Understanding high pressure molecular hydrogen with a hierarchical machine-learned potential
Hongxiang Zong1,2, Heather Wiebe3, Graeme J Ackland4
1Centre for Science at Extreme Conditions and School of Physics and Astronomy, University of Edinburgh, Edinburgh, EH9 3ET, UK. zonghust@mail.xjtu.edu.cn.
Nature Communications
|October 7, 2020
Summary
A new computational model explains unusual features in the hydrogen phase diagram, revealing insights into molecular hydrogen phases and high-pressure behavior. This model clarifies why liquid hydrogen is denser than solid hydrogen at extreme pressures.
Area of Science:
- Condensed matter physics
- Computational materials science
- Quantum chemistry
Background:
- Density functional calculations accurately model hydrogen phases but lack physical insight.
- Unusual features in the hydrogen phase diagram require further explanation.
Purpose of the Study:
- Develop a fast interatomic potential for molecular hydrogen.
- Provide physical insights into the observed phases and properties of hydrogen.
Main Methods:
- Development of a novel, fast interatomic potential for H2.
- Simulations reproducing orientationally disordered Phase I, broken-symmetry Phase II, and reentrant melt curve.
Main Results:
- The potential accurately reproduces key molecular hydrogen phases and the reentrant melt curve.
- High-pressure vibrational frequency drop is due to intermolecular coupling, not bond weakening.
- Liquid H2's higher density is attributed to a switch in favored molecular orientation (steric repulsion over quadrupole energy).
- Negative thermal expansion and hindered rotation in Phase I are explained by steric effects and frustration.
Conclusions:
- The new potential offers physical insights into hydrogen's complex phase behavior.
- Molecular orientation and steric repulsion are key factors governing high-pressure hydrogen properties.
- High-pressure Phase I of hydrogen is not a molecular rotor phase.
Related Concept Videos
Hydrogen Bonds
12.5K
A hydrogen bond is formed when a weakly positive hydrogen atom already bonded to one electronegative atom (for example, the oxygen in the water molecule) is attracted to another electronegative atom from another polar molecule, such as water (H2O), hydrogen fluoride (HF), or ammonia (NH3). The huge electronegativity difference between the H atom (2.1) and the atom to which it is bonded (4.0 for an F atom, 3.5 for an O atom, or 3.0 for an N atom), combined with the very small size of an H atom...
12.5K
Hydrogen Bonds
129.1K
Hydrogen bonds are weak attractions between atoms that have formed other chemical bonds. One of these atoms is electronegative, like oxygen, and has a partial negative charge. The other is a hydrogen atom that has bonded with another electronegative atom and has a partial positive charge.
Hydrogen Bonds Control the World!
Because hydrogen has very weak electronegativity when it binds with a strongly electronegative atom, such as oxygen or nitrogen, electrons in the bond are unequally shared....
Hydrogen Bonds Control the World!
Because hydrogen has very weak electronegativity when it binds with a strongly electronegative atom, such as oxygen or nitrogen, electrons in the bond are unequally shared....
129.1K
High-Resolution Mass Spectrometry (HRMS)
2.1K
The resolution of a mass spectrometer depends on the efficiency of separating ions with different ion masses. The mass of an atom is approximated to the sum of the masses of protons and neutrons inside, considering the masses of protons and neutrons as equal. However, the masses of the proton (1.6726 × 10−24 g) and neutron (1.6749 × 10−24 g) are not truly equal. There is a minor error in the expression of atomic masses relative to the simplest atom of hydrogen. For...
2.1K
Molecular Orbital Theory II
25.5K
Molecular Orbital Energy Diagrams
25.5K
IR Spectrum Peak Broadening: Hydrogen Bonding
1.5K
The vibrational frequency of a bond is directly proportional to its bond strength. As a result, stronger bonds vibrate at higher frequencies, while weaker bonds vibrate at lower frequencies. The stretching vibration of the strong O–H bond in alcohols and phenols (very dilute solution or gas phase) appears as a sharp peak at 3600–3650 cm−1.
However, the extent of hydrogen bonding influences the observed stretching frequency and band broadening. Intermolecular or intramolecular...
However, the extent of hydrogen bonding influences the observed stretching frequency and band broadening. Intermolecular or intramolecular...
1.5K
Predicting Molecular Geometry
43.2K
VSEPR Theory for Determination of Electron Pair Geometries
43.2K


