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REVIEW 3 major objections 4 minor 91 references

Zero-point vibrational corrections move mercury NMR and EFG calculations closer to experiment

Reviewed by Pith at T0; open to challenge. T0 means a machine referee read the full paper against a public rubric. the ladder, T0–T4 →

The Dalton Project's vibrational averaging module now works with ADF to compute ZORA-level vibrational corrections to EFG, NMR shielding, and spin-spin coupling constants, improving agreement with experiment for mercury compounds.

T0 review reviewed 2026-08-04 challenge →

load-bearing objection Useful, honest software-extension study: ZORA/ADF vibrational corrections work and improve mercury property agreement with experiment; main caveat is the untested transferability of the step length. the 3 major comments →

arxiv 2509.12412 v1 pith:L2CSIWKI submitted 2025-09-15 physics.chem-ph

Vibrational corrections to molecular properties including relativistic corrections at the level of the Zeroth-Order Regular Approximation

classification physics.chem-ph
keywords vibrational correctionszero-point averagingZORArelativistic effectselectric field gradientNMR shieldingspin-spin coupling constantsmercury compounds
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved

The pith

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The reading

The paper extends a vibrational averaging module to work with a quantum chemistry program that supports ZORA relativistic calculations, making it possible to compute zero-point vibrational corrections to molecular properties for heavy-element systems. For a series of mercury compounds, it applies this to the electric field gradient tensor, NMR isotropic shielding, and spin-spin coupling constants. The central claim is that including these vibrational corrections improves agreement with experimental values, and that the size of the correction depends on the level of relativity and the basis set. A distinct practical finding is that the standard numerical step length used for light molecules is too small for mercury systems; a step length of 0.50 reduced normal coordinates is needed.

Core claim

The authors report that extending the vibrational averaging module to work with the Amsterdam Density Functional (ADF) program enables zero-point vibrational corrections to EFG, isotropic shielding, and SSCC with ZORA relativistic treatment. Comparing equilibrium-geometry values and vibrationally corrected values to experiment for mercury halides and methylmercury halides, they find the corrected values are closest to experiment for all three properties. They also find that including scalar and spin-orbit ZORA relativity changes the magnitude of the corrections, and that the correction changes with basis set. A step-length analysis on HgCl2 showed the default 0.05 step length is inadequate,

What carries the argument

The central object is the VPT2 correction formula for zero-point vibrational corrections, evaluated with numerically differentiated property surfaces from a five-point stencil. The module drives the property calculations at the ZORA level, and for the EFG tensor it adds the correction tensor to the equilibrium tensor before diagonalization. The step-length choice of 0.50 reduced normal coordinates is the practical mechanism that makes the numerical derivatives stable for mercury-containing molecules.

Load-bearing premise

The step length of 0.50 reduced normal coordinates, chosen on HgCl2, is assumed adequate for all other mercury compounds compared with experiment, despite the authors' note that other complexes may need a different step length.

What would settle it

Repeat the vibrational averaging for HgI2 or methylmercury iodide using step lengths 0.25 and 0.75 and compare the corrected EFG, shielding, and SSCC values; if they change substantially relative to the claimed accuracy, the fixed step length is not transferable.

Watch this falsifier. Get emailed when new claim-graph text bears on it.

If this is right

  • Zero-point vibrational corrections can now be computed for properties of heavy-element systems at the ZORA level, so benchmark comparisons can move beyond fixed-geometry values.
  • For mercury compounds, vibrationally corrected EFG, shielding, and SSCC values lie closer to experiment than equilibrium-geometry values, reducing mean absolute deviations.
  • The magnitude of the correction depends sensitively on spin-orbit ZORA for mercury, so scalar or non-relativistic corrections alone can be misleading.
  • Basis set choice affects the correction; mixed basis sets (TZP for the Hessian, QZ4P for properties) closely reproduce QZ4P results, while DZ is poor.
  • A step length of 0.50 in reduced normal coordinates is needed for mercury compounds; the default 0.05 is too small.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The fixed step length of 0.50 was calibrated on HgCl2; transferring it to other mercury or heavy-element systems without rechecking could introduce step-length error, and a per-molecule calibration or a direct relationship between step length and bond length would strengthen the method.
  • Because the experiments were performed at nonzero temperature while the corrections are zero-point only, further improvement might come from thermal vibrational corrections, especially for bond-length-sensitive EFG.
  • The same module could be applied to other heavy NMR nuclei (e.g., cadmium) or to mercury-containing biomolecules, provided the convergence issues and linear dependencies described in the paper are handled.
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Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit.

