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

lemmalem:affine-c2-extension-2026b
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Reason: Carried onto lem:affine-c2-extension-2026b and re-grounded on the new Euclidean layer. Step 3 now derives the partial derivatives of the extension directly from def:partial-derivative-euclidean-2026a, replacing the withdrawn slice-function lemma; Step 5 additionally establishes continuity of the extension and of its first partial derivatives, as clause 1 of def:ck-map-euclidean-2026a requires; the ad-hoc openness argument for U x V is replaced by lem:euclidean-open-product-2026a, and the Taylor citation bumped to lem:taylor-second-order-uniform-2026b.

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 of class C2C^2 on UU — by clauses 2 and 3 of that definition this means that each is of class C1C^1 on UU and that each of its partial derivatives i\partial_i, unambiguous by Uniqueness of the Partial Derivative on a Euclidean Open Set, is again of class 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) Once VV is known to be open (Step 2), U×VU\times V is an open subset of Rl+m\mathbb{R}^{l+m} by claim 2 of Products of Euclidean Open Sets are Open, the identification of Rl×Rm\mathbb{R}^l\times\mathbb{R}^m with Rl+m\mathbb{R}^{l+m} being the one fixed in the statement.

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.

Admissible increments. By (0d) the set U×VU\times V is open, so there is a real r>0r>0 such that every yRl+my\in\mathbb{R}^{l+m} with k=1l+m(ykxk)2<r2\sum_{k=1}^{l+m}(y_k-x_k)^2<r^2 lies in U×VU\times V. For j{1,,l+m}j\in\{1,\dots,l+m\} and real hh write x(j,h)x^{(j,h)} for the point obtained from xx by replacing its jjth coordinate xjx_j by xj+hx_j+h; then k(xk(j,h)xk)2=h2\sum_{k}(x^{(j,h)}_k-x_k)^2=h^2, so every real hh with h<r|h|<r has x(j,h)U×Vx^{(j,h)}\in U\times V, by clause 2 of monotonicity of squaring.

(a) State coordinates. Fix i{1,,l}i\in\{1,\dots,l\}, and note that for real hh the point x(i,h)x^{(i,h)} is (Σ(h),α)(\Sigma^{(h)},\alpha), where Σ(h)Rl\Sigma^{(h)}\in\mathbb{R}^l is obtained from Σ\Sigma by replacing Σi\Sigma^i by Σi+h\Sigma^i+h; in particular the control coordinates are unchanged. Since gg and each gkg_k are of class C1C^1 on the open set UU, their partial derivatives with respect to the iith variable exist at Σ\Sigma. Put

L=ig(Σ)+k=1mαkigk(Σ),C=1+k=1mαk,L=\partial_ig(\Sigma)+\sum_{k=1}^m\alpha^k\,\partial_ig_k(\Sigma),\qquad C=1+\sum_{k=1}^m|\alpha^k| ,

so that C1>0C\ge1>0. Let ε>0\varepsilon>0 be real and put ε=ε(2C)1\varepsilon'=\varepsilon\cdot(2C)^{-1}, positive by claims 5, 7 and 8 of the order arithmetic of an ordered field. By the definition of the partial derivative there are reals δ0,δ1,,δm>0\delta_0,\delta_1,\dots,\delta_m>0 such that every real hh with 0<h<δ00<|h|<\delta_0 satisfies Σ(h)U\Sigma^{(h)}\in U and

g(Σ(h))g(Σ)hig(Σ)<ε,\left|\frac{g(\Sigma^{(h)})-g(\Sigma)}{h}-\partial_ig(\Sigma)\right|<\varepsilon' ,

and, for each k{1,,m}k\in\{1,\dots,m\}, every real hh with 0<h<δk0<|h|<\delta_k satisfies Σ(h)U\Sigma^{(h)}\in U and the same inequality with gg and ig(Σ)\partial_ig(\Sigma) replaced by gkg_k and igk(Σ)\partial_ig_k(\Sigma). Let δ\delta be the least of the finitely many positive reals r,δ0,δ1,,δmr,\delta_0,\delta_1,\dots,\delta_m, obtained by repeated application of claim 9 of that lemma, so that δ>0\delta>0. For real hh with 0<h<δ0<|h|<\delta we then have x(i,h)U×Vx^{(i,h)}\in U\times V, and, the control coordinates of x(i,h)x^{(i,h)} and xx agreeing,

