 93123.341 cm-1); Paschen 2p6 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p6 \[3/2\]2 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 3\.1196 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Kr\_p32\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Kr_p32_2", "material": "Kr", "file": "Kr/petrov_2011__s12_Kr_p32_2.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p[3/2]2 = 4s2.4p5.(2P*<3/2>).5p 2[3/2] J = 2 (NIST, 93123.341 cm-1); Paschen 2p6 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p6 \[3/2\]2 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 3\.7854 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Kr\_p32\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Kr_p32_1", "material": "Kr", "file": "Kr/petrov_2011__fig_Kr_p32_1.csv", "table": "fig_c5f6d8609180", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Kr 5p[3/2]1 = 4s2.4p5.(2P*<3/2>).5p 2[3/2] J = 1 (NIST, 92964.394 cm-1); Paschen 2p7 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 4 \(p\. 351\), panel 2p7 5p\[3/2\]1\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 3\.1393 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Kr\_p32\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Kr_p32_1", "material": "Kr", "file": "Kr/petrov_2011__tot_Kr_p32_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p[3/2]1 = 4s2.4p5.(2P*<3/2>).5p 2[3/2] J = 1 (NIST, 92964.394 cm-1); Paschen 2p7 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p7 \[3/2\]1 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 3\.1393 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Kr\_p32\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Kr_p32_1", "material": "Kr", "file": "Kr/petrov_2011__s32_Kr_p32_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p[3/2]1 = 4s2.4p5.(2P*<3/2>).5p 2[3/2] J = 1 (NIST, 92964.394 cm-1); Paschen 2p7 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p7 \[3/2\]1 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 3\.1393 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Kr\_p32\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Kr_p32_1", "material": "Kr", "file": "Kr/petrov_2011__s12_Kr_p32_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p[3/2]1 = 4s2.4p5.(2P*<3/2>).5p 2[3/2] J = 1 (NIST, 92964.394 cm-1); Paschen 2p7 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p7 \[3/2\]1 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 3\.8051 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Kr\_p52\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Kr_p52_2", "material": "Kr", "file": "Kr/petrov_2011__fig_Kr_p52_2.csv", "table": "fig_c5f6d8609180", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Kr 5p[5/2]2 = 4s2.4p5.(2P*<3/2>).5p 2[5/2] J = 2 (NIST, 92307.379 cm-1); Paschen 2p8 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 4 \(p\. 351\), panel 2p8 5p\[5/2\]2\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 3\.2208 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Kr\_p52\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Kr_p52_2", "material": "Kr", "file": "Kr/petrov_2011__tot_Kr_p52_2.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p[5/2]2 = 4s2.4p5.(2P*<3/2>).5p 2[5/2] J = 2 (NIST, 92307.379 cm-1); Paschen 2p8 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p8 \[5/2\]2 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 3\.2208 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Kr\_p52\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Kr_p52_2", "material": "Kr", "file": "Kr/petrov_2011__s32_Kr_p52_2.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p[5/2]2 = 4s2.4p5.(2P*<3/2>).5p 2[5/2] J = 2 (NIST, 92307.379 cm-1); Paschen 2p8 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p8 \[5/2\]2 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 3\.2208 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Kr\_p52\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Kr_p52_2", "material": "Kr", "file": "Kr/petrov_2011__s12_Kr_p52_2.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p[5/2]2 = 4s2.4p5.(2P*<3/2>).5p 2[5/2] J = 2 (NIST, 92307.379 cm-1); Paschen 2p8 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p8 \[5/2\]2 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 3\.8866 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Kr\_p52\_3 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Kr_p52_3", "material": "Kr", "file": "Kr/petrov_2011__fig_Kr_p52_3.csv", "table": "fig_c5f6d8609180", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Kr 5p[5/2]3 = 4s2.4p5.(2P*<3/2>).5p 2[5/2] J = 3 (NIST, 92294.401 cm-1); Paschen 2p9 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 4 \(p\. 