Imaging Reveals Delayed HDO Formation at Water Interface

Wide-field infrared spectra from a flowing flat jet track H₂O, D₂O, and HDO over the first 100 microseconds.

Editorial Desk·July 13, 2026·4 min readstrong

Underlying Paper

Non-equilibrium state during proton-deuteron exchange at a liquid-liquid interface

Proton-deuteron exchange is a very fast process, even across macroscopic length scales. Here we directly and quantitatively measure the formation of HDO within the first 100 microseconds of the reaction at the liquid-liquid interface between D$_2$O and H$_2$O, using a fast-flowing liquid flat jet combined with infrared spectroscopic imaging. We demonstrate that, at early stages HDO formation is reaction-limited, set by the low concentration of the hydroxide and hydronium ions that mediate the exchange. As the ion concentration rises, the rate rapidly approaches the diffusion limit. The reaction rate constant we extract is consistent with the picosecond timescale of the elementary proton-deuteron exchange. Access to these microsecond kinetics reveals a non-equilibrium state in the early H$_2$O/D$_2$O interface: the two liquids are fully mixed by diffusion, yet the HDO concentration remains well below equilibrium. Quantitative imaging of reactant and product concentrations at well-defined liquid-liquid interfaces, as introduced here, will enable the study of fast kinetics across a wide range of chemical reactions.

arXiv:2509.17724Submitted: Jul 13, 2026v2

Proton-deuteron exchange in water is often treated as effectively immediate once H₂O and D₂O meet, because the elementary proton-transfer steps occur on picosecond timescales. This paper tests that assumption at a well-defined liquid-liquid interface rather than in a premixed sample. The authors use two impinging cylindrical microjets to form a fast-flowing liquid sheet with an H₂O/D₂O interface, then image wavelength-tunable infrared transmission across the sheet as the interface moves downstream in time.

The result is a direct concentration movie of H₂O, D₂O, and HDO during the first 100 microseconds of contact. The central finding is that the early interface can be diffusively mixed while still chemically out of equilibrium: H₂O and D₂O have overlapped, but the HDO concentration remains below the local equilibrium value.

Core Contribution

The contribution is not a new exchange mechanism. It is a measurement that separates molecular mixing from isotopic equilibration on microsecond length and time scales. The experiment reads out chemically specific vibrational bands: the H-O-H bend near 1640 cm⁻¹, the D-O-D bend near 1210 cm⁻¹, and the H-O-D bend near 1450 cm⁻¹. By fitting each local spectrum as a linear combination of reference spectra, the authors convert infrared images into optical thicknesses for the reactants and product.

Figure 1 shows the experimental idea and why the spectroscopy is sufficient for quantification: the three bending bands are separated enough to follow HDO formation without relying on an indirect proxy.

Figure 1. Spatio-spectral imaging of proton-deuteron exchange at a liquid-liquid interface. (A) Schematic of the experiment. Two impinging cylindrical microjets of H_2O and D_2O form a LS with a liquid-liquid interface. The inset schematically shows a cross-section of the H_2O (green) - D_2O (blue) LS as it evolves downstream, which leads to the gradual formation of HDO in the diffusively mixed region (turquoise) at the interface. The transmission of a narrowband and wavelength-tunable IR-FEL beam through the LS is imaged with an IR camera. (B) Transmission image T(y,z) for an H_2O/D_2O LS at the H-O-H bending vibration (_IR=1640 cm^-1). (C) Optical density -_10(T) spectra extracted from three locations of the LS in B) marked by circles. The H-O-H and D-O-D bending vibrations of H_2O and D_2O, as well as the H-O-D bending vibration of HDO are well separated and allow for a quantitative analysis of the proton-deuteron exchange. (D) Reference spectra of pre-mixed solutions of H_2O (green), D_2O (blue), and a 50:50 mix of H_2O:D_2O (magenta).

Technical Approach

The time axis comes from flow, not from repeated pump-probe delay scans. As the liquid sheet travels downstream, positions along the sheet correspond to later reaction times. The paper bins regions at the interface and extracts spectra with 10 µs time resolution. That design matters because it lets the authors compare pure H₂O/D₂O exchange with acid- or base-doped cases under the same imaging geometry.

Figure 2 is the key measurement. In pure H₂O/D₂O, the HDO band grows gradually as the interface evolves. In a 10⁻² M HCl/D₂O liquid sheet, the HDO signal rises much faster. The interpretation is chemical rather than geometric: increasing the available hydronium or hydroxide concentration accelerates the proton-deuteron exchange until it approaches the diffusion-limited case.

Figure 2. Temporal evolution of the infrared absorption spectra of the H_2O/D_2O interface. (A) Optical density image of H_2O/D_2O LS at _IR=1640 cm^-1 with binned areas (colored boxes) that are used to extract IR spectra from averaging over all pixels in each area corresponding to different times of the reaction, with 10 µs time resolution. (B) Average IR spectra from binned areas in A) recorded at the H_2O/D_2O interface. Besides the vibrational modes of H_2O (1640 cm^-1) and D_2O (1210 cm^-1) the band of HDO (1450 cm^-1) is evolving with reaction time. The lines show fits to the measured data points (symbols) using a linear combination of reference spectra (Methods), where the colors refer to the bins in A). (C) Same as B) but for a 10^-2 M HCl/D_2O LS, which leads to an accelerated formation of HDO. (D) Optical thickness of H_2O (green) and D_2O (blue) and (E) of HDO as a function of time. Full symbols refer to the H_2O/D_2O LS in B), and empty symbols to the HCl/D_2O interface in C).

