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Smooth dependence of solutions on initial data

Statement

Let F:DR×RnRn be smooth in the state variable, and suppose nearby initial states share one compact local time interval I. Then the solution map

Φ:I×U0Rn,Φ(t,y)=x(t;y),

is smooth in the initial-state variable y on some neighbourhood U0 of the base point.

Facts & Assumptions

Given: The common local solution map Φ(t,y)=x(t;y) on a compact time interval I.

[L1]

The solution map is C1 in the initial data, and the first derivative is given by the variational equation (C1 dependence of solutions on initial data).

[F1]

The variational equation is a linear matrix ODE whose coefficients are the state derivatives of the vector field along the base solution (The variational equation along an ODE solution).

[L2]

Linear matrix ODEs on a compact interval have unique solutions (Linear matrix ODEs have unique global solutions on a fixed interval).

[F2]

Every solution satisfies the Volterra integral equation (A first-order initial value problem is equivalent to its Volterra integral equation).

Proof

technique · direct
1.1

By [L1], the derivative DyΦ(t,y) exists and is the solution of the variational equation below.

L1F1

t(DyΦ)=DxF(t,Φ(t,y))DyΦ,DyΦ(t0,y)=In.

Because F is smooth and Φ is continuous, the coefficient DxF(t,Φ(t,y)) is as regular in y as Φ is.

2.1

For each r1, let Er be the finite-dimensional space of r-linear maps (Rn)rRn, with E0:=Rn. Repeated differentiation of the ODE or of its Volterra form produces the finite-dimensional jet system below.

F1F2step 1.1algebra

Jr=Gr(t,Jr)

for Jr=(X0,,Xr)E0××Er, whose first components are

X0=F(t,X0),X1=DxF(t,X0)X1,

and whose higher components have the form Xm=DxF(t,X0)Xm+Pm(t,X0,,Xm1), where Pm is a universal polynomial expression in derivatives of F and lower jets. For example, X2=DxF(t,X0)X2+Dx2F(t,X0)[X1,X1]. Because F is smooth, each Gr is smooth in its state variables.

3.1

Fix r1. If Φ is Cr in y, then its jet Jr(t,y)=(Φ,DyΦ,,DyrΦ)(t,y) is a continuous solution of the system from step 2.1 on the same compact interval I, with initial data X0(t0)=y, X1(t0)=In, and Xm(t0)=0 for m2. The highest-jet component is linear in Xr once the lower jets are fixed, so [L2] supplies its unique evolution on I. Applying [L1] to this enlarged smooth system shows that Jr depends C1 on the initial value y. In particular its first component Φ is Cr+1 in y.

L1L2step 2.1
4.1

Step 1.1 is the base case r=1. Step 3.1 upgrades Cr regularity of Φ to Cr+1 for every r1, so by induction Φ is Cm in y for every m. Therefore Φ is smooth in the initial-state variable.

step 1.1step 3.1
5.1

Hence the solution map depends smoothly on initial data.

step 4.1

Depends on

Used by

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Sources