Helium hydride ion

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Helium hydride ion
Spacefill model of the helium hydride ion
Ball and stick model of the helium hydride ion
Names
Systematic IUPAC name
Hydridohelium(1+)[1]
Identifiers
3D model (JSmol)
ChEBI
ChemSpider
2
Properties
HeH+
Molar mass 5.01054 g·mol−1
Conjugate base Helium
Except where otherwise noted, data are given for materials in their standard state (at 25 °C [77 °F], 100 kPa).
Infobox references

The helium hydride ion or hydridohelium(1+) ion is a cation (positively charged ion) with chemical formula HeH+. It consists of a helium atom bonded to a hydrogen atom, with one electron removed. It is the lightest heteronuclear ion, and is believed to be one of the first compounds formed in the universe after the big bang.[2]

The ion was first produced in a laboratory in 1925. It is stable in isolation, but extremely reactive, and cannot be prepared in bulk because it would react with any other molecule it came in contact with. Noted as the strongest known acid, its occurrence in the interstellar medium has been conjectured since the 1970s,[3] and it was finally detected in April 2019.[4]

Physical properties[edit]

The helium hydrogen ion is isoelectronic with molecular hydrogen (H
2
).[4]

Unlike the dihydrogen ion H+
2
, the helium hydride ion has a permanent dipole moment, which makes its spectroscopic characterization easier.[5] The calculated dipole moment of HeH+ is 2.26 or 2.84 D.[6] The electron density in the molecule is higher around the helium nucleus than the hydrogen. 80% of the electron charge is closer to the helium nucleus than to the hydrogen nucleus.[7]

One of its most prominent spectral lines, at 149.14 μm, coincides with a doublet of spectral lines belonging to the methylidyne radical CH.[8]

The length of the covalent bond in the ion is 0.772 Å.[9]

Isotopologues[edit]

The helium hydride ion has six relatively stable isotopologues, that differ in the isotopes of the two elements, and hence in the total atomic mass number (A) and the total number of neutrons (N) in the two nuclei:

  • [3
    He1
    H]+ or [3
    HeH]+ (A = 4, N = 1) [10][11]
  • [3
    He2
    H]+ or [3
    HeD]+ (A = 5, N = 2) [10][11]
  • [3
    He3
    H]+ or [3
    HeT]+ (A = 6, N = 3; radioactive) [12][10][13]
  • [4
    He1
    H]+ or [4
    HeH]+ (A = 5, N = 2) [4][14][15][2][11]
  • [4
    He2
    H]+ or [4
    HeD]+ (A = 6, N = 3) [14][11]
  • [4
    He3
    H]+ or [4
    HeT]+ (A = 7, N = 4; radioactive) 

They all have three protons and two electrons. The first three are generated by radioactive decay of tritium in the molecules HT = 1
H3
H, DT = 2
H3
H, and T
2
= 3
H
2
, respectively. The last three can be generated by ionizing the appropriate isotopologue of H
2
in the presence of helium-4.[4]

The following isotopologues of the helium hydride ion, of the dihydrogen ion H
2
, and of the trihydrogen ion H+
3
have the same total atomic mass number A:

  • [3
    HeH]+, [D
    2
    ]+, [TH]+, [DH
    2
    ]+ (A = 4)
  • [3
    HeD]+, [4
    HeH]+, [DT]+, [TH
    2
    ]+, [D
    2
    H]+ (A = 5)
  • [3
    HeT]+, [4
    HeD]+, [T
    2
    ]+, [TDH]+, [D
    3
    ]+ (A = 6)
  • [4
    HeT]+, [TD
    2
    ]+, [T
    2
    H]+ (A = 7)

The masses in each row above are not equal, though, because the binding energies in the nuclei are different.[14]

Neutral molecule[edit]

Unlike the helium hydride ion, the neutral helium hydride molecule HeH is not stable in the ground state. However, it does exist in an excited state as an excimer (HeH*), and its spectrum was first observed in the mid 1980s.[16][17][18]

The neutral molecule is the first entry in the Gmelin database.[3]

Chemical properties and reactions[edit]

Preparation[edit]

Since HeH+ cannot be stored in any usable form, its chemistry must be studied by forming it in situ.

