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Proof of The Twice Continuously Differentiable Extension Determined by Affine-Controlled Rate Data

lemmalem:affine-c2-extension-2026a
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Reason: Proof that C^2 affine-controlled rate data restrict to an affine-controlled transition-rate family, that the unit neighbourhood V of the control set is open, convex and bounded, that the induced extension is twice continuously differentiable with derivative bound K, and that its second control derivatives vanish.

Proof

Throughout we fix an ordered pair (σ,γ)(\sigma,\gamma) with σγ\sigma\neq\gamma in {1,,l}\{1,\dots,l\} and abbreviate g=βˉ0(σ,γ,)g=\bar{\beta}_0(\sigma,\gamma,\cdot) and gk=βˉ1k(σ,γ,)g_k=\bar{\beta}_1^k(\sigma,\gamma,\cdot) for k{1,,m}k\in\{1,\dots,m\}; these are real-valued functions on UU. All estimates obtained below hold for every such pair, of which there are finitely many. We write

F(x)=βˉ(σ,γ,Σ,α)=g(Σ)+k=1mgk(Σ)αk(x=(Σ,α)U×V),F(x)=\bar{\beta}(\sigma,\gamma,\Sigma,\alpha)=g(\Sigma)+\sum_{k=1}^mg_k(\Sigma)\,\alpha^k\qquad(x=(\Sigma,\alpha)\in U\times V),

the second equality being the coordinate formula for the dot product. We use throughout the norm properties: clause 1 (the square of the norm is the sum of the squares of the coordinates), clause 4 (xix|x_i|\le|x|), clause 5 (absolute homogeneity) and clause 6 (the triangle inequality). By the definition of the rate data, UU is open, convex and bounded with ΔlU\Delta^l\subset U, the control set A\mathcal{A} is nonempty, convex and compact, each of g,g1,,gmg,g_1,\dots,g_m is a C1C^1 map on UU whose partial derivatives are again C1C^1 on UU, and all of g,gk|g|,|g_k|, their first partial derivatives and their second partial derivatives are bounded by K0K_0 on UU.

Step 0. Elementary bounds.

(0a) If n1n\ge1, yRny\in\mathbb{R}^n and C0C\ge0 is a real number with yiC|y_i|\le C for every ii, then ynC|y|\le\sqrt{n}\,C. Indeed yi2=yi2C2y_i^2=|y_i|^2\le C^2 by monotonicity of squaring (clause 2), so y2=iyi2nC2=(nC)2|y|^2=\sum_iy_i^2\le nC^2=(\sqrt{n}\,C)^2, and since y0|y|\ge0 and nC0\sqrt{n}\,C\ge0 the same clause, read in the other direction, gives ynC|y|\le\sqrt{n}\,C.

(0b) 1l1\le\sqrt{l} and 1m1\le\sqrt{m}: since 1l1\le l and 12=11^2=1, (l)2=l(\sqrt{l})^2=l, clause 2 of the same lemma applied to the nonnegative reals 11 and l\sqrt{l} gives 1l1\le\sqrt{l}; likewise for mm.

(0c) For x=(Σ,α)x=(\Sigma,\alpha) and x=(Σ,α)x'=(\Sigma',\alpha') in Rl+m\mathbb{R}^{l+m} we have ΣΣxx|\Sigma-\Sigma'|\le|x-x'| and ααxx|\alpha-\alpha'|\le|x-x'|, because ΣΣ2ΣΣ2+αα2=xx2|\Sigma-\Sigma'|^2\le|\Sigma-\Sigma'|^2+|\alpha-\alpha'|^2=|x-x'|^2 and both quantities are nonnegative, so clause 2 of the monotonicity lemma applies; similarly for the second inequality.

(0d) U×VU\times V is an open subset of Rl+m\mathbb{R}^{l+m} once VV is known to be open (Step 2): given x=(Σ,α)U×Vx=(\Sigma,\alpha)\in U\times V, choose ρ1,ρ2>0\rho_1,\rho_2>0 such that every point within distance ρ1\rho_1 of Σ\Sigma lies in UU and every point within distance ρ2\rho_2 of α\alpha lies in VV; if xx<min(ρ1,ρ2)|x'-x|<\min(\rho_1,\rho_2) then by (0c) ΣΣ<ρ1|\Sigma'-\Sigma|<\rho_1 and αα<ρ2|\alpha'-\alpha|<\rho_2, so xU×Vx'\in U\times V.

