Selected ATcT [1, 2] enthalpy of formation based on version 1.176 of the Thermochemical Network [3]

This version of ATcT results[3] was generated by additional expansion of version 1.172 to include species related to Criegee intermediates that are involved in several ongoing studies[4].

Dihelium anion

Formula: [He2]- (g, quartet 4Pig)
CAS RN: 90188-47-9
ATcT ID: 90188-47-9*1
SMILES: [He][He-]
InChI: InChI=1S/He2/c1-2/q-1
InChIKey: TUONMHFMKUTRCM-UHFFFAOYSA-N
Hills Formula: He2-

2D Image:

[He][He-]
Aliases: [He2]-; Dihelium anion; Dihelium ion (1-); Diatomic helium anion; Diatomic helium ion (1-); Helium dimer anion; Helium dimer ion (1-); Molecular helium anion; Molecular helium ion (1-)
Relative Molecular Mass: 8.0057526 ± 0.0000040

   ΔfH°(0 K)   ΔfH°(298.15 K)UncertaintyUnits
1714.91711.2± 1.9kJ/mol

3D Image of [He2]- (g, quartet 4Pig)

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Top contributors to the provenance of ΔfH° of [He2]- (g, quartet 4Pig)

The 7 contributors listed below account for 92.4% of the provenance of ΔfH° of [He2]- (g, quartet 4Pig).

Please note: The list is limited to 20 most important contributors or, if less, a number sufficient to account for 90% of the provenance. The Reference acts as a further link to the relevant references and notes for the measurement. The Measured Quantity is normaly given in the original units; in cases where we have reinterpreted the original measurement, the listed value may differ from that given by the authors. The quoted uncertainty is the a priori uncertainty used as input when constructing the initial Thermochemical Network, and corresponds either to the value proposed by the original authors or to our estimate; if an additional multiplier is given in parentheses immediately after the prior uncertainty, it corresponds to the factor by which the prior uncertainty needed to be multiplied during the ATcT analysis in order to make that particular measurement consistent with the prevailing knowledge contained in the Thermochemical Network.

Contribution
(%)
TN
ID
Reaction Measured Quantity Reference
42.09309.1 [He2]- (g, quartet 4Pig) → He2 (g, triplet) ΔrH°(0 K) = 0.175 ± 0.030 eVKvale 1986
15.39311.1 [He2]- (g, quartet 4Pig) → 2 He (g) ΔrH°(0 K) = -142978 ± 400 cm-1Pluta 1989, est unc
15.19309.2 [He2]- (g, quartet 4Pig) → He2 (g, triplet) ΔrH°(0 K) = 0.212 ± 0.050 eVPluta 1989, est unc
5.99309.4 [He2]- (g, quartet 4Pig) → He2 (g, triplet) ΔrH°(0 K) = 0.182 ± 0.080 eVMichels 1986, est unc
5.89311.3 [He2]- (g, quartet 4Pig) → 2 He (g) ΔrH°(0 K) = -143465 ± 650 cm-1Michels 1986, est unc
4.39316.2 [He2]- (g, quartet 4Pig) → He (g, triplet) He (g) ΔrH°(0 K) = 1.954 ± 0.080 (×1.164) eVMichels 1986, est unc
3.89311.2 [He2]- (g, quartet 4Pig) → 2 He (g) ΔrH°(0 K) = -143058 ± 800 cm-1Michels 1984, est unc


Most Influential reactions involving [He2]- (g, quartet 4Pig)

Please note: The list, which is based on a hat (projection) matrix analysis, is limited to no more than 20 largest influences.

Influence
Coefficient
TN
ID
Reaction Measured Quantity Reference
0.4209309.1 [He2]- (g, quartet 4Pig) → He2 (g, triplet) ΔrH°(0 K) = 0.175 ± 0.030 eVKvale 1986
0.1539311.1 [He2]- (g, quartet 4Pig) → 2 He (g) ΔrH°(0 K) = -142978 ± 400 cm-1Pluta 1989, est unc
0.1519309.2 [He2]- (g, quartet 4Pig) → He2 (g, triplet) ΔrH°(0 K) = 0.212 ± 0.050 eVPluta 1989, est unc
0.0599309.4 [He2]- (g, quartet 4Pig) → He2 (g, triplet) ΔrH°(0 K) = 0.182 ± 0.080 eVMichels 1986, est unc
0.0589311.3 [He2]- (g, quartet 4Pig) → 2 He (g) ΔrH°(0 K) = -143465 ± 650 cm-1Michels 1986, est unc
0.0439316.2 [He2]- (g, quartet 4Pig) → He (g, triplet) He (g) ΔrH°(0 K) = 1.954 ± 0.080 (×1.164) eVMichels 1986, est unc
0.0389311.2 [He2]- (g, quartet 4Pig) → 2 He (g) ΔrH°(0 K) = -143058 ± 800 cm-1Michels 1984, est unc
0.0379316.1 [He2]- (g, quartet 4Pig) → He (g, triplet) He (g) ΔrH°(0 K) = 2.005 ± 0.100 eVMichels 1984, est unc
0.0379309.3 [He2]- (g, quartet 4Pig) → He2 (g, triplet) ΔrH°(0 K) = 0.233 ± 0.100 eVMichels 1984, est unc


References
1   B. Ruscic, R. E. Pinzon, M. L. Morton, G. von Laszewski, S. Bittner, S. G. Nijsure, K. A. Amin, M. Minkoff, and A. F. Wagner,
Introduction to Active Thermochemical Tables: Several "Key" Enthalpies of Formation Revisited.
J. Phys. Chem. A 108, 9979-9997 (2004) [DOI: 10.1021/jp047912y]
2   B. Ruscic, R. E. Pinzon, G. von Laszewski, D. Kodeboyina, A. Burcat, D. Leahy, D. Montoya, and A. F. Wagner,
Active Thermochemical Tables: Thermochemistry for the 21st Century.
J. Phys. Conf. Ser. 16, 561-570 (2005) [DOI: 10.1088/1742-6596/16/1/078]
3   B. Ruscic and D. H. Bross,
Active Thermochemical Tables (ATcT) values based on ver. 1.176 of the Thermochemical Network (2024); available at ATcT.anl.gov
4   T. L. Nguyen et al, ongoing studies (2024)
5   B. Ruscic,
Uncertainty Quantification in Thermochemistry, Benchmarking Electronic Structure Computations, and Active Thermochemical Tables.
Int. J. Quantum Chem. 114, 1097-1101 (2014) [DOI: 10.1002/qua.24605]
6   B. Ruscic and D. H. Bross,
Thermochemistry
Computer Aided Chem. Eng. 45, 3-114 (2019) [DOI: 10.1016/B978-0-444-64087-1.00001-2]

Formula The aggregate state is given in parentheses following the formula, such as: g - gas-phase, cr - crystal, l - liquid, etc.
Uncertainties The listed uncertainties correspond to estimated 95% confidence limits, as customary in thermochemistry (see, for example, Ruscic [5] and Ruscic and Bross[6]).
Note that an uncertainty of ± 0.000 kJ/mol indicates that the estimated uncertainty is < ± 0.0005 kJ/mol.
Website Functionality Credits The reorganization of the website was developed and implemented by David H. Bross (ANL).
The find function is based on the complete Species Dictionary entries for the appropriate version of the ATcT TN.
The molecule images are rendered by Indigo-depict.
The XYZ renderings are based on Jmol: an open-source Java viewer for chemical structures in 3D. http://www.jmol.org/.
Acknowledgement This work was supported by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, Division of Chemical Sciences, Geosciences and Biosciences under Contract No. DE-AC02-06CH11357.