Reactions with organic substances, for example, can be studied by creating a tritium derivative of the desired organic compound. Decay of tritium to 3He+ followed by its extraction of a hydrogen atom yields 3HeH+ which is then surrounded by the organic material and will in turn react.[19][20]

Acidity[edit]

HeH+ cannot be prepared in a condensed phase, as it would donate a proton to any anion, molecule or atom that it came in contact with. It has been shown to protonate O2, NH3, SO2, H2O, and CO2, giving O2H+, NH+
4
, HSO+
2
, H3O+, and HCO+
2
.[19] Other molecules such as nitric oxide, nitrogen dioxide, nitrous oxide, hydrogen sulfide, methane, acetylene, ethylene, ethane, methanol and acetonitrile react but break up due to the large amount of energy produced.[19]

In fact, HeH+ is the strongest known acid, with a proton affinity of 177.8 kJ/mol.[21] The hypothetical aqueous acidity can be estimated using Hess's law:

HeH+(g) H+(g) + He(g) +178 kJ/mol   [21]
HeH+(aq) HeH+(g)   +973 kJ/mol   (a)
H+(g) H+(aq)   −1530 kJ/mol  
He(g) He(aq)   +19 kJ/mol   (b)
HeH+(aq) H+(aq) + He(aq) −360 kJ/mol  

(a) Estimated to be same as for Li+(aq) → Li+(g).
(b) Estimated from solubility data.

A free energy change of dissociation of −360 kJ/mol is equivalent to a pKa of −63.

Other helium-hydrogen ions[edit]

Additional helium atoms can attach to HeH+ to form larger clusters such as He2H+, He3H+, He4H+, He5H+ and He6H+.[19]

The dihelium hydride cation, He2H+, is formed by the reaction of dihelium cation with molecular hydrogen:

He+
2
+ H2 → He2H+ + H

It is a linear ion with hydrogen in the centre.[19]

The hexahelium hydride ion, He6H+, is particularly stable.[19]

Other helium hydride ions are known or have been studied theoretically. Helium dihydride ion, or dihydridohelium(1+), HeH+
2
, has been observed using microwave spectroscopy.[22] It has a calculated binding energy of 25.1 kJ/mol, while trihydridohelium(1+), HeH+
3
, has a calculated binding energy of 0.42 kJ/mol.[23]

History[edit]

Discovery in ionization experiments[edit]

Hydridohelium(1+), specifically [4
He1
H]+, was first detected indirectly in 1925 by T. R. Hogness and E. G. Lunn. They were injecting protons of known energy into a rarefied mixture of hydrogen and helium, in order to study the formation of hydrogen ions like H+
, H+
2
and H+
3
. They observed that H+
3
appeared at the same beam energy (16 eV) as H+
2
, and its concentration increased with pressure much more than that of the other two ions. From this data, they concluded that the H+
2
ions were transferring a proton to molecules that they collided with, including helium.[4]

In 1933, K. Bainbridge used mass spectrometry to compare the masses of the ions [4
He1
H]+ (helium hydride ion) and [2
H
2
1
H]+ (twice-deuterated trihydrogen ion) in order to obtain an accurate measurement of the atomic mass of deuterium relative to that of helium. Both ions have 3 protons, 2 neutrons, and 2 electrons. He also compared [4
He2
H]+ (helium deuteride ion) with [2
H
3
]+ (trideuterium ion), both with 3 protons and 3 neutrons.[14]

Early theoretical studies[edit]

The first attempt to compute the structure of the HeH+ ion (specifically, [4
He1
H]+) by quantum mechanical theory was made by J. Beach in 1936.[24] Improved computations were sporadically published over the next decades.[25] [26]

Tritium decay methods in chemistry[edit]

H. Schwartz observed in 1955 that the decay of the tritium molecule T
2
= 3
H
2
should generate the helium hydride ion [3
HeT]+ with high probability.

