Quantum Simulations Reveal That Hydrogen Bonds Persist in Supercritical Water
Astronomy

Quantum Simulations Reveal That Hydrogen Bonds Persist in Supercritical Water

Physicists use quantum molecular dynamics to settle a decades-long debate over whether water molecules stay connected under extreme conditions.

By John Williams
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Quantum Simulations Reveal That Hydrogen Bonds Persist in Supercritical Water
Partial pair distribution function g HO (r) of 1,000 K water at various densities. Coordination numbers at r 0 = 2.1 Å marked on top of blue arrows. Nitish Baradwaj et al. / The journal of physical chemistry letters

Water is arguably the most anomalous liquid on Earth, boasting an unusually high boiling point and a complex local tetrahedral organization that dictates everything from its maximum density at four degrees Celsius to its exceptional heat capacity. At the heart of this macroscopic behavior lies the intermolecular hydrogen bond and the intricate three-dimensional network it forms between individual molecules. Yet, when water is heated and pressurized beyond its critical point, entering the supercritical regime, its familiar identity undergoes a radical transformation. Researchers have long sought to understand what happens to these delicate atomic connections in supercritical water (SCW), a state of matter prized for its ability to dissolve organic pollutants, catalyze green chemical reactions, and serve as an advanced heat-transfer medium.

The core scientific debate has centered on whether hydrogen bonds survive in this harsh environment. Early interpretations of neutron diffraction measurements suggested that hydrogen bonding was virtually nonexistent in supercritical water, pointing to a severe structural breakdown. However, subsequent experimental reinterpretations and proton nuclear magnetic resonance studies argued that appreciable hydrogen bonding might still endure at extreme temperatures and pressures. Complicating matters further, X-ray Raman spectroscopy revealed a spatially heterogeneous picture, suggesting the existence of tiny, isolated hydrogen-bonded patches drifting within a sea of non-bonded molecules. These conflicting conclusions arose largely because traditional analytical methods relied on time-averaged pair distribution functions and geometric distance cutoffs that struggle to decouple overlapping atomic signals under extreme thermodynamic stress.

To cut through this methodological ambiguity, the research team published in The Journal of Physical Chemistry Letters a comprehensive computational investigation utilizing quantum molecular dynamics (QMD) simulations combined with density functional theory. The scientists employed the strongly constrained and appropriately normed (SCAN) meta-generalized gradient approximation functional to accurately model exchange and correlation effects. Beginning with a relaxed bulk water configuration containing one hundred eight molecules at room temperature, the system was heated to one thousand Kelvin and systematically stepped down across ten different densities ranging from 0.1 to 1.0 grams per cubic centimeter.

1: (a) g N (r), which is the neutron weighted pair distribution function obtained from neutron experiments (blue dots), Soper et al. (“A. K. Soper, International Scholarly Research Notices, Vol. 2013, Issue 1, Jan 2013; licensed under a Creative Commons Attribution (CC BY) license.”) and g N (r) from QMD simulations of water at 300 K is computed using a deuterium neutron cross section (black line) and (b) experimental g N (r) for SCW at a density of 0.7 g/cm3 obtained from Bernabei et al. (Reproduced with permission from Physical Review E 78, 021505 August 28 2008 Copyright 2008, American Physical Society) and at a temperature of 673 K (blue dots) and from QMD simulations of SCW water is computed using deuterium neutron cross section (red line). Partial pair distribution functions (PDFs), g αβ(r), for water at ambient conditions (ρ0 = 1.0, 300 K) compared with supercritical water at ρ0 = 0.75, 673 K. Panels (c) and (d) show the partial PDF for H–O and H–H, respectively. Total PDFs are sho
(a) g N (r), which is the neutron weighted pair distribution function obtained from neutron experiments (blue dots), Soper et al. (“A. K. Soper, International Scholarly Research Notices, Vol. 2013, Issue 1, Jan 2013; licensed under a Creative Commons Attribution (CC BY) license.”) and g N (r) from QMD simulations of water at 300 K is computed using a deuterium neutron cross section (black line) and (b) experimental g N (r) for SCW at a density of 0.7 g/cm3 obtained from Bernabei et al. (Reproduced with permission from Physical Review E 78, 021505 August 28 2008 Copyright 2008, American Physical Society) and at a temperature of 673 K (blue dots) and from QMD simulations of SCW water is computed using deuterium neutron cross section (red line). Partial pair distribution functions (PDFs), g αβ(r), for water at ambient conditions (ρ0 = 1.0, 300 K) compared with supercritical water at ρ0 = 0.75, 673 K. Panels (c) and (d) show the partial PDF for H–O and H–H, respectively. Total PDFs are sho Credit: Nitish Baradwaj et al. / The journal of physical chemistry letters

Probing Electronic Overlap Under Extreme Conditions

A major breakthrough of this study was the introduction of a first-principles framework based on electronic charge-density overlap to define and identify hydrogen bonds. In standard radial distribution functions, the peak corresponding to intermolecular hydrogen-bonding heavily overlaps with intramolecular hydrogen-hydrogen correlations, masking true structural changes. By directly probing the underlying quantum mechanical electron charge densities, the authors established a robust electronic overlap criterion that remains reliable even when thermal agitation severely perturbs molecular geometry.