351\), panel 2p9 5p\[5/2\]3\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 3\.2224 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Kr\_p52\_3 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Kr_p52_3", "material": "Kr", "file": "Kr/petrov_2011__tot_Kr_p52_3.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p[5/2]3 = 4s2.4p5.(2P*<3/2>).5p 2[5/2] J = 3 (NIST, 92294.401 cm-1); Paschen 2p9 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p9 \[5/2\]3 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 3\.2224 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Kr\_p52\_3 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Kr_p52_3", "material": "Kr", "file": "Kr/petrov_2011__s32_Kr_p52_3.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p[5/2]3 = 4s2.4p5.(2P*<3/2>).5p 2[5/2] J = 3 (NIST, 92294.401 cm-1); Paschen 2p9 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p9 \[5/2\]3 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 3\.2224 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Kr\_p52\_3 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Kr_p52_3", "material": "Kr", "file": "Kr/petrov_2011__s12_Kr_p52_3.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p[5/2]3 = 4s2.4p5.(2P*<3/2>).5p 2[5/2] J = 3 (NIST, 92294.401 cm-1); Paschen 2p9 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p9 \[5/2\]3 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 3\.8882 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Kr\_p12\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Kr_p12_1", "material": "Kr", "file": "Kr/petrov_2011__fig_Kr_p12_1.csv", "table": "fig_c5f6d8609180", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Kr 5p[1/2]1 = 4s2.4p5.(2P*<3/2>).5p 2[1/2] J = 1 (NIST, 91168.515 cm-1); Paschen 2p10 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 4 \(p\. 351\), panel 2p10 5p\[1/2\]1\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 3\.3620 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Kr\_p12\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Kr_p12_1", "material": "Kr", "file": "Kr/petrov_2011__tot_Kr_p12_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p[1/2]1 = 4s2.4p5.(2P*<3/2>).5p 2[1/2] J = 1 (NIST, 91168.515 cm-1); Paschen 2p10 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p10 \[1/2\]1 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 3\.3620 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Kr\_p12\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Kr_p12_1", "material": "Kr", "file": "Kr/petrov_2011__s32_Kr_p12_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p[1/2]1 = 4s2.4p5.(2P*<3/2>).5p 2[1/2] J = 1 (NIST, 91168.515 cm-1); Paschen 2p10 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p10 \[1/2\]1 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 3\.3620 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Kr\_p12\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Kr_p12_1", "material": "Kr", "file": "Kr/petrov_2011__s12_Kr_p12_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Kr 5p[1/2]1 = 4s2.4p5.(2P*<3/2>).5p 2[1/2] J = 1 (NIST, 91168.515 cm-1); Paschen 2p10 of Kr", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p10 \[1/2\]1 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Kr\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 4\.0278 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Xe\_pp12\_0 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Xe_pp12_0", "material": "Xe", "file": "Xe/petrov_2011__fig_Xe_pp12_0.csv", "table": "fig_f7565eddc4c9", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Xe 6p'[1/2]0 = 5p5.(2P*<1/2>).6p 2[1/2] J = 0 (NIST, 89860.015 cm-1); Paschen 2p1 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 5 \(p\. 351\), panel 2p1 6p'\[1/2\]0\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 2\.2950 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Xe\_pp12\_0 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Xe_pp12_0", "material": "Xe", "file": "Xe/petrov_2011__tot_Xe_pp12_0.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p'[1/2]0 = 5p5.(2P*<1/2>).6p 2[1/2] J = 0 (NIST, 89860.015 cm-1); Paschen 2p1 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p1 \[1/2\]0' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 2\.2950 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Xe\_pp12\_0 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Xe_pp12_0", "material": "Xe", "file": "Xe/petrov_2011__s32_Xe_pp12_0.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p'[1/2]0 = 5p5.