Polyhydride

A polyhydride or superhydride is a compound that contains an abnormally large amount of hydrogen. This can be described as high hydrogen stoichiometry. Examples include iron pentahydride FeH5, LiH6, and LiH7. The more well known lithium hydride only has one hydrogen atom.[1]

Polyhydrides are only known to be stable under high pressure.[1]

Polyhydrides are important because they can form substances with a very high density of hydrogen. They may resemble the elusive metallic hydrogen, but can be made under lower pressures. One possibility is that they could be superconductors. Hydrogen sulfide under high pressures forms SH3 units, and can be a superconductor at 203 K (−70 °C) and a pressure of 1.5 million atmospheres.[1]

Structures

Unit cell diagram showing the structure of NaH7, which contains H3 complexes. The coloured balls it the isosurface, plotted at the level of 0.07 electrons*Å−3. One of H2 molecules is bonded to a hydrogen atom in the NaH unit with a bond length of 1.25 Å, forming a H3 linear anion.

The polyhydrides of alkaline earth and alkali metals contain cage structures. Also hydrogen may be clustered into H, H3, or H2 units. Polyhydrides of transition metals may have the hydrogen atoms arranged around the metal atom. Computations suggest that increasing hydrogen levels will reduce the dimensionality of the metal arrangement, so that layers form separated by hydrogen sheets.[1] The H3 substructure is linear.[2]

H3+ would form triangular structures in the hypothetical H5Cl.[2]

Compounds

When sodium hydride is compressed with hydrogen NaH3 and NaH7. These are formed at 30 GPa and 2,100 K.[2]

formula name temperature

°C

pressure

GPa

crystal structure space group a Å b c β cell volume formulae per unit cell refs
LiH2 lithium dihydride 27 130 [3]
LiH6 Lithium hexahydride [1]
LiH7 Lithium heptahydride [1]
NaH3 sodium trihydride orthorhombic Cmcm 3.332 Å 6.354 Å 4.142 Å 90 87.69 4 [2]
NaH7 sodium heptahydride monoclinic Cc 6.99 3.597 5.541 69.465 130.5 [2]
CaHx 500 22 double hexagon [4]
CaHx 600 121 [4]
FeH5 iron pentahydride 1200 66 tetragonal I4/mmm [1]
H3Se Selenium trihydride 10 [5]
LaH10 Lanthanum decahydride 1000 170 cubic Fm3m 5.09 5.09 5.09 132 4 [6]
LaH10 Lanthanum decahydride 25 121 Hexagonal R3m 3.67 3.67 8.83 1 [6]
LaH7 Lanthanum heptahydride 25 109 monoclinic C2/m 6.44 3.8 3.69 135 63.9 2 [6]
UH7 Uranium heptahydride 2000 63 fcc P63/mmc [7]
UH8 Uranium octahydride 300 1-55 fcc Fm3m [7]
UH8 Uranium nonahydride 40-55 fcc P63/mmc [7]

Predicted

Using computational chemistry many other polyhydrides are predicted, including LiH8,[8] LiH9,[9] LiH10,[9] CsH3,[10] KH5 RbH5,[11] RbH9,[8] NaH9, BaH6,[11] CaH6,[12] MgH4, MgH12, MgH16,[13] SrH4, SrH6,[14] SrH10, SrH12,[8] ScH4, ScH6, ScH8,[15] YH4 and YH6,[16] YH24, LaH8, LaH10,[17] YH9, LaH11, CeH8, CeH9, CeH10, PrH8, PrH9,[18] ThH6, ThH7 and ThH10,[19] U2H13, UH7, UH8, UH9,[7] AlH5,[20] GaH5, InH5,[8] SnH8, SnH12, SnH14,[21] PbH8,[22] SiH8 (subsequently discovered),[8] GeH8,[23] (although Ge3H11 may be stable instead)[24] AsH8, SbH4,[25] BiH4, BiH5, BiH6,[26] H3Se,[27] H3S,[28] Te2H5, TeH4,[29] PoH4, PoH6,[8] H2F, H3F,[8] H2Cl, H3Cl, H5Cl, H7Cl,[30] H2Br, H3Br, H4Br, H5Br, H5I,[8] XeH2, XeH4,.[31]

Among the transition elements, VH8 in a C2/m structure around 200 Gpa is predicted to have a superconducting transition temperature of 71.4 K. VH5 in a P63/mmm space group has a lower transition temperature.[32]

Properties

Superconduction

Under suitably high pressures polyhydrides may become superconducting. Characteristics of substances that are predicted to have high superconducting temperatures are a high phonon frequency, which will happen for light elements, and strong bonds. Hydrogen is the lightest and so will have the highest frequency of vibration. Even changing the isotope to deuterium will lower the frequency and lower the transition temperature. Compounds with more hydrogen will resemble the predicted metallic hydrogen. However superconductors also tend to be substances with high symmetry, and also need the electrons not to be locked into molecular subunits, and require large numbers of electrons in states near the Fermi level. There should also be electron-phonon coupling which happens when the electric properties are tied to the mechanical position of the hydrogen atoms.[18][33] For example Lithium hexahydride is predicted to lose all electrical resistance below 38 K at a pressure of 150 Gpa. The hypotheical LiH8 has a predicted superconducting transition temperature at 31 K at 200 GPa.[34] MgH6 is predicted to have a Tc of 400 K around 300 Gpa.[35] CaH6 could have a Tc of 260 K at 120 GPa. PH3 doped H3S is also predicted to have a transition temperature above the 203 K measured for H3S (contaminated with solid sulfur).[36] Rare earth and actinide polyhydrides may also have highish transition temperatures, for example ThH10 with Tc = 194 K.[19] UH8, which can be decompressed to room temperature without decomposition, is predicted to have a transition temperature of 193 K.[19] AcH10, if it could be ever made, is predicted to superconduct at temperatures over 204 K, and AcH10 would be similarly conduction under lower pressures (150 GPa).[37]

H3Se actually is a van der Waals solid with formula 2H2Se•H2 with a measured Tc of 105K under a pressure of 135 GPa.[5]

References

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