<p>Accurate representation of three-dimensional (3D) molecular structures is essential for quantitative structure-activity relationship (QSAR) modeling; however, it remains unclear whether increasing the level of theory used for quantum-chemical geometry optimization yields a practically meaningful benefit for classical conformation-dependent 3D descriptors (Dragon 3D) and the resulting QSAR performance. Here, we benchmark eight commonly used quantum-chemical (QM) geometry-optimization protocols—from minimal-basis Hartree–Fock (HF/STO-3&#xa0;G) to def2-based hybrid density functional theory (DFT) and the composite method r<InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(^2\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>2</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>SCAN-3c—across three anticancer activity datasets and ten machine-learning classifiers. Descriptor-level analyses (relative deviation, rank correlation, and chemical-space similarity) reveal systematic method dependence in descriptor magnitudes: high-accuracy def2-based DFT protocols produce highly consistent descriptor spaces, whereas some intermediate/low-level settings introduce larger variability, although molecular rankings remain largely robust (Spearman <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\rho &gt;0.95\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ρ</mi> <mo>&gt;</mo> <mn>0.95</mn> </mrow> </math></EquationSource> </InlineEquation>). In contrast, downstream QSAR performance is only weakly affected by the QM level. Across paired dataset<InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\times\)</EquationSource> <EquationSource Format="MATHML"><math> <mo>×</mo> </math></EquationSource> </InlineEquation>model blocks (<InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(n=30\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>=</mo> <mn>30</mn> </mrow> </math></EquationSource> </InlineEquation>), mean balanced accuracies cluster tightly (0.852–0.871). B3LYP/3-21&#xa0;G achieves the highest overall mean balanced accuracies (BA) (0.8709; 95% CI 0.8565–0.8840), while the lowest mean is observed for HF/STO-3&#xa0;G (0.8518; 95% CI 0.8371–0.8661); def2-based B3LYP methods are numerically slightly lower (<InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\sim\)</EquationSource> <EquationSource Format="MATHML"><math> <mo>∼</mo> </math></EquationSource> </InlineEquation>0.855–0.856). A repeated-measures omnibus test indicates a statistically detectable method effect (Friedman <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(p=0.006\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>=</mo> <mn>0.006</mn> </mrow> </math></EquationSource> </InlineEquation>) but with a small effect size (Kendall’s <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(W=0.094\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>W</mi> <mo>=</mo> <mn>0.094</mn> </mrow> </math></EquationSource> </InlineEquation>), and post-hoc Wilcoxon tests with Holm correction identify only one robust pairwise difference (B3LYP/3-21&#xa0;G vs. HF/STO-3&#xa0;G, <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(p_{\textrm{Holm}}=0.025\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>p</mi> <mtext>Holm</mtext> </msub> <mo>=</mo> <mn>0.025</mn> </mrow> </math></EquationSource> </InlineEquation>). Thus, the observed performance shifts are marginal in magnitude (<InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\le\)</EquationSource> <EquationSource Format="MATHML"><math> <mo>≤</mo> </math></EquationSource> </InlineEquation>1–2%) compared with the 10–100<InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\times\)</EquationSource> <EquationSource Format="MATHML"><math> <mo>×</mo> </math></EquationSource> </InlineEquation> differences in computational cost.To support pragmatic method selection, we propose a two-tier Absolute Efficiency Ratio (AER) framework integrating predictive performance with efficiency and methodological considerations. Overall, these results indicate a non-linear and practically weak relationship between QM geometry-optimization level, classical 3D descriptor fidelity, and QSAR performance, suggesting that QM-level upgrades mainly reshape descriptor values without yielding commensurate or actionable gains in predictive accuracy.</p>

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How quantum-chemical geometry optimization level affects classical 3D descriptors and QSAR performance: a comparative study

  • Jianmin Li,
  • Rongling Gu,
  • Shijie Du,
  • Lu Xu

摘要

Accurate representation of three-dimensional (3D) molecular structures is essential for quantitative structure-activity relationship (QSAR) modeling; however, it remains unclear whether increasing the level of theory used for quantum-chemical geometry optimization yields a practically meaningful benefit for classical conformation-dependent 3D descriptors (Dragon 3D) and the resulting QSAR performance. Here, we benchmark eight commonly used quantum-chemical (QM) geometry-optimization protocols—from minimal-basis Hartree–Fock (HF/STO-3 G) to def2-based hybrid density functional theory (DFT) and the composite method r \(^2\) 2 SCAN-3c—across three anticancer activity datasets and ten machine-learning classifiers. Descriptor-level analyses (relative deviation, rank correlation, and chemical-space similarity) reveal systematic method dependence in descriptor magnitudes: high-accuracy def2-based DFT protocols produce highly consistent descriptor spaces, whereas some intermediate/low-level settings introduce larger variability, although molecular rankings remain largely robust (Spearman \(\rho >0.95\) ρ > 0.95 ). In contrast, downstream QSAR performance is only weakly affected by the QM level. Across paired dataset \(\times\) × model blocks ( \(n=30\) n = 30 ), mean balanced accuracies cluster tightly (0.852–0.871). B3LYP/3-21 G achieves the highest overall mean balanced accuracies (BA) (0.8709; 95% CI 0.8565–0.8840), while the lowest mean is observed for HF/STO-3 G (0.8518; 95% CI 0.8371–0.8661); def2-based B3LYP methods are numerically slightly lower ( \(\sim\) 0.855–0.856). A repeated-measures omnibus test indicates a statistically detectable method effect (Friedman \(p=0.006\) p = 0.006 ) but with a small effect size (Kendall’s \(W=0.094\) W = 0.094 ), and post-hoc Wilcoxon tests with Holm correction identify only one robust pairwise difference (B3LYP/3-21 G vs. HF/STO-3 G, \(p_{\textrm{Holm}}=0.025\) p Holm = 0.025 ). Thus, the observed performance shifts are marginal in magnitude ( \(\le\) 1–2%) compared with the 10–100 \(\times\) × differences in computational cost.To support pragmatic method selection, we propose a two-tier Absolute Efficiency Ratio (AER) framework integrating predictive performance with efficiency and methodological considerations. Overall, these results indicate a non-linear and practically weak relationship between QM geometry-optimization level, classical 3D descriptor fidelity, and QSAR performance, suggesting that QM-level upgrades mainly reshape descriptor values without yielding commensurate or actionable gains in predictive accuracy.