(2P*<1/2>).6p 2[1/2] J = 0 (NIST, 89860.015 cm-1); Paschen 2p1 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p1 \[1/2\]0' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 2\.2950 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Xe\_pp12\_0 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Xe_pp12_0", "material": "Xe", "file": "Xe/petrov_2011__s12_Xe_pp12_0.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p'[1/2]0 = 5p5.(2P*<1/2>).6p 2[1/2] J = 0 (NIST, 89860.015 cm-1); Paschen 2p1 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p1 \[1/2\]0' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 3\.6015 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Xe\_pp12\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Xe_pp12_1", "material": "Xe", "file": "Xe/petrov_2011__fig_Xe_pp12_1.csv", "table": "fig_f7565eddc4c9", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Xe 6p'[1/2]1 = 5p5.(2P*<1/2>).6p 2[1/2] J = 1 (NIST, 89278.706 cm-1); Paschen 2p2 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 5 \(p\. 351\), panel 2p2 6p'\[1/2\]1\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 2\.3671 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Xe\_pp12\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Xe_pp12_1", "material": "Xe", "file": "Xe/petrov_2011__tot_Xe_pp12_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p'[1/2]1 = 5p5.(2P*<1/2>).6p 2[1/2] J = 1 (NIST, 89278.706 cm-1); Paschen 2p2 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p2 \[1/2\]1' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 2\.3671 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Xe\_pp12\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Xe_pp12_1", "material": "Xe", "file": "Xe/petrov_2011__s32_Xe_pp12_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p'[1/2]1 = 5p5.(2P*<1/2>).6p 2[1/2] J = 1 (NIST, 89278.706 cm-1); Paschen 2p2 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p2 \[1/2\]1' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 2\.3671 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Xe\_pp12\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Xe_pp12_1", "material": "Xe", "file": "Xe/petrov_2011__s12_Xe_pp12_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p'[1/2]1 = 5p5.(2P*<1/2>).6p 2[1/2] J = 1 (NIST, 89278.706 cm-1); Paschen 2p2 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p2 \[1/2\]1' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 3\.6735 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Xe\_pp32\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Xe_pp32_2", "material": "Xe", "file": "Xe/petrov_2011__fig_Xe_pp32_2.csv", "table": "fig_f7565eddc4c9", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Xe 6p'[3/2]2 = 5p5.(2P*<1/2>).6p 2[3/2] J = 2 (NIST, 89162.356 cm-1); Paschen 2p3 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 5 \(p\. 351\), panel 2p3 6p'\[3/2\]2\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 2\.3815 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Xe\_pp32\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Xe_pp32_2", "material": "Xe", "file": "Xe/petrov_2011__tot_Xe_pp32_2.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p'[3/2]2 = 5p5.(2P*<1/2>).6p 2[3/2] J = 2 (NIST, 89162.356 cm-1); Paschen 2p3 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p3 \[3/2\]2' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 2\.3815 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Xe\_pp32\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Xe_pp32_2", "material": "Xe", "file": "Xe/petrov_2011__s32_Xe_pp32_2.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p'[3/2]2 = 5p5.(2P*<1/2>).6p 2[3/2] J = 2 (NIST, 89162.356 cm-1); Paschen 2p3 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p3 \[3/2\]2' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 2\.3815 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Xe\_pp32\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Xe_pp32_2", "material": "Xe", "file": "Xe/petrov_2011__s12_Xe_pp32_2.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p'[3/2]2 = 5p5.(2P*<1/2>).6p 2[3/2] J = 2 (NIST, 89162.356 cm-1); Paschen 2p3 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p3 \[3/2\]2' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 3\.6880 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Xe\_pp32\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Xe_pp32_1", "material": "Xe", "file": "Xe/petrov_2011__fig_Xe_pp32_1.csv", "table": "fig_f7565eddc4c9", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Xe 6p'[3/2]1 = 5p5.(2P*<1/2>).6p 2[3/2] J = 1 (NIST, 88379.126 cm-1); Paschen 2p4 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 5 \(p\. 