hohm_1994b ========== U\. Hohm, "Frequency\-dependence of second refractivity virial coefficients of small molecules between 325 nm and 633 nm", Mol\. Phys\. 81, 157 \(1994\) `Source record `__ · :doc:`Catalogue ` · :doc:`Review register ` DOI: `10\.1080/00268979400100111 `__ **Source kind:** measurement **Recorded technique:** Michelson interferometer with a sample cell of length 0\.5 m, illuminated simultaneously by four He\-Ne lasers \(vacuum wavelengths 632\.990, 611\.971, 594\.096 and 543\.516 nm\) and a He\-Cd laser \(325\.130 nm\)\. The cell is evacuated from at most 3e5 Pa while the superposed interferogram I\(rho\_0\) is recorded; Fourier transformation with respect to rho\_0\[1 \+ B\*\(omega\_1, T\) rho\_0\] gives the dispersion of the polarizability of the free molecule, and with respect to rho\_0 the dispersion of B\*\(omega, T\) and hence of B\_R relative to a fixed reference value B\_R^\(0\)\(omega\_1, T\) \(Eqs\. 7\-13, pp\. 159\-161\)\. Room temperature, 292\-299 K \(p\. 157, Tables 1\-2\)\. **Materials in structured entries:** Ar, CH4, CO2, Kr, N2O, O2, Xe **Dataset quantities:** polarizability, refractivity\_virial\_coefficient **Contents:** 31 datasets; 0 formulas. Curation notes -------------- Page numbers are the journal's \(157\-168\); pdf pages 1\-2 are the publisher's cover, so p\. = pdf page \+ 154\. The paper that hohm\_1994 \(Chem\. Phys\. 179, 533\) cites as 'U\. Hohm, Mol\. Phys\. \(1993\); in press' \(its ref\. \[29\]\)\: its O2, N2O and CO2 inputs are this paper's Table 1 rows, digit for digit\. Reduction \(Eqs\. 7\-9, p\. 159\)\: \(n^2 \- 1\)/\(n^2 \+ 2\) = sum\_k A\_k\(omega, T\) rho\_0^\(k\-1\) with the ideal\-gas density rho\_0 = p/RT; A\_1 = N\_A alpha\_0\(omega, T\)/\(3 eps0\) is the polarizability of the free molecule \(zero density\), so the Table 1 values need no state\. Atomic units of polarizability\. The wavelengths are vacuum wavelengths \(p\. 159; Table 1 note a prints 632\.99 nm, the text 632\.990 nm\)\. Table 1 \(p\. 160\)\: mean polarizabilities at the five wavelengths, with the gas temperature\. Rows marked b are this work, h are 'already given elsewhere \[4\]' \(Hohm, Mol\. Phys\. 78, 929 \(1993\), hohm\_1993; p\. 160\)\: among the curated gases, CH4\. The second row of each gas is 'calculated using Cauchy moments' of a DOSD \(note b\: c \[21\] Kumar and Meath 1985, d \[22\] Zeiss et al\. 1977, e \[23\] Thomas and Meath 1977, j \[28\] Jhanwar and Meath 1982; f \[24\], g \[25\], i \[27\] belong to out\-of\-scope molecules\)\. The digits in parentheses are the uncertainty of the last digits; the paper does not say what they are \(level not stated\)\. They are the same at all five wavelengths of a gas \(0\.0020 au for argon, 1\.8e\-4 of alpha\), which suggests the uncertainty of the absolute level; the dispersion itself is claimed to about 1e\-5 relative to alpha\(omega\_1\) \(hohm\_1994, p\. 536, 'Delta alpha\(omega\)/alpha\(omega\) ~ 10^\-5 with respect to a reference value'; this paper states no figure\)\. 'Overall, there is a very good agreement between the dispersion \[alpha\(omega\_5\) \- alpha\(omega\_1\)\] \.\.\. measured in this work and the values given in the literature' \(p\. 161\)\. Xe and N2O have no measurement at 611\.971 nm\. Table 2 \(p\. 162\)\: B\_R\(omega\_k, T\) in 1e\-12 m^6 mol^\-2 \(= cm^6/mol^2\)\. Only the dispersion of B\*\(omega\) = A\_2/A\_1 is measured; B\_R\(omega\_k\) follows from Eqs\. \(12\)\-\(13\) with a reference value B\_R^\(0\)\(omega\_1, T\) \(the omega\_1 column\)\: from Burns et al\. 