F(x(i,h))F(x)hL=(g(Σ(h))g(Σ)hig(Σ))+k=1mαk(gk(Σ(h))gk(Σ)higk(Σ)),\frac{F(x^{(i,h)})-F(x)}{h}-L=\left(\frac{g(\Sigma^{(h)})-g(\Sigma)}{h}-\partial_ig(\Sigma)\right)+\sum_{k=1}^m\alpha^k\left(\frac{g_k(\Sigma^{(h)})-g_k(\Sigma)}{h}-\partial_ig_k(\Sigma)\right),

whose modulus is at most ε+k=1mαkε=Cε=ε21<ε\varepsilon'+\sum_{k=1}^m|\alpha^k|\,\varepsilon'=C\varepsilon'=\varepsilon\cdot2^{-1}<\varepsilon, by claim 5 of the properties of the absolute value in an ordered field (the triangle inequality, extended to the m+1m+1 summands by induction on their number) together with claim 4 of that lemma (multiplicativity), and by claim 8 of the order lemma. As ε>0\varepsilon>0 was arbitrary, the partial derivative of FF with respect to the iith variable exists at xx with value LL, and by Uniqueness of the Partial Derivative on a Euclidean Open Set no other value is possible:

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\}. For real hh with 0<h<r0<|h|<r the point x(l+k,h)x^{(l+k,h)} lies in U×VU\times V and differs from xx only in the control coordinate αk\alpha^k, which is replaced by αk+h\alpha^k+h; hence

F(x(l+k,h))F(x)h=gk(Σ)hh=gk(Σ),\frac{F(x^{(l+k,h)})-F(x)}{h}=\frac{g_k(\Sigma)\,h}{h}=g_k(\Sigma),

so the difference quotient is exactly gk(Σ)g_k(\Sigma) and its distance to gk(Σ)g_k(\Sigma) is 0<ε0<\varepsilon for every real ε>0\varepsilon>0. Therefore the partial derivative of FF with respect to the (l+k)(l+k)th variable exists at xx with value gk(Σ)g_k(\Sigma), and 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 of class C1C^1 on UU because gg and the gkg_k are of class C2C^2 there. 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 difference quotients in any control coordinate xl+kx_{l+k'} all vanish, giving l+kl+kF=0\partial_{l+k'}\partial_{l+k}F=0, the second identity of clause 4; and the argument of (a), applied to the single function gkg_k 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 at every point of U×VU\times V: given a real ε>0\varepsilon>0, the bound just proved, applied with ε21\varepsilon\cdot2^{-1} in place of ε\varepsilon, supplies a real δ>0\delta>0 such that any two points of U×VU\times V at distance at most δ\delta have their second partial derivatives of FF within ε21<ε\varepsilon\cdot2^{-1}<\varepsilon of each other, by claim 8 of the order arithmetic of an ordered field. Each first partial derivative of FF is continuous as well: 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'|. Each of these two bounds has the form jF(x)jF(x)C1xx|\partial_jF(x)-\partial_jF(x')|\le C_1|x-x'| with a nonnegative real constant C1C_1, so for a real ε>0\varepsilon>0 the choice δ=ε(2(C1+1))1\delta=\varepsilon\cdot\big(2(C_1+1)\big)^{-1} makes the left-hand side smaller than ε\varepsilon whenever xx<δ|x-x'|<\delta; hence every jF\partial_jF is continuous at every point of U×VU\times V.

The function FF itself is continuous there too. Writing

F(x)F(x)=(g(Σ)g(Σ))+k=1m(gk(Σ)gk(Σ))αk+k=1mgk(Σ)(αkαk)F(x)-F(x')=\big(g(\Sigma)-g(\Sigma')\big)+\sum_{k=1}^m\big(g_k(\Sigma)-g_k(\Sigma')\big)\alpha^k+\sum_{k=1}^mg_k(\Sigma')\big(\alpha^k-\alpha'^k\big)

and bounding the first group by clause (i) of the Taylor lemma, the second by Cauchy-Schwarz together with (0a), that same clause and αR+1|\alpha|\le R+1, and the third by Cauchy-Schwarz together with (0a) and gkK0|g_k|\le K_0, we obtain from (0c)

F(x)F(x)(lK0(1+m(R+1))+mK0)xx,|F(x)-F(x')|\le\Big(\sqrt{l}\,K_0\big(1+\sqrt{m}\,(R+1)\big)+\sqrt{m}\,K_0\Big)|x-x'| ,

and the same choice of δ\delta as above applies.

So FF is continuous at every point of the open set U×VU\times V and all of its partial derivatives exist and are continuous there, which by clauses 1 and 3 of the definition of a CkC^k map makes FF of class C1C^1 on U×VU\times V; and each jF\partial_jF is likewise continuous with all of its own partial derivatives existing and continuous, hence of class C1C^1 on U×VU\times V. By clause 2 of that definition, FF is of class C2C^2 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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