The analysis revealed that while the covalent oxygen-hydrogen bonds holding individual water molecules together remain remarkably robust and intact across all tested supercritical states, the intermediate-range structure suffers profound broadening. At an isosurface threshold corresponding to a separation of approximately 2.03 angstroms, the simulations showed that electronic charge-density regions touch to form a valid hydrogen bond. Setting a stringent cutoff at 2.10 angstroms where the overlap drops significantly below standard thresholds, the researchers mapped out the exact population and behavior of surviving bonds.

Lifetimes and Density-Driven Distortions

The results demonstrate that a reduced level of residual hydrogen bonding stubbornly persists across the entire explored envelope of supercritical water. At a density of 1.0 grams per cubic centimeter and one thousand Kelvin, the average number of hydrogen bonds per water molecule drops from 3.6 in ambient liquid water down to 1.62. As the density is further reduced toward gas-like conditions at 0.1 grams per cubic centimeter, the average number of hydrogen bonds per molecule falls further to 0.29.

2: Electronic charge-density distributions in hexagonal ice and supercritical water (SCW). (a) A tetrahedrally hydrogen-bonded H2O molecule in hexagonal ice. Each water molecule participates in four hydrogen bonds with the corresponding distances marked by solid lines. (b) Local molecular environment in SCW at 1.0 g/cm3, showing three water molecules extracted from a 108-molecule QMD configuration. Three intermolecular H--O separations are indicated two by solid lines. Charge-density overlap identifies a hydrogen bond at 1.65 Å, while 2.10 Å marks the limiting distance under this criterion. No overlap occurs at 2.13 Å, indicating the absence of a hydrogen bond. (c) Four water molecules from an SCW configuration at 0.7 g/cm3. Charge-density overlap identifies hydrogen bonds at 1.77 and 1.96 Å, whose distances are marked by solid lines. The absence of overlap at 2.61 Å indicates no hydrogen bond at this separation. In panels (b) and (c), each water molecule has two intramolecular O–H covale
Electronic charge-density distributions in hexagonal ice and supercritical water (SCW). (a) A tetrahedrally hydrogen-bonded H2O molecule in hexagonal ice. Each water molecule participates in four hydrogen bonds with the corresponding distances marked by solid lines. (b) Local molecular environment in SCW at 1.0 g/cm3, showing three water molecules extracted from a 108-molecule QMD configuration. Three intermolecular H--O separations are indicated two by solid lines. Charge-density overlap identifies a hydrogen bond at 1.65 Å, while 2.10 Å marks the limiting distance under this criterion. No overlap occurs at 2.13 Å, indicating the absence of a hydrogen bond. (c) Four water molecules from an SCW configuration at 0.7 g/cm3. Charge-density overlap identifies hydrogen bonds at 1.77 and 1.96 Å, whose distances are marked by solid lines. The absence of overlap at 2.61 Å indicates no hydrogen bond at this separation. In panels (b) and (c), each water molecule has two intramolecular O–H covale Credit: Nitish Baradwaj et al. / The journal of physical chemistry letters

Furthermore, evaluating population time correlation functions allowed the team to calculate hydrogen bond lifetimes in supercritical water. While room-temperature water exhibits a relatively stable hydrogen bond lifetime of about 1.43 picoseconds, the extreme thermal motion at one thousand Kelvin causes these bonds to break and reform at astonishing speeds, with lifetimes plunging to between 0.04 and 0.09 picoseconds depending on the fluid density. These ultra-short lifetimes highlight just how transient and fleeting intermolecular connections become in the supercritical regime.

Ultimately, this quantum mechanical investigation reconciles decades of contradictory experimental interpretations by providing a unified picture of supercritical water. By proving that weak, highly dynamic hydrogen bonds survive even in highly expanded supercritical fluids, the work supplies foundational data that will aid scientists in designing better machine-learned force fields, optimizing industrial hydrothermal oxidation processes, and understanding planetary interiors where supercritical fluids play a critical geochemical role.

The research was published in The journal of physical chemistry letters on October 15, 2026.

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Reference(s)

  1. Baradwaj, Nitish., et al. “Hydrogen Bonding in Supercritical Water Using Quantum Molecular Dynamics.” The Journal of Physical Chemistry Letters, vol. 17, no. 41, September 29, 2026, pp. 11760-11768. American Chemical Society (ACS), doi: 10.1021/acs.jpclett.6c02526. <https://doi.org/10.1021/acs.jpclett.6c02526>.

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Williams, John. “Quantum Simulations Reveal That Hydrogen Bonds Persist in Supercritical Water.” BioScience. BioScience ISSN 2521-5760, 26 October 2026. <https://www.bioscience.com.pk/en/subject/astronomy/hydrogen-bonding-in-supercritical-water-using-quantum-molecular-dynamics>. Williams, J. (2026, October 26). “Quantum Simulations Reveal That Hydrogen Bonds Persist in Supercritical Water.” BioScience. ISSN 2521-5760. Retrieved October 26, 2026 from https://www.bioscience.com.pk/en/subject/astronomy/hydrogen-bonding-in-supercritical-water-using-quantum-molecular-dynamics Williams, John. “Quantum Simulations Reveal That Hydrogen Bonds Persist in Supercritical Water.” BioScience. ISSN 2521-5760. https://www.bioscience.com.pk/en/subject/astronomy/hydrogen-bonding-in-supercritical-water-using-quantum-molecular-dynamics (accessed October 26, 2026).
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