1986 \(note a, \[8\]\) for Ar, Kr, Xe, CO2 and CH4; estimated by Hohm's heuristic extrapolation of Buckingham's theory \(note b, \[12\], U\. Hohm, Z\. Naturforsch\. A 48, 505 \(1993\)\) for O2 and N2O, whose absolute B\_R is 'estimated for the first time' \(p\. 164\)\. So the omega\_3\-omega\_5 values are this work relative to the reference and not independent of it\. 'The uncertainties of B\_R\(omega\_k\>1, T\) are given relative to B\_R\(omega\_1, T\)' \(caption\); Delta B\* ~ 1e\-7 m^3/mol \(pp\. 166\-167\); 'However, the full uncertainty in B\_R might be approximately twice the error given above' \(p\. 167\), since the two CO2 runs do not overlap\. The datasets keep the printed uncertainties; the full one is about twice\. \(1\) and \(2\) are two independent measurements \(Xe, CO2\)\. The last column, 10^6 B\*\(omega\_1\) in m^3/mol, is a fit constant \(not extracted\); for CH4 it is Hohm 1993's B\_2\*\(omega\_1\) = 48\.58\(1\.20\) cm^3/mol, and the CH4 B\_R\(omega\_4\), B\_R\(omega\_5\) follow from that paper's Table 3 B\_2\* \(49\.17, 49\.00\) by Eq\. \(13\) with Burns's 7\.76 \(checked\: 11\.72, 11\.14\)\. Footnotes \(checked on the image, p\. 162\)\: c 'lambda = 688 nm, \[29\]' \(NH3; the text, p\. 165, says 668 nm\), d 'T = 373 K, \[9\]' \(the library renders it as T approximately 373 K\), f the Kr B\_R\(omega\_2\) = 6\.46\(54\) x 10^\-12 m^6 mol^\-2 \(the library renders the unit as mol^\-1; the image has mol^\-2\)\. Xe shows anomalous dispersion of B\_R, doubted by the author \(p\. 163, Bulanin's private communication\)\. Checks against optmat's fits \(2026\-09\-26\)\: argon's measured shape alpha\(omega\_k\)/ alpha\(omega\_1\) departs from fit/Ar \(ab initio moments with refractometry\) by \+26, \-5, \-6 and \-70 ppm at 612, 594, 544 and 325 nm, several times the 1e\-5 claimed for the dispersion \(hohm\_1994, p\. 536\); its absolute level is \+117 ppm \(within the printed 0\.0020 au\)\. The absolute levels are \+0\.20 % \(Kr\), \+0\.47 % \(Xe\), \+0\.21 % \(O2\), \+0\.16 % \(N2O\), \+0\.04 % \(CO2\) and \+0\.04 % \(CH4\) against the fits at 633 nm; the 325 nm shape departs by \+260 \(Kr\), \+158 \(Xe\) and \+157 ppm \(CH4\), the others within 55 ppm\. Not extracted\: NH3, C2H4, C2H6, C3H6 and cyclo\-C3H6 \(not curated species\); B\* and the figures \(B\_R dispersion curves against the heuristic estimate\); the discussion of the expansion technique's fitting bias \(Eqs\. 14\-16\)\. **Recorded bibliographic identity status:** VALIDATED\_WITH\_WARNINGS. This concerns identification of the source; it does not establish the scientific correctness of its contents. Datasets -------- hohm\_1994b/alpha\_Ar ~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "alpha_Ar", "material": "Ar", "file": "Ar/hohm_1994b__alpha_Ar.csv", "table": "tbl_43f3f21f6009", "quantity": "polarizability", "unit": "au", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "primary", "uncertainty": { "column": true, "level": "not stated" }, "parameters": { "temperature_k": 296.82 } } Table 1 \(p\. 