Helium hydride ion
|Helium hydride ion|
|Jmol-3D images||Image 1|
|Molar mass||5.01054 g mol-1|
|Except where noted otherwise, data are given for materials in their standard state (at 25 °C, 100 kPa)|
The hydrohelium(1+) cation, HeH+, also known as the helium hydride ion, is a positively charged ion formed by the reaction of a proton with a helium atom in the gas phase, first produced in the laboratory in 1925 and isoelectronic with molecular hydrogen. It is the strongest known acid, with a proton affinity of 177.8 kJ/mol. This ion is also called the helium-hydride molecular ion. It has been suggested that HeH+ should occur naturally in the interstellar medium, but it has not yet been detected. It is the simplest heteronuclear ion, and is comparable with the hydrogen molecular ion, H+
2. Unlike H+
2, however, it has a permanent dipole moment, which makes its spectroscopic characterization easier.
HHe+ cannot be prepared in a condensed phase, as it would protonate any anion, molecule or atom with which it were associated. However it is possible to estimate a hypothetical aqueous acidity using Hess's law:
|HHe+(g)||→||H+(g)||+ He(g)||+178 kJ/mol|||
|H+(g)||→||H+(aq)||– 1530 kJ/mol|
|HHe+(aq)||→||H+(aq)||+ He(aq)||– 360 kJ/mol|
Other helium hydride ions are known or have been studied theoretically. HeH+
2, which has been observed using microwave spectroscopy, has a calculated binding energy of 6 kcal/mol, while HeH+
3 has a calculated binding energy of 0.1 kcal/mol.
HeH+ is thought to exist in the interstellar medium, although it has not yet been unambiguously detected. It is believed to be the first compound to have formed in the universe, and is of fundamental importance in understanding the chemistry of the early universe. This is because hydrogen and helium were almost the only types of atoms formed in Big Bang nucleosynthesis. Stars formed from the primordial material should contain HeH+, which could influence their formation and subsequent evolution. In particular, its strong dipole moment makes it relevant to the opacity of zero-metallicity stars. HeH+ is also thought to be an important constituent of the atmospheres of helium-rich white dwarfs, where it increases the opacity of the gas and causes the star to cool more slowly.
Several locations have been suggested as possible places HeH+ might be detected. These include cool helium stars, H II regions, and dense planetary nebulae (in particular NGC 7027). Detecting HeH+ spectroscopically is complicated by the fact that one of its most prominent spectral lines, at 149.14 μm, coincides with a doublet of spectral lines belonging to the methylidyne radical ⫶CH.
HeH+ could be formed in the cooling gas behind dissociative shocks in dense interstellar clouds, such as the shocks caused by stellar winds, supernovae and outflowing material from young stars. If the speed of the shock is greater than about 90 km/s, quantities large enough to detect might be formed. If detected, the emissions from HeH+ would then be useful tracers of the shock.
Unlike the helium hydride ion, the neutral helium hydride molecule is not stable in the ground state. However, it does exist in an excited state as an excimer, and its spectrum was first observed in the mid 1980s.
References and notes
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- Estimated to be the same as for Li+(aq) → Li+(g).
- Estimated from solubility data.
- Coyne, John P.; Ball, David W. (2009). "Alpha particle chemistry. On the formation of stable complexes between He2+ and other simple species: implications for atmospheric and interstellar chemistry". Journal of Molecular Modeling 15 (1): 35–40. doi:10.1007/s00894-008-0371-3. PMID 18936986.
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- Engel, Elodie A.; Doss, Natasha; Harris, Gregory J.; Tennyson, Jonathan (2005). "Calculated spectra for HeH+ and its effect on the opacity of cool metal-poor stars". Monthly Notices of the Royal Astronomical Society 357 (2): 471–477. arXiv:astro-ph/0411267. Bibcode:2005MNRAS.357..471E. doi:10.1111/j.1365-2966.2005.08611.x.
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- Harris, G.J.; Lynas-Gray, A.E.; Miller, S.; Tennyson, J. (2004). "The Role of HeH+ in Cool Helium-rich White Dwarfs". The Astrophysical Journal 617 (2): L143–L146. arXiv:astro-ph/0411331. Bibcode:2004ApJ...617L.143H. doi:10.1086/427391.
- Roberge, W.; Delgarno, A. (1982). "The formation and destruction of HeH/+/ in astrophysical plasmas". The Astrophysical Journal 255: 489–496. Bibcode:1982ApJ...255..489R. doi:10.1086/159849.
- Neufeld, David A.; Dalgarno, A. (1989). "Fast molecular shocks. I – Reformation of molecules behind a dissociative shock". Astrophysical Journal 340: 869–893. Bibcode:1989ApJ...340..869N. doi:10.1086/167441.
- Thomas Möller, Michael Beland, and Georg Zimmerer (1985). "Observation of Fluorescence of the HeH Molecule". Phys. Rev. Lett. 55 (20): 2145–2148. Bibcode:1985PhRvL..55.2145M. doi:10.1103/PhysRevLett.55.2145. PMID 10032060.
- Wolfgang Ketterle, The Nobel Prize in Physics 2001
- W. Ketterle, H. Figger, and H. Walther (1985). "Emission spectra of bound helium hydride". Phys. Rev. Lett. 55 (27): 2941–2944. Bibcode:1985PhRvL..55.2941K. doi:10.1103/PhysRevLett.55.2941. PMID 10032281.