Referee Report

3 major / 4 minor

Summary. The paper reports an extension of the Dalton Project's vibrational averaging module to the ADF program, enabling zero-point vibrational corrections to be computed for electric field gradients, NMR isotropic shielding constants, and spin-spin coupling constants at the ZORA level of relativity. Using VPT2 (Eq. 3) with numerical differentiation (Eqs. 8-9), the authors apply the method to a series of mercury and cadmium compounds and examine the dependence of the corrections on basis set and on the level of relativistic treatment (non-relativistic, scalar ZORA, spin-orbit ZORA). They find that the vibrational corrections generally improve agreement with experiment, reporting mean absolute deviations for EFG ratios, 199Hg chemical shifts, and 1J/2J SSCCs that decrease when vibrational corrections are added. The central claim is that, for all three properties, vibrationally corrected values perform closest to experimental values.

Significance. If the result holds, this is a useful and timely methodological contribution: it brings a well-established vibrational averaging tool (Dalton Project) to a widely used relativistic DFT package (ADF/ZORA), making zero-point corrections available for heavy-element NMR and EFG properties. The demonstration of consistent MAD reductions across three distinct properties is a concrete step beyond previous 4-component treatments (Ref. 64). The paper also provides useful data on how the corrections vary with basis set and with the level of relativity. The main limitations are the small test set, the unquantified uncertainty of the MAD improvements, and the transferability of the numerical step length; these temper the strength of the quantitative claims.

major comments (3)
  1. [V.A, V.D, Eqs. (8)-(9)] The step length h=0.50 is calibrated for HgCl2 at ZORA/BHandHLYP/QZ4P (Section V.A) and then applied to all molecules, functionals, and basis sets in the experimental comparisons (Section V.D, including PBE0 and QZ4P-J). The authors themselves state: 'For another complexs [sic], the step length may need to be adjusted' (V.A). Since Eq. (3) depends on derivatives evaluated with Eqs. (8)-(9), an inappropriate h would change the reported corrections and hence the MAD improvements (e.g., 486 to 290 ppm for shifts; 202 to 169 Hz for SSCC). Please provide at least a sensitivity analysis of h for a representative heavier system per property (e.g., HgI2 or MeHgI), or a per-functional/reference-set validation, to support the fixed h=0.50 used throughout V.D.
  2. [V.C and Conclusion] The conclusion that 'it is necessary to include spin-orbit relativistic effects in the vibrational averaging' is not supported by the data as presented. V.C shows that corrections vary with the relativity level, but all experimental comparisons in V.D are performed at spin-orbit ZORA only; there is no benchmark against experiment at non-relativistic or scalar ZORA levels. Variation of corrections with method does not demonstrate that the spin-orbit values are more accurate. A concrete fix is to compute equilibrium and vibrationally corrected values at all three relativity levels for a subset of the experimental set and compare their MADs; alternatively, the wording should be softened to a statement about the dependence of the corrections on the relativity level.
  3. [V.D, Tables S16-S19] The central claim that vibrational corrections improve agreement with experiment is based on mean absolute deviations over very small samples: 4 EFG ratios, 6 chemical shifts, and 6 SSCCs. No uncertainty estimates, error bars (except for some EFG ratios), or significance tests are reported. For instance, the chemical-shift MAD drops from 486 to 290 ppm, but individual deviations are not shown against experimental error, so the reader cannot judge whether the improvement is systematic or driven by one or two outliers. Please report per-system deviations with experimental uncertainties and a simple significance measure (e.g., paired deviations, leave-one-out MAD, or bootstrap confidence intervals) to support the claim that the corrections perform 'closest to experimental values.'
minor comments (4)
  1. [V.A] Typographical errors: 'For another complexs' should be 'For other complexes'; 'the the EFG tensor' is a doubled article. Also, the sentence 'It was simply too small' after 'a step length of 0.05' reads as colloquial; consider rephrasing.
  2. [Fig. 7] The right-hand panel is described as 'deviations from the ratio of the experimental values,' but the axis labels and units are not stated in the caption. Please specify the axis (e.g., absolute deviation in Vzz ratio) and clarify which ratios are included in the MAD.
  3. [IV.D] The statement that solvent effects are excluded is clear, but it may be worth giving one sentence on the expected direction of solvent-induced shifts for the experimental comparisons (solid-state and liquid-crystal data), since the authors already note this in V.D.2 for the mercury halides.
  4. [II and IV] The basis set nomenclature is inconsistent: some places use 'QZ4P-J' and others 'QZ4P(-J)'. Please use a single convention throughout, ideally with a definition at first use.