160\), this work \(b\), 296\.82\(1\) K; the parenthesised last digits in the sigma column, level not stated\. hohm\_1994b/kumar\_1985\_Ar ~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "kumar_1985_Ar", "material": "Ar", "file": "Ar/hohm_1994b__kumar_1985_Ar.csv", "table": "tbl_43f3f21f6009", "quantity": "polarizability", "unit": "au", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "reproduced", "reproduced_from": [ "kumar_1985" ] } Table 1, row c\: calculated by Hohm from Kumar and Meath's \(1985\) Cauchy moments\. hohm\_1994b/alpha\_Kr ~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "alpha_Kr", "material": "Kr", "file": "Kr/hohm_1994b__alpha_Kr.csv", "table": "tbl_43f3f21f6009", "quantity": "polarizability", "unit": "au", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "primary", "uncertainty": { "column": true, "level": "not stated" }, "parameters": { "temperature_k": 296.29 } } Table 1 \(p\. 160\), this work \(b\), 296\.29\(1\) K; the parenthesised last digits in the sigma column, level not stated\. hohm\_1994b/kumar\_1985\_Kr ~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "kumar_1985_Kr", "material": "Kr", "file": "Kr/hohm_1994b__kumar_1985_Kr.csv", "table": "tbl_43f3f21f6009", "quantity": "polarizability", "unit": "au", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "reproduced", "reproduced_from": [ "kumar_1985" ] } Table 1, row c\: calculated by Hohm from Kumar and Meath's \(1985\) Cauchy moments\. hohm\_1994b/alpha\_Xe ~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "alpha_Xe", "material": "Xe", "file": "Xe/hohm_1994b__alpha_Xe.csv", "table": "tbl_43f3f21f6009", "quantity": "polarizability", "unit": "au", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "primary", "uncertainty": { "column": true, "level": "not stated" }, "parameters": { "temperature_k": 293.6 } } Table 1 \(p\. 160\), this work \(b\), 293\.60\(1\) K, no value at 611\.971 nm; the parenthesised last digits in the sigma column, level not stated\. hohm\_1994b/kumar\_1985\_Xe ~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "kumar_1985_Xe", "material": "Xe", "file": "Xe/hohm_1994b__kumar_1985_Xe.csv", "table": "tbl_43f3f21f6009", "quantity": "polarizability", "unit": "au", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "reproduced", "reproduced_from": [ "kumar_1985" ] } Table 1, row c\: calculated by Hohm from Kumar and Meath's \(1985\) Cauchy moments\. hohm\_1994b/alpha\_O2 ~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "alpha_O2", "material": "O2", "file": "O2/hohm_1994b__alpha_O2.csv", "table": "tbl_43f3f21f6009", "quantity": "polarizability", "unit": "au", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "primary", "uncertainty": { "column": true, "level": "not stated" }, "parameters": { "temperature_k": 292.06 } } Table 1 \(p\. 160\), this work \(b\), 292\.06\(3\) K \(Table 2 prints 292\.06\(2\)\); the parenthesised last digits in the sigma column, level not stated\. Reprinted as hohm\_1994/input\_O2\. hohm\_1994b/zeiss\_1977\_O2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "zeiss_1977_O2", "material": "O2", "file": "O2/hohm_1994b__zeiss_1977_O2.csv", "table": "tbl_43f3f21f6009", "quantity": "polarizability", "unit": "au", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "reproduced", "reproduced_from": [ "zeiss_1977" ] } Table 1, row d\: calculated by Hohm from the Cauchy moments of Zeiss et al\. \(1977\)\. hohm\_1994b/alpha\_N2O ~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "alpha_N2O", "material": "N2O", "file": "N2O/hohm_1994b__alpha_N2O.csv", "table": "tbl_43f3f21f6009", "quantity": "polarizability", "unit": "au", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "primary", "uncertainty": { "column": true, "level": "not stated" }, "parameters": { "temperature_k": 295.05 } } Table 1 \(p\. 