351\), panel 2p4 6p'\[3/2\]1\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 2\.4787 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Xe\_pp32\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Xe_pp32_1", "material": "Xe", "file": "Xe/petrov_2011__tot_Xe_pp32_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p'[3/2]1 = 5p5.(2P*<1/2>).6p 2[3/2] J = 1 (NIST, 88379.126 cm-1); Paschen 2p4 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p4 \[3/2\]1' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 2\.4787 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Xe\_pp32\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Xe_pp32_1", "material": "Xe", "file": "Xe/petrov_2011__s32_Xe_pp32_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p'[3/2]1 = 5p5.(2P*<1/2>).6p 2[3/2] J = 1 (NIST, 88379.126 cm-1); Paschen 2p4 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p4 \[3/2\]1' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 2\.4787 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Xe\_pp32\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Xe_pp32_1", "material": "Xe", "file": "Xe/petrov_2011__s12_Xe_pp32_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p'[3/2]1 = 5p5.(2P*<1/2>).6p 2[3/2] J = 1 (NIST, 88379.126 cm-1); Paschen 2p4 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p4 \[3/2\]1' \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 3\.7851 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Xe\_p12\_0 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Xe_p12_0", "material": "Xe", "file": "Xe/petrov_2011__fig_Xe_p12_0.csv", "table": "fig_f7565eddc4c9", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Xe 6p[1/2]0 = 5p5.(2P*<3/2>).6p 2[1/2] J = 0 (NIST, 80118.962 cm-1); Paschen 2p5 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 5 \(p\. 351\), panel 2p5 6p\[1/2\]0\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 3\.5028 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Xe\_p12\_0 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Xe_p12_0", "material": "Xe", "file": "Xe/petrov_2011__tot_Xe_p12_0.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p[1/2]0 = 5p5.(2P*<3/2>).6p 2[1/2] J = 0 (NIST, 80118.962 cm-1); Paschen 2p5 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p5 \[1/2\]0 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 3\.5028 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Xe\_p12\_0 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Xe_p12_0", "material": "Xe", "file": "Xe/petrov_2011__s32_Xe_p12_0.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p[1/2]0 = 5p5.(2P*<3/2>).6p 2[1/2] J = 0 (NIST, 80118.962 cm-1); Paschen 2p5 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p5 \[1/2\]0 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 3\.5028 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Xe\_p12\_0 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Xe_p12_0", "material": "Xe", "file": "Xe/petrov_2011__s12_Xe_p12_0.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p[1/2]0 = 5p5.(2P*<3/2>).6p 2[1/2] J = 0 (NIST, 80118.962 cm-1); Paschen 2p5 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p5 \[1/2\]0 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 4\.8092 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Xe\_p32\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Xe_p32_2", "material": "Xe", "file": "Xe/petrov_2011__fig_Xe_p32_2.csv", "table": "fig_f7565eddc4c9", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Xe 6p[3/2]2 = 5p5.(2P*<3/2>).6p 2[3/2] J = 2 (NIST, 79212.465 cm-1); Paschen 2p6 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 5 \(p\. 351\), panel 2p6 6p\[3/2\]2\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 3\.6152 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Xe\_p32\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Xe_p32_2", "material": "Xe", "file": "Xe/petrov_2011__tot_Xe_p32_2.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p[3/2]2 = 5p5.(2P*<3/2>).6p 2[3/2] J = 2 (NIST, 79212.465 cm-1); Paschen 2p6 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p6 \[3/2\]2 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 3\.6152 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Xe\_p32\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Xe_p32_2", "material": "Xe", "file": "Xe/petrov_2011__s32_Xe_p32_2.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p[3/2]2 = 5p5.(2P*<3/2>).6p 2[3/2] J = 2 (NIST, 79212.465 cm-1); Paschen 2p6 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p6 \[3/2\]2 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 3\.6152 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Xe\_p32\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Xe_p32_2", "material": "Xe", "file": "Xe/petrov_2011__s12_Xe_p32_2.