In 1963, F. Cacace at the Sapienza University of Rome conceived the decay technique for preparing and studying organic radicals and carbenium ions.[27] In a variant of that technique, the exotic species like the methonium cation are produced by reacting organic compounds with the [3
HeT]+ that is produced by the decay of T
2
that is mixed with the desired reagents. Much of what we know about the chemitry of [HeH]+ came though this technique.[28]

Implications for neutrino mass experiments[edit]

In 1980, V. Lubimov (Lyubimov) at the ITEP laboratory in Moscow claimed to have detected a significant rest mass (30 ± 16) eV for the neutrino, by analyzing the energy spectrum of the β decay of tritium.[29] The claim was disputed, and several other groups set out to check it by studying the decay of molecular tritium T
2
. It was known that some of the energy released by that decay would be diverted to the excitation of the decay products, including [3
HeT]+; and this phenomenon could be a significant source of error in that experiment. This observation motivated numerous efforts to precisely compute the expected energy states of that ion in order to reduce the uncertainty of those measurements.[citation needed] Many have improved the computations since then, and now there is quite good agreement between computed and experimental properties; including for the isotopologues [4
He2
H]+, [3
He1
H]+, and [3
He2
H]+.[2][11]

Spectral predictions and detection[edit]

In 1956, M. Cantwell predicted theoretically that the spectrum of vibrations of that ion should be observable in the infrared; and the spectra of the deuterium and common hydrogen isotopologues ([3
HeD]+ and [3
He1
H]+) should lie closer to visible light and hence easier to observe.[10] The first detection of the spectrum of [4
He1
H]+ was made by D. Tolliver and others in 1979, at wavenumbers between 1700 and 1900 cm−1.[30] In 1982, P. Bernath and T. Amano detected nine infrared lines between 2164 and 3158 waves per cm.[15]

Interstellar space[edit]

HeH+ has long been conjectured since the 1970s to exist in the interstellar medium.[31] Its first detection, in the nebula NGC 7027, was reported in an article published in the journal Nature in April 2019.[32]

Natural occurrence[edit]

From decay of tritium[edit]

The helium hydride ion is formed during the decay of tritium in the molecule HT or tritium molecule T2. Although excited by the recoil from the beta decay, the molecule remains bound together.[33]

Interstellar medium[edit]

It is believed to be the first compound to have formed in the universe,[8] and is of fundamental importance in understanding the chemistry of the early universe.[34] 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.[8] 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.[35]

Several locations have been suggested as possible places HeH+ might be detected. These include cool helium stars,[8] H II regions,[36] and dense planetary nebulae[36] like NGC 7027.[34]

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 kilometres per second (56 mi/s), quantities large enough to detect might be formed. If detected, the emissions from HeH+ would then be useful tracers of the shock.[37]

References[edit]