160\), this work \(b\), 295\.05\(2\) K, no value at 611\.971 nm; the parenthesised last digits in the sigma column, level not stated\. Reprinted as hohm\_1994/input\_N2O\. hohm\_1994b/zeiss\_1977\_N2O ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "zeiss_1977_N2O", "material": "N2O", "file": "N2O/hohm_1994b__zeiss_1977_N2O.csv", "table": "tbl_43f3f21f6009", "quantity": "polarizability", "unit": "au", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "reproduced", "reproduced_from": [ "zeiss_1977" ] } Table 1, row d\: calculated by Hohm from the Cauchy moments of Zeiss et al\. \(1977\)\. hohm\_1994b/alpha\_CO2 ~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "alpha_CO2", "material": "CO2", "file": "CO2/hohm_1994b__alpha_CO2.csv", "table": "tbl_43f3f21f6009", "quantity": "polarizability", "unit": "au", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "primary", "uncertainty": { "column": true, "level": "not stated" }, "parameters": { "temperature_k": 293.8 } } Table 1 \(p\. 160\), this work \(b\), 293\.80\(1\) K; the parenthesised last digits in the sigma column, level not stated\. Reprinted as hohm\_1994/input\_CO2\. hohm\_1994b/jhanwar\_1982\_CO2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "jhanwar_1982_CO2", "material": "CO2", "file": "CO2/hohm_1994b__jhanwar_1982_CO2.csv", "table": "tbl_43f3f21f6009", "quantity": "polarizability", "unit": "au", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "reproduced", "reproduced_from": [ "jhanwar_1982" ] } Table 1, row j \(\[28\]\)\: calculated by Hohm from Jhanwar and Meath's Cauchy moments \(not in the library\)\. Spackman's \(1991\) Meath moments of CO2 \(S\(\-2\), S\(\-4\), S\(\-6\) = 17\.51, 50\.99, 211\.4\) reproduce this row to 4e\-4 au at 544\-633 nm, so they are the same DOSD\. hohm\_1994b/alpha\_CH4 ~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "alpha_CH4", "material": "CH4", "file": "CH4/hohm_1994b__alpha_CH4.csv", "table": "tbl_43f3f21f6009", "quantity": "polarizability", "unit": "au", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "reproduced", "reproduced_from": [ "hohm_1993" ], "uncertainty": { "column": true, "level": "not stated" }, "parameters": { "temperature_k": 294.47 } } Table 1, row h \(\[4\]\)\: Hohm's 1993 CH4 values at 294\.47\(1\) K, digit\-identical to hohm\_1993/alpha\_CH4\. hohm\_1994b/thomas\_1977\_CH4 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "thomas_1977_CH4", "material": "CH4", "file": "CH4/hohm_1994b__thomas_1977_CH4.csv", "table": "tbl_43f3f21f6009", "quantity": "polarizability", "unit": "au", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "reproduced", "reproduced_from": [ "thomas_1977" ] } Table 1, row e \(\[23\]\)\: calculated from Thomas and Meath's Cauchy moments; identical to hohm\_1993/thomas\_1977\_CH4\. hohm\_1994b/B\_R\_reference\_Ar ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "B_R_reference_Ar", "material": "Ar", "file": "Ar/hohm_1994b__B_R_reference_Ar.csv", "table": "tbl_83390c4d1bfd", "quantity": "refractivity_virial_coefficient", "unit": "cm6/mol2", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "reproduced", "reproduced_from": [ "burns_1986" ], "uncertainty": { "column": true, "level": "not stated" } } Table 