Step 1. The restriction is an affine-controlled family (clause 1).

Requirement 1 of an affine-controlled transition-rate family is exactly clause 1 of the rate-data definition, restricted to Δl×A\Delta^l\times\mathcal{A}.

For requirement 2, let ff be any one of g,g1,,gmg,g_1,\dots,g_m and let Σ,ΣΔl\Sigma,\Sigma'\in\Delta^l. Since ΔlU\Delta^l\subset U and UU is convex, the segment joining Σ\Sigma to Σ\Sigma' lies in UU. The map ff is C1C^1 on the open set UU with ifK0|\partial_if|\le K_0 there, so clause (i) of the multivariate Taylor lemma, applied with n=ln=l and M1=K0M_1=K_0, gives

f(Σ)f(Σ)lK0ΣΣ.|f(\Sigma)-f(\Sigma')|\le\sqrt{l}\,K_0\,|\Sigma-\Sigma'| .

In particular β0(Σ)β0(Σ)lK0ΣΣΛΣΣ|\beta_0(\Sigma)-\beta_0(\Sigma')|\le\sqrt{l}\,K_0|\Sigma-\Sigma'|\le\Lambda|\Sigma-\Sigma'|, using 1m1\le\sqrt{m} from (0b). Applying the displayed bound to each component gkg_k and then (0a) in Rm\mathbb{R}^m gives

β1(Σ)β1(Σ)mlK0ΣΣ=ΛΣΣ.|\beta_1(\Sigma)-\beta_1(\Sigma')|\le\sqrt{m}\,\sqrt{l}\,K_0\,|\Sigma-\Sigma'|=\Lambda|\Sigma-\Sigma'| .

Thus both maps are Lipschitz with constant Λ\Lambda on Δl\Delta^l, and since A\mathcal{A} is nonempty, convex and compact, (β0,β1)(\beta_0,\beta_1) is an affine-controlled transition-rate family on ll states with control set A\mathcal{A} and Lipschitz constant Λ\Lambda. By clause 1 of the lemma on affine-controlled data, RR and BB are finite nonnegative real numbers, and by its clause 2 the associated β\beta is a transition-rate family on ll states with control set A\mathcal{A} and rate bound BB. This proves clause 1.

Step 2. The set VV (clause 2).

AV\mathcal{A}\subseteq V. For αA\alpha\in\mathcal{A} the set whose infimum defines ρ(α)\rho(\alpha) contains the value αα=0|\alpha-\alpha|=0 and consists of nonnegative numbers, so ρ(α)=0<1\rho(\alpha)=0<1.

Openness. Let αV\alpha\in V and put s=ρ(α)<1s=\rho(\alpha)<1 and ϱ=1s>0\varrho=1-s>0. If αα<ϱ|\alpha'-\alpha|<\varrho then clause 3 of the nonexpansiveness lemma gives ρ(α)αα+ρ(α)<ϱ+s=1\rho(\alpha')\le|\alpha'-\alpha|+\rho(\alpha)<\varrho+s=1, so αV\alpha'\in V. Hence VV is open.

The bound αR+1|\alpha|\le R+1, and boundedness. Let αV\alpha\in V, put s=ρ(α)<1s=\rho(\alpha)<1 and ε=(1s)/2>0\varepsilon=(1-s)/2>0. By clause 4 of the approximation property of the infimum there is aAa\in\mathcal{A} with αa<s+ε<1|\alpha-a|<s+\varepsilon<1. Since aR|a|\le R by the definition of RR as a supremum, the triangle inequality gives αa+αaR+1|\alpha|\le|a|+|\alpha-a|\le R+1. In particular every point of VV lies within distance R+1R+1 of the origin, so VV is a bounded set.

