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We study the regularity of the flow $${\varvec{X}}(t,y)$$ X ( t , y ) , which represents (in the sense of Smirnov or as regular Lagrangian flow of Ambrosio) a solution $$\rho \in L^\infty ({\mathbb {R}}^{d+1})$$ ρ ∈ L ∞ ( R d + 1 ) of the continuity equation $$\begin{aligned} \partial _t \rho + {{\,\mathrm{div}\,}}(\rho {\varvec{b}}) = 0, \end{aligned}$$ ∂ t ρ + div ( ρ b ) = 0 , with $${\varvec{b}}\in L^1_t {{\,\mathrm{BV}\,}}_x$$ b ∈ L t 1 BV x . We prove that $${\varvec{X}}$$ X is differentiable in measure in the sense of Ambrosio–Malý, that is $$\begin{aligned} \frac{{\varvec{X}}(t,y+rz) - {\varvec{X}}(t,y)}{r} \underset{r \rightarrow 0}{\rightarrow } W(t,y) z \quad \text {in measure}, \end{aligned}$$ X ( t , y + r z ) - X ( t , y ) r → r → 0 W ( t , y ) z in measure , where the derivative W(t, y) is a BV function satisfying the ODE $$\begin{aligned} \frac{\mathrm{d}}{\mathrm{d}t} W(t, y) = \frac{(D {\varvec{b}})_y(\mathrm{d}t)}{J(t-,y)} W(t-, y), \end{aligned}$$ d d t W ( t , y ) = ( D b ) y ( d t ) J ( t - , y ) W ( t - , y ) , where $$(D{\varvec{b}})_y(\mathrm{d}t)$$ ( D b ) y ( d t ) is the disintegration of the measure $$\int D {\varvec{b}}(t,\cdot ) \, \mathrm {d}t$$ ∫ D b ( t , · ) d t with respect to the partition given by the trajectories $${\varvec{X}}(t, y)$$ X ( t , y ) and the Jacobian J(t, y) solves $$\begin{aligned} \frac{\mathrm{d}}{\mathrm{d}t} J(t,y) = ({{\,\mathrm{div}\,}}{\varvec{b}})_y(\mathrm{d}t) = \mathrm {Tr}(D{\varvec{b}})_y(\mathrm{d}t). \end{aligned}$$ d d t J ( t , y ) = ( div b ) y ( d t ) = Tr ( D b ) y ( d t ) . The proof of this regularity result is based on the theory of Lagrangian representations and proper sets introduced by Bianchini and Bonicatto in [16], on the construction of explicit approximate tubular neighborhoods of trajectories, and on estimates that take into account the local structure of the derivative of a $${{\,\mathrm{BV}\,}}$$ BV vector field.
We study the regularity of the flow $${\varvec{X}}(t,y)$$ X ( t , y ) , which represents (in the sense of Smirnov or as regular Lagrangian flow of Ambrosio) a solution $$\rho \in L^\infty ({\mathbb {R}}^{d+1})$$ ρ ∈ L ∞ ( R d + 1 ) of the continuity equation $$\begin{aligned} \partial _t \rho + {{\,\mathrm{div}\,}}(\rho {\varvec{b}}) = 0, \end{aligned}$$ ∂ t ρ + div ( ρ b ) = 0 , with $${\varvec{b}}\in L^1_t {{\,\mathrm{BV}\,}}_x$$ b ∈ L t 1 BV x . We prove that $${\varvec{X}}$$ X is differentiable in measure in the sense of Ambrosio–Malý, that is $$\begin{aligned} \frac{{\varvec{X}}(t,y+rz) - {\varvec{X}}(t,y)}{r} \underset{r \rightarrow 0}{\rightarrow } W(t,y) z \quad \text {in measure}, \end{aligned}$$ X ( t , y + r z ) - X ( t , y ) r → r → 0 W ( t , y ) z in measure , where the derivative W(t, y) is a BV function satisfying the ODE $$\begin{aligned} \frac{\mathrm{d}}{\mathrm{d}t} W(t, y) = \frac{(D {\varvec{b}})_y(\mathrm{d}t)}{J(t-,y)} W(t-, y), \end{aligned}$$ d d t W ( t , y ) = ( D b ) y ( d t ) J ( t - , y ) W ( t - , y ) , where $$(D{\varvec{b}})_y(\mathrm{d}t)$$ ( D b ) y ( d t ) is the disintegration of the measure $$\int D {\varvec{b}}(t,\cdot ) \, \mathrm {d}t$$ ∫ D b ( t , · ) d t with respect to the partition given by the trajectories $${\varvec{X}}(t, y)$$ X ( t , y ) and the Jacobian J(t, y) solves $$\begin{aligned} \frac{\mathrm{d}}{\mathrm{d}t} J(t,y) = ({{\,\mathrm{div}\,}}{\varvec{b}})_y(\mathrm{d}t) = \mathrm {Tr}(D{\varvec{b}})_y(\mathrm{d}t). \end{aligned}$$ d d t J ( t , y ) = ( div b ) y ( d t ) = Tr ( D b ) y ( d t ) . The proof of this regularity result is based on the theory of Lagrangian representations and proper sets introduced by Bianchini and Bonicatto in [16], on the construction of explicit approximate tubular neighborhoods of trajectories, and on estimates that take into account the local structure of the derivative of a $${{\,\mathrm{BV}\,}}$$ BV vector field.
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