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p[3/2]2 = 5p5.(2P*<3/2>).6p 2[3/2] J = 2 (NIST, 79212.465 cm-1); Paschen 2p6 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p6 \[3/2\]2 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 4\.9216 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Xe\_p32\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Xe_p32_1", "material": "Xe", "file": "Xe/petrov_2011__fig_Xe_p32_1.csv", "table": "fig_f7565eddc4c9", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Xe 6p[3/2]1 = 5p5.(2P*<3/2>).6p 2[3/2] J = 1 (NIST, 78956.031 cm-1); Paschen 2p7 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 5 \(p\. 351\), panel 2p7 6p\[3/2\]1\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 3\.6470 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Xe\_p32\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Xe_p32_1", "material": "Xe", "file": "Xe/petrov_2011__tot_Xe_p32_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p[3/2]1 = 5p5.(2P*<3/2>).6p 2[3/2] J = 1 (NIST, 78956.031 cm-1); Paschen 2p7 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p7 \[3/2\]1 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 3\.6470 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Xe\_p32\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Xe_p32_1", "material": "Xe", "file": "Xe/petrov_2011__s32_Xe_p32_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p[3/2]1 = 5p5.(2P*<3/2>).6p 2[3/2] J = 1 (NIST, 78956.031 cm-1); Paschen 2p7 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p7 \[3/2\]1 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 3\.6470 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Xe\_p32\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Xe_p32_1", "material": "Xe", "file": "Xe/petrov_2011__s12_Xe_p32_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p[3/2]1 = 5p5.(2P*<3/2>).6p 2[3/2] J = 1 (NIST, 78956.031 cm-1); Paschen 2p7 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p7 \[3/2\]1 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 4\.9534 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Xe\_p52\_3 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Xe_p52_3", "material": "Xe", "file": "Xe/petrov_2011__fig_Xe_p52_3.csv", "table": "fig_f7565eddc4c9", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Xe 6p[5/2]3 = 5p5.(2P*<3/2>).6p 2[5/2] J = 3 (NIST, 78403.061 cm-1); Paschen 2p8 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 5 \(p\. 351\), panel 2p8 6p\[5/2\]3\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 3\.7155 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Xe\_p52\_3 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Xe_p52_3", "material": "Xe", "file": "Xe/petrov_2011__tot_Xe_p52_3.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p[5/2]3 = 5p5.(2P*<3/2>).6p 2[5/2] J = 3 (NIST, 78403.061 cm-1); Paschen 2p8 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p9 \[5/2\]3 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 3\.7155 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Xe\_p52\_3 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Xe_p52_3", "material": "Xe", "file": "Xe/petrov_2011__s32_Xe_p52_3.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p[5/2]3 = 5p5.(2P*<3/2>).6p 2[5/2] J = 3 (NIST, 78403.061 cm-1); Paschen 2p8 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p9 \[5/2\]3 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 3\.7155 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Xe\_p52\_3 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Xe_p52_3", "material": "Xe", "file": "Xe/petrov_2011__s12_Xe_p52_3.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p[5/2]3 = 5p5.(2P*<3/2>).6p 2[5/2] J = 3 (NIST, 78403.061 cm-1); Paschen 2p8 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p9 \[5/2\]3 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 5\.0219 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Xe\_p52\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Xe_p52_2", "material": "Xe", "file": "Xe/petrov_2011__fig_Xe_p52_2.csv", "table": "fig_f7565eddc4c9", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Xe 6p[5/2]2 = 5p5.(2P*<3/2>).6p 2[5/2] J = 2 (NIST, 78119.798 cm-1); Paschen 2p9 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 5 \(p\. 351\), panel 2p9 6p\[5/2\]2\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 3\.7506 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Xe\_p52\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Xe_p52_2", "material": "Xe", "file": "Xe/petrov_2011__tot_Xe_p52_2.