  1. ^ "hydridohelium(1+) (CHEBI:33688)". Chemical Entities of Biological Interest (ChEBI). European Bioinformatics Institute.
  2. ^ a b c Krzysztof Pachucki and Jacek Komasa (2012): "", Journal of Chemical Physics, volume 137, issue 20, article 204314. doi:10.1063/1.4768169
  3. ^ a b "Hydridohelium (CHEBI:33689)". Chemical Entities of Biological Interest (ChEBI). European Bioinformatics Institute.
  4. ^ a b c d e Hogness, T. R.; Lunn, E. G. (1925). "The Ionization of Hydrogen by Electron Impact as Interpreted by Positive Ray Analysis". Physical Review. 26 (1): 44–55. Bibcode:1925PhRv...26...44H. doi:10.1103/PhysRev.26.44.
  5. ^ Coxon, J.; Hajigeorgiou, P. G. (1999). "Experimental Born–Oppenheimer Potential for the X1Σ+ Ground State of HeH+: Comparison with the Ab Initio Potential". Journal of Molecular Spectroscopy. 193 (2): 306–318. Bibcode:1999JMoSp.193..306C. doi:10.1006/jmsp.1998.7740. PMID 9920707.
  6. ^ Dias, A. M. (1999). "Dipole Moment Calculation to Small Diatomic Molecules: Implementation on a Two-Electron Self-Consistent-Field ab initio Program" (PDF). Rev da Univ de Alfenas. 5 (1): 77–79.
  7. ^ Dey, Bijoy Kr.; Deb, B. M. (April 1999). "Direct ab initio calculation of ground-state electronic energies and densities for atoms and molecules through a time-dependent single hydrodynamical equation". The Journal of Chemical Physics. 110 (13): 6229–6239. doi:10.1063/1.478527.
  8. ^ a b c d 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.
  9. ^ 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.
  10. ^ a b c d Murray Cantwell (1956): "Molecular Excitation in Beta Decay". Physical Reviews, volume 101, issue 6, pages 1747-1756.doi:10.1103/PhysRev.101.1747.
  11. ^ a b c d e Wei-Cheng Tung, Michele Pavanello, and Ludwik Adamowicz (2012): "Accurate potential energy curves for HeH+ isotopologues ". Journal of Chemical Physics, volume 137, issue 16, pages 164305. doi:10.1063/1.4759077
  12. ^ H. M. Schwartz (1955): "Excitation of Molecules in the Beta Decay of a Constituent Atom". Journal of Chemical Physics, volume 23, pages 400-401. doi:10.1063/1.1741982.
  13. ^ Arthur H. Snell, Frances Pleasonton, H. E. Leming (1957): "Molecular dissociation following radioactive decay: Tritium hydride". Journal of Inorganic and Nuclear Chemistry, volume 5, issue 2, pages 112-117. doi:10.1016/0022-1902(57)80051-7
  14. ^ a b c d Kenneth T. Bainbridge (1933): "Comparison of the Masses of H2 and Helium". Physical Reviews, volume 44, issue 1, page 57. doi:10.1103/PhysRev.44.57
  15. ^ a b P. Bernath and T. Amano (1982): "Detection of the Infrared Fundamental Band of HeH+". Physical Review Letters, volume 48, issue 1, pages 20-22. doi:10.1103/PhysRevLett.48.20
  16. ^ Möller, Thomas; Beland, Michael; Zimmerer, Georg (1985). "Observation of Fluorescence of the HeH Molecule". Physical Review Letters. 55 (20): 2145–2148. Bibcode:1985PhRvL..55.2145M. doi:10.1103/PhysRevLett.55.2145. PMID 10032060.
  17. ^ "Wolfgang Ketterle: The Nobel Prize in Physics 2001".
  18. ^ Ketterle, W.; Figger, H.; Walther, H. (1985). "Emission spectra of bound helium hydride". Physical Review Letters. 55 (27): 2941–2944. Bibcode:1985PhRvL..55.2941K. doi:10.1103/PhysRevLett.55.2941. PMID 10032281.
  19. ^ a b c d e f Grandinetti, Felice (October 2004). "Helium chemistry: a survey of the role of the ionic species". International Journal of Mass Spectrometry. 237 (2–3): 243–267. Bibcode:2004IJMSp.237..243G. doi:10.1016/j.ijms.2004.07.012.
  20. ^ Cacace, Fulvio (1970). Gaseous Carbonium Ions from the Decay of Tritiated Molecules. Advances in Physical Organic Chemistry. 8. pp. 79–149. doi:10.1016/S0065-3160(08)60321-4. ISBN 9780120335084.
