“…Motivated by Ignatova and Vicol, to deal with better, we write u 1 ( t , x , y ) and b 1 ( t , x , y ) as perturbations u ( t , x , y ) and b ( t , x , y ) of the lifts κ 1 ϕ ( t , y ) and κ 2 ϕ ( t , y ), respectively, via where (please see the details in Appendix ). Denote by Then we introduce new linearly good unknowns …”