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From molecular dynamics to kinetic models: data-driven generalized collision operators in 1D3V plasmas

Yue Zhao, Guosheng Fu, Huan Lei

Abstract

We present a data-driven approach for constructing generalized collisional kinetic models for inhomogeneous plasmas in one-dimensional physical space and three-dimensional velocity space (1D-3V). The collision operator is directly learned from micro-scale molecular dynamics (MD) and accurately accounts for the unresolved particle interactions over a broad range of plasma conditions. Unlike the standard Landau operator, the present operator takes an anisotropic, non-stationary form that captures the heterogeneous collisional energy transfer arising from the many-body interactions, which is crucial for plasma kinetics beyond the weakly coupled regime. Efficient numerical evaluation is achieved through a low-rank tensor representation with $O(N \log N)$ computational complexity. The constructed kinetic equation strictly preserves conservation laws and physical constraints and therefore, enables us to develop an explicit second-order, energy-conserving scheme that ensures fully discrete conservation of mass and total energy. Numerical results demonstrate that the present model accurately predicts both transport coefficients and several 1D-3V kinetic processes compared with MD simulations across a broad range of densities and temperatures in spatially inhomogeneous settings. This work provides a systematic pathway for bridging micro-scale MD and inhomogeneous plasma kinetic descriptions where empirical models show limitation.

From molecular dynamics to kinetic models: data-driven generalized collision operators in 1D3V plasmas

Abstract

We present a data-driven approach for constructing generalized collisional kinetic models for inhomogeneous plasmas in one-dimensional physical space and three-dimensional velocity space (1D-3V). The collision operator is directly learned from micro-scale molecular dynamics (MD) and accurately accounts for the unresolved particle interactions over a broad range of plasma conditions. Unlike the standard Landau operator, the present operator takes an anisotropic, non-stationary form that captures the heterogeneous collisional energy transfer arising from the many-body interactions, which is crucial for plasma kinetics beyond the weakly coupled regime. Efficient numerical evaluation is achieved through a low-rank tensor representation with computational complexity. The constructed kinetic equation strictly preserves conservation laws and physical constraints and therefore, enables us to develop an explicit second-order, energy-conserving scheme that ensures fully discrete conservation of mass and total energy. Numerical results demonstrate that the present model accurately predicts both transport coefficients and several 1D-3V kinetic processes compared with MD simulations across a broad range of densities and temperatures in spatially inhomogeneous settings. This work provides a systematic pathway for bridging micro-scale MD and inhomogeneous plasma kinetic descriptions where empirical models show limitation.

Paper Structure

This paper contains 17 sections, 3 theorems, 58 equations, 8 figures.

Key Result

Proposition 1

The Ampère solver iteratively updates the electric field $E^{n}$ instead of recalculating it from the density distribution, which ensures the conservation of total energy $\mathcal{E}$.

Figures (8)

  • Figure 1: Comparison of the diffusion and viscosity coefficients predicted from MD, Landau equation and DDCO models under different temperatures $T_0$ and densities $\rho = m_0 n$ with number density $n_{1}=10^{21}~{\rm m}^{-3}$ and $n_{2}=10^{24}~{\rm m}^{-3}$.
  • Figure 2: Comparison of the instantaneous velocity distribution on the $v_x$-$v_y$ plane at $t=0.4~t_{0}$ (up) and $0.8~t_{0}$ (bottom) with the initial symmetric double-well distribution. "DDCO" represents our model with the data-driven collision operator.
  • Figure 3: Comparison of the instantaneous velocity distribution on the $v_x$-$v_y$ plane at $t=0.4~t_{0}$ (up) and $0.8~t_{0}$ (bottom) with the initial asymmetric double-well distribution.
  • Figure 4: Comparison of the instantaneous velocity distribution on the $x$-$v_{x}$ plane at $t=0.4~t_{0}$ (left) and $0.6~t_{0}$ (right) with the initial symmetric double-well distribution.
  • Figure 5: Comparison of the instantaneous velocity distribution on the $x$-$v_{x}$ plane at $t=0.4~t_{0}$ (left) and $0.6~t_{0}$ (right) with the initial asymmetric double-well distribution.
  • ...and 3 more figures

Theorems & Definitions (7)

  • Proposition 1
  • proof
  • Remark 1
  • Proposition 2
  • proof
  • Proposition 3
  • proof