[1] Zhenhua Chai, Baochang Shi* and Chengjie Zhan. Multiple-distribution-function lattice Boltzmann method for convection-diffusion-system-based incompressible Navier-Stokes equations. Physical Review E, 2022, 106(5): 055305.

[2] Xi Liu, Zhenhua Chai*, Chengjie. Zhan, Baochang Shi, Wenhua Zhang*. A Diffuse-domain phase-field lattice Boltzmann method for two-phase flows in complex geometries. Multiscale Modeling & Simulation, 2022, 20(4): 1411-1436.

[3] Jiao Liu, Zhenhua Chai*, Baochang Shi. Diffuse-interface lattice Boltzmann modeling of charged particle transport in Poiseuille flow. Physical Review E, 2022, 106: 015306.

[4] Jiao Liu,Changsheng Huang, Zhenhua Chai* and Baochang Shi.A diffuse-interface lattice Boltzmann method for fluid–particle interaction problems. Computers & Fluids, 2022 233: 105240.

[5] Chengjie Zhan, Zhenhua Chai*, Baochang Shi, Consistent and conservative phase-field-based lattice Boltzmann method for incompressible two-phase flows. Physical Review E, 2022, 106: 025319.

[6] Chengjie Zhan, Zhenhua Chai and Baochang Shi*. A two-relaxation-time lattice Boltzmann study on the Soret and Dufour effects of double-diffusive convection over a rough surface. Applied Mathematical Modelling, 2022, 106: 1-29.

[7]Changsheng Huang, Zhenhua Chai and Baochang Shi*. A recursive finite-difference lattice Boltzmann model for the convection–diffusion equation with a source term. Applied Mathematics Letters, 2022, 132: 108139.

[8] Liqing Yue, Zhenhua Chai*, Huili Wang, Baochang Shi. Improved phase-field-based lattice Boltzmann method for thermocapillary flow. Physical Review E, 2022, 105(1): 015314.

[9] Xiaolei Yuan, Baochang Shi, Chengjie Zhan, Zhenhua Chai*. A phase-field-based lattice Boltzmann model for multiphase flows involving N immiscible incompressible fluids. Physics of Fluids, 2022, 34(2).

[10] Yong Zhao, Gerald G. Pereira, Shibo Kuang, Zhenhua Chai and Baochang Shi*. A Pseudopotential Lattice Boltzmann Analysis for Multicomponent Flow. Communications in Computational Physics, 2022, 32(4): 1156-1178.