2, omega\_1 column \(note a, \[8\]\)\: the reference value, Burns et al\.'s 1\.57\(58\) at 632\.8 nm \(burns\_1986/B\_R\_Ar, at room temperature, 298\.2 K\), listed here at omega\_1\. hohm\_1994b/B\_R\_Ar ~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "B_R_Ar", "material": "Ar", "file": "Ar/hohm_1994b__B_R_Ar.csv", "table": "tbl_83390c4d1bfd", "quantity": "refractivity_virial_coefficient", "unit": "cm6/mol2", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "primary", "uncertainty": { "column": true, "level": "not stated" }, "parameters": { "temperature_k": 296.82 } } Table 2 \(p\. 162\), this work at omega\_3\-omega\_5, 296\.82\(2\) K, relative to Burns et al\.'s 1\.57 at omega\_1 \(not independent of it\)\. Printed uncertainty relative to the reference; the full uncertainty is 'approximately twice' \(p\. 167\)\. hohm\_1994b/B\_R\_reference\_Kr ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "B_R_reference_Kr", "material": "Kr", "file": "Kr/hohm_1994b__B_R_reference_Kr.csv", "table": "tbl_83390c4d1bfd", "quantity": "refractivity_virial_coefficient", "unit": "cm6/mol2", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "reproduced", "reproduced_from": [ "burns_1986" ], "uncertainty": { "column": true, "level": "not stated" } } Table 2, omega\_1 column \(note a, \[8\]\)\: Burns et al\.'s 6\.23\(155\) at 632\.8 nm \(burns\_1986/B\_R\_Kr, 298\.2 K\)\. hohm\_1994b/B\_R\_Kr ~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "B_R_Kr", "material": "Kr", "file": "Kr/hohm_1994b__B_R_Kr.csv", "table": "tbl_83390c4d1bfd", "quantity": "refractivity_virial_coefficient", "unit": "cm6/mol2", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "primary", "uncertainty": { "column": true, "level": "not stated" }, "parameters": { "temperature_k": 296.29 } } Table 2 \(p\. 162\), this work at omega\_3\-omega\_5, 296\.29\(1\) K, relative to Burns et al\.'s 6\.23 at omega\_1\. Printed uncertainty relative to the reference; the full uncertainty is 'approximately twice' \(p\. 167\)\. The omega\_2 value is in footnote f \(B\_R\_omega2\_Kr\)\. hohm\_1994b/B\_R\_omega2\_Kr ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "B_R_omega2_Kr", "material": "Kr", "table": "text", "quantity": "refractivity_virial_coefficient", "unit": "cm6/mol2", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "primary", "uncertainty": { "column": true, "level": "not stated" }, "parameters": { "temperature_k": 296.29 } } 1 inline points in the source record. Table 2 footnote f \(p\. 162\)\: 'B\_R\(omega\_2, T\) = 6\.46\(54\) x 10^\-12 m^6 mol^\-2' for Kr \(the image; the library's caption text renders the unit as mol^\-1\)\. As B\_R\_Kr\. hohm\_1994b/B\_R\_reference\_Xe ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "B_R_reference_Xe", "material": "Xe", "file": "Xe/hohm_1994b__B_R_reference_Xe.csv", "table": "tbl_83390c4d1bfd", "quantity": "refractivity_virial_coefficient", "unit": "cm6/mol2", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "reproduced", "reproduced_from": [ "burns_1986" ], "uncertainty": { "column": true, "level": "not stated" } } Table 2, omega\_1 column \(note a, \[8\]\), printed with both Xe runs\: Burns et al\.'s 25\.5\(285\) at 632\.8 nm \(burns\_1986/B\_R\_Xe, 298\.2 K\)\. hohm\_1994b/B\_R\_1\_Xe ~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "B_R_1_Xe", "material": "Xe", "file": "Xe/hohm_1994b__B_R_1_Xe.csv", "table": "tbl_83390c4d1bfd", "quantity": "refractivity_virial_coefficient", "unit": "cm6/mol2", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "primary", "uncertainty": { "column": true, "level": "not stated" }, "parameters": { "temperature_k": 293.6 } } Table 2 \(p\. 