TY - JOUR
T1 - Solving many-electron Schrödinger equation using deep neural networks
AU - Han, Jiequn
AU - Zhang, Linfeng
AU - E, Weinan
N1 - Funding Information: The authors acknowledge M. Motta for helpful discussions. This work is supported in part by Major Program of NNSFC under grant 91130005, ONR grant N00014-13-1-0338 and NSFC grant U1430237. We are grateful for the computing time provided by the High-performance Computing Platform of Peking University and the TIGRESS High Performance Computing Center at Princeton University. Funding Information: The authors acknowledge M. Motta for helpful discussions. This work is supported in part by Major Program of NNSFC under grant 91130005 , ONR grant N00014-13-1-0338 and NSFC grant U1430237 . We are grateful for the computing time provided by the High-performance Computing Platform of Peking University and the TIGRESS High Performance Computing Center at Princeton University. Appendix A Publisher Copyright: © 2019 Elsevier Inc.
PY - 2019/12/15
Y1 - 2019/12/15
N2 - We introduce a new family of trial wave-functions based on deep neural networks to solve the many-electron Schrödinger equation. The Pauli exclusion principle is dealt with explicitly to ensure that the trial wave-functions are physical. The optimal trial wave-function is obtained through variational Monte Carlo and the computational cost scales quadratically with the number of electrons. The algorithm does not make use of any prior knowledge such as atomic orbitals. Yet it is able to represent accurately the ground-states of the tested systems, including He, H2, Be, B, LiH, and a chain of 10 hydrogen atoms. This opens up new possibilities for solving large-scale many-electron Schrödinger equation.
AB - We introduce a new family of trial wave-functions based on deep neural networks to solve the many-electron Schrödinger equation. The Pauli exclusion principle is dealt with explicitly to ensure that the trial wave-functions are physical. The optimal trial wave-function is obtained through variational Monte Carlo and the computational cost scales quadratically with the number of electrons. The algorithm does not make use of any prior knowledge such as atomic orbitals. Yet it is able to represent accurately the ground-states of the tested systems, including He, H2, Be, B, LiH, and a chain of 10 hydrogen atoms. This opens up new possibilities for solving large-scale many-electron Schrödinger equation.
KW - Deep neural networks
KW - Schrödinger equation
KW - Trial wave-function
KW - Variational Monte Carlo
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U2 - https://doi.org/10.1016/j.jcp.2019.108929
DO - https://doi.org/10.1016/j.jcp.2019.108929
M3 - Article
SN - 0021-9991
VL - 399
JO - Journal of Computational Physics
JF - Journal of Computational Physics
M1 - 108929
ER -