Convexity. Let α,αV\alpha,\alpha'\in V and let tt be real with 0t10\le t\le1. Put s=max{ρ(α),ρ(α)}<1s=\max\{\rho(\alpha),\rho(\alpha')\}<1 and ε=(1s)/2>0\varepsilon=(1-s)/2>0, and apply the approximation property of the infimum separately to ρ(α)\rho(\alpha) and to ρ(α)\rho(\alpha') to obtain a,aAa,a'\in\mathcal{A} with αa<ρ(α)+εs+ε|\alpha-a|<\rho(\alpha)+\varepsilon\le s+\varepsilon and αa<ρ(α)+εs+ε|\alpha'-a'|<\rho(\alpha')+\varepsilon\le s+\varepsilon. Since A\mathcal{A} is convex, ta+(1t)aAta+(1-t)a'\in\mathcal{A}, and by absolute homogeneity and the triangle inequality

tα+(1t)α(ta+(1t)a)tαa+(1t)αa<s+ε<1.\big|t\alpha+(1-t)\alpha'-\big(ta+(1-t)a'\big)\big|\le t|\alpha-a|+(1-t)|\alpha'-a'|<s+\varepsilon<1 .

As ρ(tα+(1t)α)\rho(t\alpha+(1-t)\alpha') is a lower bound for the distances to points of A\mathcal{A}, it follows that ρ(tα+(1t)α)<1\rho(t\alpha+(1-t)\alpha')<1, that is, tα+(1t)αVt\alpha+(1-t)\alpha'\in V. This proves clause 2, and with it (0d).

Step 3. The partial derivatives of βˉ\bar{\beta} (clause 4).

Let x=(Σ,α)U×Vx=(\Sigma,\alpha)\in U\times V.

(a) State coordinates. Fix i{1,,l}i\in\{1,\dots,l\} and hold all coordinates of xx except xix_i fixed. By the slice-function lemma, the slice of gg in the coordinate xix_i is differentiable at Σ\Sigma with derivative ig(Σ)\partial_ig(\Sigma), and likewise for each gkg_k. The slice of FF in the coordinate xix_i is the finite linear combination of these slices with the constant coefficients 1,α1,,αm1,\alpha^1,\dots,\alpha^m, so by the linear-combination rule it is differentiable with derivative ig(Σ)+kαkigk(Σ)\partial_ig(\Sigma)+\sum_k\alpha^k\partial_ig_k(\Sigma). By the slice-function lemma again,

iF(x)=ig(Σ)+k=1mαkigk(Σ).\partial_iF(x)=\partial_ig(\Sigma)+\sum_{k=1}^m\alpha^k\,\partial_ig_k(\Sigma).

(b) Control coordinates. Fix k{1,,m}k\in\{1,\dots,m\} and hold all coordinates except xl+kx_{l+k} fixed. The slice of FF in that coordinate is the map tc0+gk(Σ)tt\mapsto c_0+g_k(\Sigma)\,t, where c0=g(Σ)+kkgk(Σ)αkc_0=g(\Sigma)+\sum_{k'\neq k}g_{k'}(\Sigma)\alpha^{k'} does not depend on tt. For every real h0h\neq0 the corresponding difference quotient is

(c0+gk(Σ)(t+h))(c0+gk(Σ)t)h=gk(Σ),\frac{\big(c_0+g_k(\Sigma)(t+h)\big)-\big(c_0+g_k(\Sigma)t\big)}{h}=g_k(\Sigma),

a quantity independent of hh; hence the slice is differentiable with derivative gk(Σ)g_k(\Sigma), and by the slice-function lemma l+kF(x)=gk(Σ)\partial_{l+k}F(x)=g_k(\Sigma). This is the first identity of clause 4.

(c) Second derivatives. The function iF\partial_iF computed in (a) has exactly the form treated in (a) and (b), with g,gkg,g_k replaced by ig,igk\partial_ig,\partial_ig_k, which are again C1C^1 on UU. Hence, for i,i{1,,l}i,i'\in\{1,\dots,l\} and k{1,,m}k\in\{1,\dots,m\},

iiF(x)=iig(Σ)+k=1mαkiigk(Σ),l+kiF(x)=igk(Σ),\partial_{i'}\partial_iF(x)=\partial_{i'}\partial_ig(\Sigma)+\sum_{k=1}^m\alpha^k\,\partial_{i'}\partial_ig_k(\Sigma),\qquad \partial_{l+k}\partial_iF(x)=\partial_ig_k(\Sigma),

the second identity being the third identity of clause 4. Finally l+kF(x)=gk(Σ)\partial_{l+k}F(x)=g_k(\Sigma) depends only on Σ\Sigma, so its slice in any control coordinate xl+kx_{l+k'} is constant and every difference quotient vanishes, giving l+kl+kF=0\partial_{l+k'}\partial_{l+k}F=0, the second identity of clause 4; and its slice in a state coordinate xix_{i'} gives il+kF(x)=igk(Σ)\partial_{i'}\partial_{l+k}F(x)=\partial_{i'}g_k(\Sigma). This proves clause 4.