162\), Xe run \(1\), 293\.60\(1\) K, omega\_4 and omega\_5, relative to Burns et al\.'s 25\.5 at omega\_1\. B\_R falls with frequency \(anomalous dispersion\), which the author doubts \(p\. 163\)\. Full uncertainty 'approximately twice' the printed one \(p\. 167\)\. hohm\_1994b/B\_R\_2\_Xe ~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "B_R_2_Xe", "material": "Xe", "file": "Xe/hohm_1994b__B_R_2_Xe.csv", "table": "tbl_83390c4d1bfd", "quantity": "refractivity_virial_coefficient", "unit": "cm6/mol2", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "primary", "uncertainty": { "column": true, "level": "not stated" }, "parameters": { "temperature_k": 294.05 } } Table 2, Xe run \(2\), 294\.05\(2\) K, an independent measurement; as B\_R\_1\_Xe \(both print 23\.25\(80\) at omega\_5\)\. hohm\_1994b/B\_R\_reference\_O2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "B_R_reference_O2", "material": "O2", "file": "O2/hohm_1994b__B_R_reference_O2.csv", "table": "tbl_83390c4d1bfd", "quantity": "refractivity_virial_coefficient", "unit": "cm6/mol2", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "reproduced", "reproduced_from": [ "U. Hohm, Z. Naturforsch. A 48, 505 (1993)" ], "parameters": { "temperature_k": 292.06 } } Table 2, omega\_1 column \(note b, \[12\]\)\: 0\.82, no uncertainty, estimated by Hohm's heuristic extrapolation of Buckingham's theory \(theory, not a measurement; p\. 161 and p\. 164\)\. hohm\_1994b/B\_R\_O2 ~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "B_R_O2", "material": "O2", "file": "O2/hohm_1994b__B_R_O2.csv", "table": "tbl_83390c4d1bfd", "quantity": "refractivity_virial_coefficient", "unit": "cm6/mol2", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "primary", "uncertainty": { "column": true, "level": "not stated" }, "parameters": { "temperature_k": 292.06 } } Table 2 \(p\. 162\), 292\.06\(2\) K, omega\_4 and omega\_5, relative to the estimated 0\.82 at omega\_1\: the dispersion is measured, the absolute level is the estimate's\. The first B\_R dispersion of O2 \(p\. 164\)\. Full uncertainty 'approximately twice' the printed one \(p\. 167\)\. hohm\_1994b/B\_R\_reference\_N2O ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "B_R_reference_N2O", "material": "N2O", "file": "N2O/hohm_1994b__B_R_reference_N2O.csv", "table": "tbl_83390c4d1bfd", "quantity": "refractivity_virial_coefficient", "unit": "cm6/mol2", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "reproduced", "reproduced_from": [ "U. Hohm, Z. Naturforsch. A 48, 505 (1993)" ], "parameters": { "temperature_k": 295.05 } } Table 2, omega\_1 column \(note b, \[12\]\)\: 22\.42, no uncertainty, Hohm's heuristic estimate \(theory\)\. hohm\_1994b/B\_R\_N2O ~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "B_R_N2O", "material": "N2O", "file": "N2O/hohm_1994b__B_R_N2O.csv", "table": "tbl_83390c4d1bfd", "quantity": "refractivity_virial_coefficient", "unit": "cm6/mol2", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "primary", "uncertainty": { "column": true, "level": "not stated" }, "parameters": { "temperature_k": 295.05 } } Table 2 \(p\. 