Circularity Check

0 steps flagged

No significant circularity: vibrational corrections are benchmarked against external experimental data; the step-length choice is a numerical-convergence parameter, not a fit to the target observables.

full rationale

The paper's central claim is that zero-point vibrational corrections, computed with the extended Dalton/ADF vibrational-averaging module, bring calculated EFG ratios, isotropic shielding-derived chemical shifts, and SSCCs closer to experimental values. These comparisons are made against independent experimental data (PAC quadrupole coupling ratios, solid-state and liquid-crystal 199Hg NMR shifts, and experimental SSCCs), and no parameter is fitted to those target values. The step length h = 0.50 in reduced normal coordinates is chosen in Section V.A from a 17-point step-length analysis on HgCl2 at ZORA/BHandHLYP/QZ4P, comparing numerical derivatives against a 61-point polynomial fit for the same property surfaces. This is a numerical accuracy check, not a calibration to experimental properties. The authors explicitly caution that 'For another complexs, the step length may need to be adjusted' (V.A), so the transfer of h to other molecules is an acknowledged approximation rather than a hidden circular input. Self-citations appear (e.g., refs. 22–24 for ZORA adequacy for mercury EFG/shielding, and ref. 59 for the original Dalton vibrational-averaging module), but these support method choices and prior implementation details; the conclusion that vibrational corrections improve agreement with experiment is established by the paper's own external benchmark comparisons. No equation in the paper reduces a predicted quantity to a fitted input by construction, and no self-citation is used to forbid alternatives or to import a uniqueness result. Thus there is no material circularity; any residual concern about transferability of the step length is a robustness/correctness issue, not circularity.

Axiom & Free-Parameter Ledger

1 free parameters · 5 axioms · 0 invented entities

The paper introduces no new physical entities. The only tuned numerical parameter is the differentiation step length. The computations rest on standard approximate quantum chemistry: VPT2, ZORA, DFT, and numerical differentiation, all with assumptions about transferability and accuracy.

free parameters (1)
  • Numerical differentiation step length h = 0.50 (reduced normal coordinates)
    Chosen via a 17-step-length analysis on HgCl2 to balance numerical noise against anharmonic contamination (Section V.A); not fitted to experimental data, but assumed transferable to all other molecules in the study without per-system re-optimization.
axioms (5)
  • standard math VPT2 zero-point vibrational correction formula (Eq. 3) is adequate for these mercury compounds
    The correction relies on harmonic frequencies and cubic force constants from numerical derivatives; large-amplitude or very anharmonic modes could violate the perturbative assumption (Sections II, V.A).
  • domain assumption ZORA provides a sufficiently accurate relativistic treatment for Hg(II) compounds
    The paper relies on prior validation that ZORA is adequate compared with 4-component methods for EFG and NMR parameters of mercury compounds (citations 22-24).
  • domain assumption The chosen DFT functionals (BHandHLYP for EFG, PBE0 for shielding and SSCC) and basis sets (QZ4P/QZ4P-J) give reliable property surfaces
    These choices were based on previous studies (citations 23, 37), but no functional or basis-set convergence study is presented here.
  • standard math Numerical differentiation with the 5-point stencil and h=0.50 yields accurate first and second property derivatives
    The stencil formulas (Eqs. 8-9) are standard, but their accuracy depends on the step length and smoothness of the property surface, which is only verified for HgCl2 (Section V.A).
  • standard math Born-Oppenheimer separation of electronic and nuclear motion is valid
    The whole approach computes electronic properties at distorted geometries and averages with vibrational wavefunctions, which presumes the Born-Oppenheimer approximation (Section II).