  21. ^ a b Lias, S. G.; Liebman, J. F.; Levin, R. D. (1984). "Evaluated Gas Phase Basicities and Proton Affinities of Molecules; Heats of Formation of Protonated Molecules". Journal of Physical and Chemical Reference Data. 13 (3): 695. Bibcode:1984JPCRD..13..695L. doi:10.1063/1.555719.
  22. ^ Carrington, Alan; Gammie, David I.; Shaw, Andrew M.; Taylor, Susie M.; Hutson, Jeremy M. (1996). "Observation of a microwave spectrum of the long-range He⋯H+
    2
    complex". Chemical Physics Letters. 260 (3–4): 395–405. Bibcode:1996CPL...260..395C. doi:10.1016/0009-2614(96)00860-3.
  23. ^ Pauzat, F.; Ellinger, Y. (2005). "Where do noble gases hide in space?". In Markwick-Kemper, A. J. (ed.). Astrochemistry: Recent Successes and Current Challenges (PDF). Poster Book IAU Symposium No. 231. 231. Bibcode:2005IAUS..231.....L. Archived from the original (PDF) on 2007-02-02.
  24. ^ J. Y. Beach (1936): "Quantum‐Mechanical Treatment of Helium Hydride Molecule‐Ion HeH+". Journal of Chemical Physics, volume 4, issue 6, pages 353-357. doi:10.1063/1.1749857
  25. ^ Sôroku Toh (1940): "Quantum-Mechanical Treatment of Helium-Hydride Molecule Ion HeH+". Proceedings of the Physico-Mathematical Society of Japan, 3rd Series, volume 22, issue 2, pages 119-126. doi:10.11429/ppmsj1919.22.2_119.
  26. ^ Arthur A. Evett (1956): "Ground State of the Helium‐Hydride Ion". Journal of Chemical Physics, volume 24, issue 1, pages 150-152. doi:10.1063/1.1700818
  27. ^ Fulvio Cacace (1990): "Nuclear Decay Techniques in Ion Chemistry". Science, volume 250, issue 4979, pages 392-399. doi:10.1126/science.250.4979.392.
  28. ^ Maurizio Speranza (1993): "Tritium for generation of carbocations". Chemical Reviews, volume 93, issue 8, pages 2933–2980. doi:10.1021/cr00024a010.
  29. ^ V. A. Lubimov, E. G. Novikov, V. Z. Nozik, E. F. Tretyakov, V. S. Kosik (1980): "An estimate of the νe mass from the β-spectrum of tritium in the valine molecule", Physics Letters B, volume 94, issue 2, pages 266-268. doi:10.1016/0370-2693(80)90873-4.
  30. ^ David E. Tolliver, George A. Kyrala, and William H. Wing (1979): "Observation of the Infrared Spectrum of the Helium-Hydride Molecular Ion [4
    HeH]+". Physical Review Letters, volume 43, issue 23, pages 1719-1722. doi:10.1103/PhysRevLett.43.1719
  31. ^ Fernández, J.; Martín, F. (2007). "Photoionization of the HeH+ molecular ion". Journal of Physics B. 40 (12): 2471–2480. Bibcode:2007JPhB...40.2471F. doi:10.1088/0953-4075/40/12/020.
  32. ^ Stutzki, Jürgen; Risacher, Christophe; Ricken, Oliver; Klein, Bernd; Karl Jacobs; Graf, Urs U.; Menten, Karl M.; Neufeld, David; Wiesemeyer, Helmut (April 2019). "Astrophysical detection of the helium hydride ion HeH+". Nature. 568 (7752): 357. doi:10.1038/s41586-019-1090-x. PMID 30996316.
  33. ^ Mannone, F., ed. (1993). Safety in Tritium Handling Technology. Springer. p. 92. doi:10.1007/978-94-011-1910-8_4. ISBN 978-94-011-1910-8.
  34. ^ a b Liu, X.-W.; Barlow, M. J.; Dalgarno, A.; Tennyson, J.; Lim, T.; Swinyard, B. M.; Cernicharo, J.; Cox, P.; Baluteau, J.-P.; Pequignot, D.; Nguyen, Q. R.; Emery, R. J.; Clegg, P. E. (1997). "An ISO Long Wavelength Spectrometer detection of CH in NGC 7027 and an HeH+ upper limit". Monthly Notices of the Royal Astronomical Society. 290 (4): L71–L75. Bibcode:1997MNRAS.290L..71L. doi:10.1093/mnras/290.4.l71.
  35. ^ 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.
  36. ^ a b 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.
  37. ^ 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.