The analysis then couples the concentration maps to reaction-diffusion simulations. In the fast model, the local HDO concentration is assumed to reach equilibrium wherever H₂O and D₂O mix. In the slow model, the HDO formation rate is finite and constrained by the available ions that mediate exchange. The fitted diffusion coefficient is taken from the acid/base case, where the exchange is too fast for the apparatus to resolve, and the pure-water case is used to fit the rate constant.

Results and Analysis

The strongest evidence is the contrast between the pure and doped interfaces. The pure H₂O/D₂O system shows a delayed HDO buildup over the first 100 µs, while 10⁻² M acid or base drives the system close to the fast-equilibration limit. That comparison supports the authors' claim that the early pure-water interface is reaction-limited despite the fast elementary proton-transfer step.

Figure 3 makes the physical picture explicit. The fast model reaches local equilibrium concentrations, with 27.5 M corresponding to the 1:1:2 H₂O:D₂O:HDO composition. The slow model stays below that equilibrium line at early times, even though diffusion has already brought the isotopic liquids into contact. This is the paper's most useful distinction: diffusion can erase the spatial separation of the two liquids before the isotope-exchange chemistry catches up.

Figure 3. Non-equilibrium state at the liquid-liquid interface. (A) Average concentration of HDO in the bottom half of the LS (see inset) as function of available hydroxide and hydronium ions, using D_2O/(acidic/basic H_2O) (dots) and (acidic/basic D_2O)/(acidic/basic H_2O) (triangles), see legend. (B--D) Conceptual illustration of the three scenarios of the evolution of the H2O/D2O interface: (B) (hypothetical) no HDO formation, mixing only, (C) intermediate rate of HDO formation leading to a non-equilibrium state, and (D) very fast HDO formation resulting in a local equilibrium. (E) Concentration of HDO as a function of reaction time. The solid lines represent the simulated dynamics, based on integrating (along x) the concentration distributions as shown in F,G). The limited availability of ions causes severe slowing down of the dynamics for the pure H_2O/D_2O system (crimson curve), compared to fast model with higher ion concentration (light blue curve). (F,G) Simulated distribution of H_2O, D_2O, and HDO as a function of time and distance from the liquid-liquid interface, with parameters fitted to reproduce the experimental data in E). (F) Fast model: Assuming near-instantaneous HDO formation results in a local equilibrium concentration at each position of the evolving interface, cf. sub-panel D). (G) Slow model: In the case of H_2O and D_2O, the local equilibrium concentration of HDO is not yet reached, cf. sub-panel C). (H,I) HDO concentrations at an early (dotted line) and late (dashed line) time. The fast model (H) results in local equilibrium concentration of HDO at any stage where 27.5 M corresponds to 1:1:2 H2O:D2O:HDO. For the slow model (I), the HDO concentrations stay below the equilibrium values. (J) Ternary color-scale for F,G) of the non-equilibrium part of the H2O/D2O system, where the light-blue dashed-dotted line marks the HDO equilibrium concentrations as observed for the fast model in H), while red lines indicate the mixture after 25 and 100 µs as predicted by the slow model.

The evidence is convincing for the specific geometry and chemistry tested. The paper combines spatially resolved spectra, reference-based decomposition, acid/base perturbations, and reaction-diffusion modeling rather than inferring kinetics from a single bulk observable. The extracted rate constant is reported as consistent with picosecond elementary exchange, so the apparent microsecond delay is not a contradiction; it reflects the limited concentration of hydronium and hydroxide ions needed to mediate exchange at the interface.

Caveats in Practice

The measurement depends on converting optical density into concentration through reference spectra and a thickness model for the liquid sheet. The paper addresses this with calibration spectra, thickness measurements, and fits, but those steps still make the quantitative rate extraction model-dependent. The study also focuses on H₂O/D₂O and acid/base variants; its broader claim is best read as a demonstration of a measurement platform for fast liquid-liquid interfacial reactions, not as proof that all such reactions will show the same non-equilibrium delay.

Evidence Box

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Key Claims

  • H₂O/D₂O interfaces can be diffusively mixed before reaching isotopic equilibrium
  • Early HDO formation is limited by available hydronium and hydroxide ions
  • Added acid or base moves the reaction toward the diffusion-limited regime
  • Flat-jet infrared imaging can quantify fast interfacial reaction kinetics

Key Results

  • HDO formation measured within the first 100 µs of H₂O/D₂O contact
  • Spectra extracted with 10 µs time resolution along the flowing liquid sheet
  • H₂O, D₂O, and HDO bands separated at 1640 cm⁻¹, 1210 cm⁻¹, and 1450 cm⁻¹
  • 10⁻² M HCl or NaOH accelerates HDO formation relative to pure H₂O/D₂O

Limitations & Caveats

  • Rate extraction depends on reference-spectrum fitting and liquid-sheet thickness calibration
  • Pure-water kinetics are inferred with the diffusion coefficient fixed from the fast acid/base model
  • Evaluation is limited to H₂O/D₂O exchange and acid/base perturbations
  • The fastest acid/base exchange is treated as too fast to resolve directly with this setup

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Readers are encouraged to consult the original arXiv paper for complete details. SOTA Papers does not make claims beyond what is supported by the authors' reported evidence.