Step 4. Derivative bounds.

By the bounds in the rate-data definition and (0a) in Rm\mathbb{R}^m, the vector iβˉ1(σ,γ,Σ)\partial_i\bar{\beta}_1(\sigma,\gamma,\Sigma) with components igk(Σ)\partial_ig_k(\Sigma) satisfies iβˉ1(σ,γ,Σ)mK0|\partial_i\bar{\beta}_1(\sigma,\gamma,\Sigma)|\le\sqrt{m}\,K_0, and similarly for the vectors formed by iigk(Σ)\partial_{i'}\partial_ig_k(\Sigma) and by gk(Σ)g_k(\Sigma). Using clause 2 of the present lemma (αR+1|\alpha|\le R+1 on VV) and the Cauchy-Schwarz inequality, the identities of Step 3 give, at every point of U×VU\times V,

iFK0+mK0(R+1)=K,l+kF=gkK0K,|\partial_iF|\le K_0+\sqrt{m}\,K_0(R+1)=K,\qquad |\partial_{l+k}F|=|g_k|\le K_0\le K,

and, for the second derivatives,

iiFK0+mK0(R+1)=K,l+kiF=igkK0K,il+kF=igkK0K,|\partial_{i'}\partial_iF|\le K_0+\sqrt{m}\,K_0(R+1)=K,\qquad |\partial_{l+k}\partial_iF|=|\partial_ig_k|\le K_0\le K,\qquad |\partial_{i'}\partial_{l+k}F|=|\partial_{i'}g_k|\le K_0\le K,

and l+kl+kF=0K|\partial_{l+k'}\partial_{l+k}F|=0\le K, where K0KK_0\le K because m(R+1)0\sqrt{m}(R+1)\ge0. This is requirement 3 of a twice continuously differentiable extension.

Step 5. Uniform continuity of the second derivatives, and regularity.

Let ε>0\varepsilon>0 be real and put

η=ε2(1+m(R+1)),δ2=ε2(mK0+lK0+1).\eta=\frac{\varepsilon}{2\big(1+\sqrt{m}(R+1)\big)},\qquad \delta_2=\frac{\varepsilon}{2\big(\sqrt{m}K_0+\sqrt{l}K_0+1\big)} .

Requirement 4 of the rate-data definition, applied to each of the finitely many functions g,g1,,gmg,g_1,\dots,g_m attached to each of the finitely many ordered pairs (σ,γ)(\sigma,\gamma), yields a real δ1>0\delta_1>0 such that all second partial derivatives of all these functions change by at most η\eta between any two points of UU at distance at most δ1\delta_1. Put δ=min{δ1,δ2}>0\delta=\min\{\delta_1,\delta_2\}>0 and let x=(Σ,α)x=(\Sigma,\alpha) and x=(Σ,α)x'=(\Sigma',\alpha') be points of U×VU\times V with xxδ|x-x'|\le\delta; by (0c), ΣΣδ|\Sigma-\Sigma'|\le\delta and ααδ|\alpha-\alpha'|\le\delta.