162\), 295\.05\(2\) K, omega\_4 and omega\_5, relative to the estimated 22\.42 at omega\_1 \(absolute level the estimate's\)\. Full uncertainty 'approximately twice' the printed one \(p\. 167\)\. hohm\_1994b/B\_R\_reference\_CO2 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "B_R_reference_CO2", "material": "CO2", "file": "CO2/hohm_1994b__B_R_reference_CO2.csv", "table": "tbl_83390c4d1bfd", "quantity": "refractivity_virial_coefficient", "unit": "cm6/mol2", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "reproduced", "reproduced_from": [ "burns_1986" ], "uncertainty": { "column": true, "level": "not stated" } } Table 2, omega\_1 column \(note a, \[8\]\), printed with both CO2 runs\: Burns et al\.'s 4\.75\(130\) at 632\.8 nm \(burns\_1986/B\_R\_CO2, 298\.2 K\)\. hohm\_1994b/B\_R\_1\_CO2 ~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "B_R_1_CO2", "material": "CO2", "file": "CO2/hohm_1994b__B_R_1_CO2.csv", "table": "tbl_83390c4d1bfd", "quantity": "refractivity_virial_coefficient", "unit": "cm6/mol2", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "primary", "uncertainty": { "column": true, "level": "not stated" }, "parameters": { "temperature_k": 293.8 } } Table 2 \(p\. 162\), CO2 run \(1\), 293\.80\(1\) K, omega\_3\-omega\_5, relative to Burns et al\.'s 4\.75\. The two runs' error bars do not overlap \(7\.33 against 5\.74, 8\.96 against 6\.83\), the reason the author puts the full uncertainty at 'approximately twice' the printed one \(p\. 167\)\. hohm\_1994b/B\_R\_2\_CO2 ~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "B_R_2_CO2", "material": "CO2", "file": "CO2/hohm_1994b__B_R_2_CO2.csv", "table": "tbl_83390c4d1bfd", "quantity": "refractivity_virial_coefficient", "unit": "cm6/mol2", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "primary", "uncertainty": { "column": true, "level": "not stated" }, "parameters": { "temperature_k": 299.26 } } Table 2, CO2 run \(2\), 299\.26\(1\) K, omega\_3 and omega\_4 \(no omega\_5\); as B\_R\_1\_CO2\. hohm\_1994b/B\_R\_reference\_CH4 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "B_R_reference_CH4", "material": "CH4", "file": "CH4/hohm_1994b__B_R_reference_CH4.csv", "table": "tbl_83390c4d1bfd", "quantity": "refractivity_virial_coefficient", "unit": "cm6/mol2", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "reproduced", "reproduced_from": [ "burns_1986" ], "uncertainty": { "column": true, "level": "not stated" } } Table 2, omega\_1 column \(note a, \[8\]\)\: Burns et al\.'s 7\.76\(132\) at 632\.8 nm \(burns\_1986/B\_R\_CH4, 298\.2 K\)\. hohm\_1994b/B\_R\_CH4 ~~~~~~~~~~~~~~~~~~~~~ .. code-block:: text { "id": "B_R_CH4", "material": "CH4", "file": "CH4/hohm_1994b__B_R_CH4.csv", "table": "tbl_83390c4d1bfd", "quantity": "refractivity_virial_coefficient", "unit": "cm6/mol2", "abscissa_unit": "nm", "wavelength_medium": "vacuum", "use": "primary", "uncertainty": { "column": true, "level": "not stated" }, "parameters": { "temperature_k": 294.47 } } Table 2 \(p\. 162\), 294\.47\(1\) K, omega\_4 and omega\_5 \(uncertainty printed '\(0·5\)', absolute\), relative to Burns et al\.'s 7\.76\. The measurement is Hohm 1993's \(Figure 6 '\[4\]'; its Table 3 B\_2\* = 49\.17 and 49\.00 cm^3/mol, which give these values by Eq\. \(13\)\: checked\); hohm\_1993 records no B\_R, so this is the first B\_R\. Full uncertainty 'approximately twice' the printed one \(p\. 167\)\. 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.