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Reaching precise proton affinities in non-Born-Oppenheimer calculations

Luukas Nikkanen, Susi Lehtola

TL;DR

The paper tackles how to achieve precise proton affinities in non-Born-Oppenheimer calculations by dissecting basis-set convergence for both electronic and protonic parts within the non-BO-DFT framework. It shows that electronic-basis truncation dominates non-BO errors and that uncontracting the electronic basis on quantum protons dramatically accelerates convergence, enabling chemical accuracy with relatively modest protonic bases across multiple basis families. The authors demonstrate complete basis-set convergence by testing diverse electronic (pc, cc, def2) and protonic (PB and even-tempered) bases, and they provide practical guidelines for balanced electronic-protonic pairings while cautioning against basis-mixture artifacts. The work thus offers actionable strategies for precise non-BO PA computations and informs future basis-set design for multi-component quantum chemistry.

Abstract

An attractive way to model nuclear quantum effects is to describe select nuclei quantum mechanically at the same level as the electrons. This non-Born-Oppenheimer (non-BO) method is known by many names including the nuclear-electronic orbital (NEO) and the multicomponent method. Two basis sets are typically used for such calculations: a nuclear basis set and an electronic basis set. In this work, we investigate the convergence of non-BO proton affinities (PAs) with respect to the protonic and electronic basis sets. PAs are a sensitive measure of the proton and electron densities. We demonstrate that most protonic basis sets are sufficient for non-BO density-functional calculations of PAs, resulting in convergence to within 0.1 kcal/mol of the complete protonic basis set limit. This indicates that the truncation error is dominated by the electronic basis, and that smaller protonic basis sets could be developed. We show that non-BO calculations should use uncontracted electronic basis sets on the quantum protons. The contraction coefficients in typical electronic basis sets have been derived for point nuclear charge distributions, and uncontracting the electronic basis set on the quantized proton leads to significantly faster convergence to the electronic basis set limit. Uncontraction leads to results of one $ζ$-level higher quality with negligible additional computational cost in multiple diffuse basis set families: Jensen's polarization consistent aug-pc-X basis sets, Dunning's correlation-consistent aug-cc-pVXZ basis sets, as well as the Karlsruhe def2-XZPD basis sets. In specific, the aug-pc-3 electronic basis set already affords PAs converged beyond 0.1 kcal/mol when uncontracted on the quantum proton.

Reaching precise proton affinities in non-Born-Oppenheimer calculations

TL;DR

The paper tackles how to achieve precise proton affinities in non-Born-Oppenheimer calculations by dissecting basis-set convergence for both electronic and protonic parts within the non-BO-DFT framework. It shows that electronic-basis truncation dominates non-BO errors and that uncontracting the electronic basis on quantum protons dramatically accelerates convergence, enabling chemical accuracy with relatively modest protonic bases across multiple basis families. The authors demonstrate complete basis-set convergence by testing diverse electronic (pc, cc, def2) and protonic (PB and even-tempered) bases, and they provide practical guidelines for balanced electronic-protonic pairings while cautioning against basis-mixture artifacts. The work thus offers actionable strategies for precise non-BO PA computations and informs future basis-set design for multi-component quantum chemistry.

Abstract

An attractive way to model nuclear quantum effects is to describe select nuclei quantum mechanically at the same level as the electrons. This non-Born-Oppenheimer (non-BO) method is known by many names including the nuclear-electronic orbital (NEO) and the multicomponent method. Two basis sets are typically used for such calculations: a nuclear basis set and an electronic basis set. In this work, we investigate the convergence of non-BO proton affinities (PAs) with respect to the protonic and electronic basis sets. PAs are a sensitive measure of the proton and electron densities. We demonstrate that most protonic basis sets are sufficient for non-BO density-functional calculations of PAs, resulting in convergence to within 0.1 kcal/mol of the complete protonic basis set limit. This indicates that the truncation error is dominated by the electronic basis, and that smaller protonic basis sets could be developed. We show that non-BO calculations should use uncontracted electronic basis sets on the quantum protons. The contraction coefficients in typical electronic basis sets have been derived for point nuclear charge distributions, and uncontracting the electronic basis set on the quantized proton leads to significantly faster convergence to the electronic basis set limit. Uncontraction leads to results of one -level higher quality with negligible additional computational cost in multiple diffuse basis set families: Jensen's polarization consistent aug-pc-X basis sets, Dunning's correlation-consistent aug-cc-pVXZ basis sets, as well as the Karlsruhe def2-XZPD basis sets. In specific, the aug-pc-3 electronic basis set already affords PAs converged beyond 0.1 kcal/mol when uncontracted on the quantum proton.

Paper Structure

This paper contains 13 sections, 6 equations, 9 figures, 1 table.

Figures (9)

  • Figure 1: Pople diagramPople1965_JCP_229 illustrating the complete basis set limit in non-BO calculations, which require going to the complete protonic and the complete electronic basis set.
  • Figure 2: Box plot representing the BSTEs of PAs obtained with the aug-pc-$n$ family of electronic basis sets and the PB4-F1 protonic basis set. The reference is the largest basis set studied, i.e., the uncHq-aug-pc-4/PB4-F1 values. The box is drawn from the first to the third quartile, thus containing the second and third quartiles, and the line represents the median. The whiskers show the full range of values. The shaded area shows the range of our target precision of $\pm0.1$ kcal/mol.
  • Figure 3: BSTEs of PAs obtained with the aug-pc-$n$ family using conventional BO calculations. All data are relative to the uncHq-aug-pc-4 values. Even though these calculations feature no quantum protons, the electronic basis set on the most acidic hydrogen is uncontracted in analogy to the results of \ref{['fig:pc']}. The distributions for the quadruple- and quintuple-$\zeta$ basis sets (aug-pc-3, uncHq-aug-pc-3, aug-pc-4) are sharply focused around zero. The plot and box parameters are the same as in \ref{['fig:pc']}
  • Figure 4: BSTEs of PAs obtained with the protonic PB set family and the electronic uncHq-aug-pc-4 basis set. All data are reported relative to uncHq-aug-pc-4/PB6-H values. Observe the small scale of the $y$-axis. The plot and box parameters are the same as in \ref{['fig:pc']}
  • Figure 5: BSTEs of PAs obtained with the even-tempered protonic basis sets and the electronic uncHq-aug-pc-4 basis set. All data are reported relative to uncHq-aug-pc-4/PB6-H values. KTZ refers to the basis sets of Khan2025_JCC_70082.Khan2025_JCC_70082 The plot and box parameters are the same as in \ref{['fig:pc']}
  • ...and 4 more figures