For i,i{1,,l}i,i'\in\{1,\dots,l\} let cc and cc' be the vectors of Rm\mathbb{R}^m with components iigk(Σ)\partial_{i'}\partial_ig_k(\Sigma) and iigk(Σ)\partial_{i'}\partial_ig_k(\Sigma') respectively. By (0a), ccmη|c-c'|\le\sqrt{m}\,\eta and cmK0|c'|\le\sqrt{m}\,K_0. Hence, by Step 3(c), the triangle inequality and Cauchy-Schwarz,

iiF(x)iiF(x)iig(Σ)iig(Σ)+(cc)α+c(αα)η+mη(R+1)+mK0δε2+ε2=ε,|\partial_{i'}\partial_iF(x)-\partial_{i'}\partial_iF(x')|\le\big|\partial_{i'}\partial_ig(\Sigma)-\partial_{i'}\partial_ig(\Sigma')\big|+|(c-c')\cdot\alpha|+|c'\cdot(\alpha-\alpha')|\le\eta+\sqrt{m}\,\eta\,(R+1)+\sqrt{m}\,K_0\,\delta\le\frac{\varepsilon}{2}+\frac{\varepsilon}{2}=\varepsilon ,

using the choices of η\eta and δ2\delta_2. For the mixed second derivatives, Step 3(c) and clause (i) of the Taylor lemma applied to gkg_k (whose first partial derivatives are bounded by K0K_0 on the convex set UU) give

l+kiF(x)l+kiF(x)=igk(Σ)igk(Σ)lK0ΣΣlK0δε2ε,|\partial_{l+k}\partial_iF(x)-\partial_{l+k}\partial_iF(x')|=|\partial_ig_k(\Sigma)-\partial_ig_k(\Sigma')|\le\sqrt{l}\,K_0|\Sigma-\Sigma'|\le\sqrt{l}\,K_0\,\delta\le\frac{\varepsilon}{2}\le\varepsilon ,

and the same bound for il+kF(x)il+kF(x)|\partial_{i'}\partial_{l+k}F(x)-\partial_{i'}\partial_{l+k}F(x')|; here the Taylor lemma is applied to the function igk\partial_ig_k, which is C1C^1 on UU with second partial derivatives of gkg_k as its partial derivatives, all bounded by K0K_0. Finally l+kl+kF\partial_{l+k'}\partial_{l+k}F vanishes identically, so its increment is 0ε0\le\varepsilon. This is requirement 4 of a twice continuously differentiable extension.

The estimates just obtained show in particular that every second partial derivative of FF is continuous on U×VU\times V, so each first partial derivative of FF is a C1C^1 map there. Moreover each first partial derivative of FF is itself continuous: by Step 3(a), the triangle inequality, Cauchy-Schwarz and clause (i) of the Taylor lemma applied to gg and to each gkg_k (all with first partial derivatives bounded by K0K_0 on the convex set UU), together with (0a) and (0c),

iF(x)iF(x)lK0ΣΣ+mlK0ΣΣ(R+1)+mK0αα(lK0(1+m(R+1))+mK0)xx,|\partial_iF(x)-\partial_iF(x')|\le\sqrt{l}\,K_0|\Sigma-\Sigma'|+\sqrt{m}\,\sqrt{l}\,K_0|\Sigma-\Sigma'|(R+1)+\sqrt{m}\,K_0|\alpha-\alpha'|\le\Big(\sqrt{l}\,K_0\big(1+\sqrt{m}(R+1)\big)+\sqrt{m}\,K_0\Big)|x-x'| ,

and l+kF(x)l+kF(x)=gk(Σ)gk(Σ)lK0xx|\partial_{l+k}F(x)-\partial_{l+k}F(x')|=|g_k(\Sigma)-g_k(\Sigma')|\le\sqrt{l}\,K_0|x-x'|. Since all partial derivatives of FF exist on the open set U×VU\times V and are continuous there, FF is a C1C^1 map on U×VU\times V; this is requirement 2.

Step 6. Conclusion (clause 3).

The set UU is open, convex and bounded with ΔlU\Delta^l\subset U by the rate-data definition, and VV is open, convex and bounded with AV\mathcal{A}\subseteq V by Step 2. For (Σ,α)Δl×A(\Sigma,\alpha)\in\Delta^l\times\mathcal{A} the defining formulas for βˉ\bar{\beta} and for β\beta agree, since β0,β1\beta_0,\beta_1 are the restrictions of βˉ0,βˉ1\bar{\beta}_0,\bar{\beta}_1; this is requirement 1. Requirements 2, 3 and 4 were established in Steps 5, 4 and 5 respectively. Hence (U,V,βˉ)(U,V,\bar{\beta}) is a twice continuously differentiable extension of β\beta with derivative bound KK, which is clause 3.

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