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p[5/2]2 = 5p5.(2P*<3/2>).6p 2[5/2] J = 2 (NIST, 78119.798 cm-1); Paschen 2p9 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p8 \[5/2\]2 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 3\.7506 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Xe\_p52\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Xe_p52_2", "material": "Xe", "file": "Xe/petrov_2011__s32_Xe_p52_2.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p[5/2]2 = 5p5.(2P*<3/2>).6p 2[5/2] J = 2 (NIST, 78119.798 cm-1); Paschen 2p9 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p8 \[5/2\]2 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 3\.7506 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Xe\_p52\_2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Xe_p52_2", "material": "Xe", "file": "Xe/petrov_2011__s12_Xe_p52_2.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p[5/2]2 = 5p5.(2P*<3/2>).6p 2[5/2] J = 2 (NIST, 78119.798 cm-1); Paschen 2p9 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p8 \[5/2\]2 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 5\.0571 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/fig\_Xe\_p12\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "fig_Xe_p12_1", "material": "Xe", "file": "Xe/petrov_2011__fig_Xe_p12_1.csv", "table": "fig_f7565eddc4c9", "digitised": "vector", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "check", "uncertainty": { "absolute": 0.1, "level": "not stated" }, "parameters": { "initial_level": "Xe 6p[1/2]1 = 5p5.(2P*<3/2>).6p 2[1/2] J = 1 (NIST, 77269.145 cm-1); Paschen 2p10 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Fig\. 5 \(p\. 351\), panel 2p10 6p\[1/2\]1\: the total cross section sigma\_tot \(black line\) against the photon energy, converted from the printed omega\_1/2 \(0 to 6 eV above the 2P1/2 threshold\) by adding 3\.8561 eV \(record notes\); every vertex of the drawn line inside the frame\. At omega\_1/2 = 0 it is Table 2's sigma\_tot^0 within 0\.06 Mb \(script check\)\. 0\.1 Mb\: the digitising uncertainty \(record notes\)\. petrov\_2011/tot\_Xe\_p12\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "tot_Xe_p12_1", "material": "Xe", "file": "Xe/petrov_2011__tot_Xe_p12_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p[1/2]1 = 5p5.(2P*<3/2>).6p 2[1/2] J = 1 (NIST, 77269.145 cm-1); Paschen 2p10 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "total" } } Table 2 \(p\. 352\), row 2p10 \[1/2\]1 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_tot^0 \(footnote a\), the total at the 2P1/2 threshold \(omega\_1/2 = 0\), at the photon energy 3\.8561 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s32\_Xe\_p12\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s32_Xe_p12_1", "material": "Xe", "file": "Xe/petrov_2011__s32_Xe_p12_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p[1/2]1 = 5p5.(2P*<3/2>).6p 2[1/2] J = 1 (NIST, 77269.145 cm-1); Paschen 2p10 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P3/2 ion" } } Table 2 \(p\. 352\), row 2p10 \[1/2\]1 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_3/2^0 \(b\), the partial into the 2P3/2 ion at the 2P1/2 threshold \(omega\_1/2 = 0, photoelectron energy Delta\_FS\), at the photon energy 3\.8561 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. petrov\_2011/s12\_Xe\_p12\_1 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "s12_Xe_p12_1", "material": "Xe", "file": "Xe/petrov_2011__s12_Xe_p12_1.csv", "table": "tbl_63001e98ed74", "quantity": "excited_state_photoionization_cross_section", "unit": "Mb", "abscissa_unit": "eV", "use": "primary", "parameters": { "initial_level": "Xe 6p[1/2]1 = 5p5.(2P*<3/2>).6p 2[1/2] J = 1 (NIST, 77269.145 cm-1); Paschen 2p10 of Xe", "gauge": "length", "method": "CIPFCP: configuration interaction Pauli-Fock with core polarisation (the paper's Sec. 3; Slater integrals scaled as Table 1), length gauge", "channel": "2P1/2 ion" } } Table 2 \(p\. 352\), row 2p10 \[1/2\]1 \(Ar's Paschen label with the jK label; the level is identified by jK, footnote e\), Xe\: sigma\_1/2^Delta\_FS \(c\), the partial into the 2P1/2 ion at omega\_1/2 = Delta\_FS \(photoelectron energy Delta\_FS\), at the photon energy 5\.1625 eV \(record notes\)\. No unit printed\: Mb \(Figs\. 3\-5\)\. No uncertainty stated\. Formulas -------- No formulas are recorded. Corrections ----------- No dataset errata are recorded in this source record. Formula corrections, where recorded, appear with their formulas above. Curation notes may also discuss corrections or unresolved interpretation. Consult the :doc:`review register ` for the checks and decisions.