reviewed 2026-08-04 · how reviews work

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Cite this review

Pith. "Pith review of Vibrational corrections to molecular properties including relativistic corrections at the level of the Zeroth-Order Regular Approximation." pith.science (2026). https://pith.science/paper/L2CSIWKI

@misc{pith2026250912412,
  author       = {Pith},
  title        = {Pith review of: Vibrational corrections to molecular properties including relativistic corrections at the level of the Zeroth-Order Regular Approximation},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/L2CSIWKI}},
  note         = {Machine review of arXiv:2509.12412}
}
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read the original abstract

The vibrational averaging module of the Dalton Project was extended to work also with the Amsterdam Density Functional (ADF) program, making it possible to calculate vibrational corrections to properties and at the same time include a treatment of relativistic effects for heavier atoms at the level of the Zeroth-Order Regular Approximation (ZORA). To illustrate the importance of the relativistic contributions, zero-point vibrational corrections were calculated for the electric field gradient tensor and the two NMR parameters, the isotropic shielding and the spin-spin coupling constants (SSCC), of selected mercury compounds. For all three properties, the vibrational corrected values performed closest to experimental values, and the magnitudes of the corrections depended on the level of relativity and the basis set in the calculation.

Figures

Figures reproduced from arXiv: 2509.12412 by Lars Hemmingsen, Louise M{\o}ller Jessen, Ronan Gleeson, Stephan P. A. Sauer.

Figure 1
Figure 1. Figure 1: An example for the variations in the fitting of the changes in V [PITH_FULL_IMAGE:figures/full_fig_p009_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: An example of the step length analysis with 61 points and a fourth-degree polynomial of the [PITH_FULL_IMAGE:figures/full_fig_p010_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: The vibrational corrections for HgCl2 calculated at the spin-orbit ZORA level with different basis sets and the BHandHLYP functional. To the left is the correction to the Vzz, in the middle is the correction to the isotropic shielding, and to the right is the correction to the SSCC. The values can be found in section S2 of the supplementary material. ppm). For chlorine, the correction for TZ2P is closest t… view at source ↗
Figure 4
Figure 4. Figure 4: The correction for the electric field gradients [PITH_FULL_IMAGE:figures/full_fig_p013_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: The correction for the isotropic shielding constants [in ppm] calculated with PBE0/QZ4P at [PITH_FULL_IMAGE:figures/full_fig_p014_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: The correction for the 1 JHg-X, 1 JHg-C and 2 JHg-H SSCCs in the methylmercury-halides calculated with PBE0/QZ4P-J at different levels of relativity. Without relativistic corrections (none) is shown in blue, with scalar ZORA relativistic corrections (scalar) is shown in orange, and with also spin-orbit ZORA rela￾tivistic corrections (spin-orbit) is shown in green. The values and corrections can be found in… view at source ↗
Figure 7
Figure 7. Figure 7: The ratio between Vzz for two mercury-halides and between the three cadmium-halides calculated with ZORA(spin-orbit)/BHandHLYP/QZ4P. To the left are the values for the ratio calculated at the equilib￾rium geometry (blue), the ratio with vibrational correction (orange), and the ratio of the experimental values (green), where the uncertainties are the dotted green line. To the right are the deviations from t… view at source ↗
Figure 8
Figure 8. Figure 8: The 199Hg chemical shift for mercury-halides (HgX2) and the methylmercury-halides (MeHgX) with respect to Hg(CH3)2 calculated with ZORA(spin-orbit)/PBE0/QZ4P. To the left are the values for the shift (blue), the shift with correction (orange), and the experimental values (green). To the right are the deviations from the experimental values for the shift (blue) and the shift with correction (orange). The ch… view at source ↗
Figure 9
Figure 9. Figure 9: The 1 JHg-C (upper) and 2 JHg-H (lower) spin-spin coupling constants for the three methylmercury￾halides calculated with ZORA(spin-orbit)/PBE0/QZ4P(-J). To the left are the values for the SSCC (blue), the SSCC with correction (orange), and the experimental values (green). To the right are the deviations from the experimental values for the equilibrium SSCC (blue) and the corrected SSCC (orange). 3. SSCC Th… view at source ↗

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This paper was first reviewed by deepseek-v4-flash on August 4, 2026.