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Preprint of "Critical Assessment of Curvature-Driven Surface Hopping Algorithms"

Slavicek, Petr; Paušová, Šárka; Bouzek, Karel

Abstract

Trajectory surface-hopping (TSH) methods have become the most used approach in nonadiabatic molecular dynamics. The increasingly popular curvature-driven schemes represent a subset of TSH based on implicit local diabatization of potential energy surfaces. Their appeal partly stems from compatibility with machine-learning frameworks that often provide only local PES information. Here, we critically assess the limitations of these curvature-based algorithms by examining three challenging scenarios: (i) dynamics involving more than two strongly coupled electronic states; (ii) trivial crossings; and (iii) spurious transitions arising from small discontinuities in multireference potential energy surfaces. Furthermore, we extend the Landau–Zener Surface Hopping (LZSH) method beyond two-state systems and introduce practical modifications to enhance its robustness. The performance is benchmarked on both low- and higher-dimensional model Hamiltonians, as well as realistic molecular systems treated with \textit{ab initio} methods. While curvature-driven TSH using the explicit electronic coefficient propagation qualitatively captures the dynamics in most cases, we find no regime where it outperforms LZSH, especially when trivial crossings, multistate crossings, or discontinuities are encountered. Hence, we advocate for using a conceptually simple but solid LZSH method when nonadiabatic couplings are not available.

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Supporting information Curvature Based Surface Hopping Algorithms Tom´aˇs J´ıra, Jiˇr´ı Janoˇs and Petr Slav´ıˇcek∗ University of Chemistry and Technology, 166 28 Prague 6, Czech Republic ∗Corresponding author: [email protected] 1 Uracil VC Model Constants Below are the constants for an 8-dimensional uracil model described in Ref. 1. Mode κ(0) κ(1) κ(2) κ(3) λ(02) λ(13) γ(0) γ(1) γ(2) γ(3) ν18 -0.02203 0.09074 0.02748 -0.04054 -0.03538 0.08077 0.01938 0.00694 -0.00294 0.00752 ν20 -0.12147 0.05316 0.11233 0.00747 -0.02049 0.01489 0.00828 0.00183 0.00546 ν21 -0.09468 0.04454 0.14539 0.00050 0.07284 0.00970 0.00096 -0.00114 0.01108 Table 1: Uracil VC model constants for ν18,ν20 and ν21 modes using the harmonic potential. Mode d0a q0e0λ(02) λ(13) ν25 (D0) 4.80270 –0.13675 0.02883 –0.00007 0.00114 0.12606 (D1) 74.15995 –0.03064 –1.34468 –0.12082 (D2) 90.76928 –0.03374 –0.29923 –0.00916 (D3) 20.56079 –0.08044 0.38841 –0.02071 ν26 (D0) 22.92802 0.07438 –0.32069 –0.01274 0.13035 0.14272 (D1) 18.27440 0.07911 –0.01711 –0.00003 (D2) 9.46894 0.08653 0.37635 –0.01037 (D3) 65.09678 0.03660 1.66312 –0.25639 ν24 (D0) 41.89704 0.04719 0.81440 –0.06431 –0.01832 (D1) 38.37122 0.05231 0.37488 –0.01505 (D2) 39.25691 0.05286 0.14859 –0.00244 (D3) 37.97847 0.05431 –0.18152 –0.00366 Table 2: Uracil VC model constants for the ν25,ν26 and ν24 modes using the Morse potential. 1 Mode k(0) k(1) k(2) λ(01) λ(12) ν10 0.03317 0.01157 0.01534 0.04633 0.03148 ν12 0.02979 0.01488 0.01671 0.03540 0.03607 Table 3: Uracil VC model constants for ν10 and ν12 modes using the quartic potentials. 2 LZSH Discontinuity Patch Effect 200 400 600 Time (a.u.) 0.0 0.2 0.4 0.6 0.8 1.0 Populations S0LZSH S1LZSH S0LZSH (no patch) S1LZSH (no patch) Figure 1: Comparison of electronic population dynamics in cis-stilbene using the LZSH method with and without the discontinuity correction described in the main manuscript. References Patricia Vindel-Zandbergen, Spiridoula Matsika, and Neepa T. Maitra. Exact-factorization-based surface hopping for multistate dynamics. The Journal of Physical Chemistry Letters, 13(7):1785–1790, 2022. doi: 10.1021/acs. jpclett.1c04132. 2