Permutation invariant polynomial neural network based diabatic ansatz for the (E plus A) x (e plus a) Jahn-Teller and Pseudo-Jahn-Teller systems

被引:9
作者
Guan, Yafu [1 ,2 ]
Yarkony, David R. [3 ]
Zhang, Dong H. [1 ,2 ]
机构
[1] Chinese Acad Sci, State Key Lab Mol React Dynam, Dalian Inst Chem Phys, Dalian 116023, Peoples R China
[2] Chinese Acad Sci, Ctr Theoret Computat Chem, Dalian Inst Chem Phys, Dalian 116023, Peoples R China
[3] Johns Hopkins Univ, Dept Chem, Baltimore, MD 21218 USA
基金
中国国家自然科学基金;
关键词
POTENTIAL-ENERGY SURFACES; NONADIABATIC COUPLING TERMS; BLOCK DIAGONALIZATION; AB-INITIO; ANALYTIC REPRESENTATION; FEEDFORWARD NETWORKS; QUASIDIABATIC STATES; CONICAL INTERSECTION; QUANTUM DYNAMICS; MULLIKEN-HUSH;
D O I
10.1063/5.0096912
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
In this work, the permutation invariant polynomial neural network (PIP-NN) approach is employed to construct a quasi-diabatic Hamiltonian for system with non-Abelian symmetries. It provides a flexible and compact NN-based diabatic ansatz from the related approach of Williams, Eisfeld, and co-workers. The example of H-3(+) is studied, which is an (E + A) x (e + a) Jahn-Teller and Pseudo-Jahn-Teller system. The PIP-NN diabatic ansatz is based on the symmetric polynomial expansion of Viel and Eisfeld, the coefficients of which are expressed with neural network functions that take permutation-invariant polynomials as input. This PIP-NN-based diabatic ansatz not only preserves the correct symmetry but also provides functional flexibility to accurately reproduce ab initio electronic structure data, thus resulting in excellent fits. The adiabatic energies, energy gradients, and derivative couplings are well reproduced. A good description of the local topology of the conical intersection seam is also achieved. Therefore, this diabatic ansatz completes the PIP-NN based representation of DPEM with correct symmetries and will enable us to diabatize even more complicated systems with complex symmetries.
引用
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页数:10
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共 77 条
[1]   An optimal adiabatic-to-diabatic transformation of the 1 2A′ and 2 2A′ states of H3 [J].
Abrol, R ;
Kuppermann, A .
JOURNAL OF CHEMICAL PHYSICS, 2002, 116 (03) :1035-1062
[2]   Determination of diabatic states through enforcement of configurational uniformity [J].
Atchity, GJ ;
Ruedenberg, K .
THEORETICAL CHEMISTRY ACCOUNTS, 1997, 97 (1-4) :47-58
[3]   ADIABATIC AND DIABATIC REPRESENTATIONS FOR ATOM-DIATOM COLLISIONS - TREATMENT OF 3-DIMENSIONAL CASE [J].
BAER, M .
CHEMICAL PHYSICS, 1976, 15 (01) :49-57
[4]   Introduction to the theory of electronic non-adiabatic coupling terms in molecular systems [J].
Baer, M .
PHYSICS REPORTS-REVIEW SECTION OF PHYSICS LETTERS, 2002, 358 (02) :75-142
[5]  
Baer M, 2006, Beyond Born-Oppenheimer: Electronic Nonadiabatic Coupling Terms and Conical Intesections
[6]   The (E plus A) x (e plus a) Jahn-Teller and Pseudo-Jahn-Teller Hamiltonian Including Spin Orbit Coupling for Trigonal Systems [J].
Bhattacharyya, Swarnendu ;
Opalka, Daniel ;
Poluyanov, Leonid V. ;
Domcke, Wolfgang .
JOURNAL OF PHYSICAL CHEMISTRY A, 2014, 118 (51) :11962-11970
[7]   Permutationally invariant potential energy surfaces in high dimensionality [J].
Braams, Bastiaan J. ;
Bowman, Joel M. .
INTERNATIONAL REVIEWS IN PHYSICAL CHEMISTRY, 2009, 28 (04) :577-606
[8]  
Bunker P. R., 2006, Molecular Symmetry and Spectroscopy, V46853
[9]   Generalization of the Mulliken-Hush treatment for the calculation of electron transfer matrix elements [J].
Cave, RJ ;
Newton, MD .
CHEMICAL PHYSICS LETTERS, 1996, 249 (1-2) :15-19
[10]   Calculation of electronic coupling matrix elements for ground and excited state electron transfer reactions: Comparison of the generalized Mulliken-Hush and block diagonalization methods [J].
Cave, RJ ;
Newton, MD .
JOURNAL OF CHEMICAL PHYSICS, 1997, 106 (22) :9213-9226