Bourbaki

Theorem 2

Tag 08CS, permanent. Cite it as [Bourbaki, Tag 08CS].

Functions of a Real Variable, chapter IV, § 2. LINEAR DIFFERENTIAL EQUATIONS

For every point (t0,x0)(t_0, \mathbf{x}_0) of J×EJ \times E let u(t,t0,x0)\mathbf{u}(t, t_0, \mathbf{x}_0) be the integral of the homogeneous equation (4) defined on JJ and equal to x0\mathbf{x}_0 at t0t_0. 1. For every point t∈Jt \in J the map x0↦u(t,t0,x0)\mathbf{x}_0 \mapsto \mathbf{u}(t, t_0, \mathbf{x}_0) is a bijective bicontinuous linear map C(t,t0)C(t, t_0) of EE to itself. 2. The map t↦C(t,t0)t \mapsto C(t, t_0) of JJ into L(E)\mathscr{L}(E) is identical to the integral of the homogeneous linear differential equation

dUdt=A(t) U \frac{dU}{dt} = A(t)\ U
which takes the value II **(the identity map of* EE to itself) at the point t0t_0. 3. For any points s,t,us, t, u of JJ
C(s,u)=C(s,t)C(t,u),C(s,t)=(C(t,s))−1. C(s, u) = C(s, t)C(t, u), \qquad C(s, t) = (C(t, s))^{-1}.

By prop. 1, u(t,t0,x1)+u(t,t0,x2)\mathbf{u}(t, t_0, \mathbf{x}_1) + \mathbf{u}(t, t_0, \mathbf{x}_2) (resp. λu(t,t0,x0)\lambda \mathbf{u}(t, t_0, \mathbf{x}_0)) is an integral of (4) and takes the value x1+x2\mathbf{x}_1 + \mathbf{x}_2 (resp. λx0\lambda \mathbf{x}_0) at t0t_0, so, by th. 1 of IV, p. 179, is identical to u(t,t0,x1+x2)\mathbf{u}(t, t_0, \mathbf{x}_1 + \mathbf{x}_2) (resp. u(t,t0,λx0)\mathbf{u}(t, t_0, \lambda \mathbf{x}_0)); the map x0↦u(t,t0,x0)\mathbf{x}_0 \mapsto \mathbf{u}(t, t_0, \mathbf{x}_0) is thus a linear map C(t,t0)C(t, t_0) of E into itself, and one can write u(t,t0,x0)=C(t,t0).x0\mathbf{u}(t, t_0, \mathbf{x}_0) = C(t, t_0). \mathbf{x}_0.

Since the map (X,Y)↦XY(X, Y) \mapsto XY of L(E)×L(E)\mathscr{L}(E) \times \mathscr{L}(E) into L(E)\mathscr{L}(E) is continuous (Gen. Top., X, p. 298, prop. 8), the map t↦A(t)Ut \mapsto A(t)U of J into L(E)\mathscr{L}(E) is regulated for all U∈L(E)U \in \mathscr{L}(E); further (Gen. Top., X, p. 296)

∥A(t)X−A(t)Y∥=∥A(t)(X−Y)∥≤∥A(t)∥∥X−Y∥, \| A(t)X - A(t)Y \| = \| A(t)(X - Y) \| \leq \| A(t) \| \| X - Y \|,

so one can apply th. I of IV, p. 179 to the homogeneous linear equation (5); let V(t)V(t) be the integral of this equation defined on J and equal to II at t0t_0. One has (I, p. 6, prop. 3)

ddt(V(t)x0)=dV(t)dtx0=A(t)(V(t)x0) \frac{d}{dt} (V(t)\mathbf{x}_0) = \frac{dV(t)}{dt} \mathbf{x}_0 = A(t)(V(t)\mathbf{x}_0)

and for t=t0t = t_0 we have V(t)x0=Ix0=x0V(t)\mathbf{x}_0 = I\mathbf{x}_0 = \mathbf{x}_0; by th. 1 of IV, p. 179 one must have V(t).x0=C(t,t0)x0V(t).\mathbf{x}_0 = C(t, t_0)\mathbf{x}_0 for all x0∈E\mathbf{x}_0 \in E, that is, V(t)=C(t,t0)V(t) = C(t, t_0); this proves that C(t,t0)C(t, t_0) belongs to L(E)\mathscr{L}(E), in other words, that x0↦C(t,t0).x0\mathbf{x}_0 \mapsto C(t, t_0).\mathbf{x}_0 is continuous on E, and that the map t↦C(t,t0)t \mapsto C(t, t_0) is the integral of (5) which is equal to II at t0t_0.

Finally, the integral s↦C(s,u).x0s \mapsto C(s, u).\mathbf{x}_0 of (4) is equal to C(t,u).x0C(t, u).\mathbf{x}_0 at the point tt, so, by definition,

C(s,u).x0=C(s,t)(C(t,u).x0)=(C(s,t)C(t,u)).x0 C(s, u).\mathbf{x}_0 = C(s, t)(C(t, u).\mathbf{x}_0) = (C(s, t)C(t, u)).\mathbf{x}_0

for any x0∈E\mathbf{x}_0 \in E, whence the first relation (6); since C(s,s)=IC(s, s) = I one has C(s,t)C(t,s)=IC(s, t)C(t, s) = I, for any ss and tt in J; this proves (Set Theory, II, p. 86, corollary) that C(t,t0)C(t, t_0) is a bijective map of E onto itself, with inverse map C(t0,t)C(t_0, t). This completes the proof of the theorem.

One says that C(t,t0)C(t, t_0) is the resolvent of equation (2) of IV, p. 178.

Bourbaki puts the proof directly after the statement, so what is above is the statement and its proof together.

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Cites

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