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Proof of A C1C^1 Map is Differentiable at Every Point

theoremthm:c1-implies-differentiable-2026a
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Β· 7,965 chars Β· 13 deps Β· depth 9 Reason: Initial publication of the proof that a C^1 map is differentiable: telescoping along coordinate segments, one mean-value point per coordinate, and an epsilon/n estimate against continuity of the partials. Step 3 now fixes the auxiliary radius once as rho=(r-||h||)/2 and derives the bound ||h||+rho<r on the distance from a of every point of the coordinate slice. Claim-9 references point at lem:absolute-value-properties-2026b.

Proof

Let βˆ£β‹…βˆ£|\cdot| be the absolute value, write βˆ‚mf\partial_{m}f for βˆ‚f/βˆ‚xm\partial f/\partial x_{m}, and for z∈Rnz\in\mathbb{R}^{n} write βˆ₯zβˆ₯\lVert z\rVert for the Euclidean distance from zz to the origin, the nonnegative real with βˆ₯zβˆ₯2=βˆ‘i=1nzi2\lVert z\rVert^{2}=\sum_{i=1}^{n}z_{i}^{2}. For z∈Rnz\in\mathbb{R}^{n}, an index mm and u∈Ru\in\mathbb{R}, write z[m:u]z[m{:}u] for the point whose mmth coordinate is uu and whose other coordinates are those of zz. Claim numbers refer to Elementary Order Arithmetic in an Ordered Field and to Properties of the Absolute Value in an Ordered Field as indicated.

As in earlier arguments we use that squares are strictly monotone on nonnegative reals: if 0≀α0\le\alpha, 0≀β0\le\beta and Ξ±<Ξ²\alpha<\beta, then 0<Ξ²0<\beta by claim 2, so Ξ²Ξ±<Ξ²Ξ²\beta\alpha<\beta\beta by claim 10 and αα≀βα\alpha\alpha\le\beta\alpha, whence Ξ±2<Ξ²2\alpha^{2}<\beta^{2} by claim 2; consequently α≀β\alpha\le\beta whenever Ξ±2≀β2\alpha^{2}\le\beta^{2}. In particular ∣ziβˆ£β‰€βˆ₯zβˆ₯|z_{i}|\le\lVert z\rVert for each ii, since zi2≀βˆ₯zβˆ₯2z_{i}^{2}\le\lVert z\rVert^{2} and ∣zi∣2=zi2|z_{i}|^{2}=z_{i}^{2} by claim 4 of Properties of the Absolute Value in an Ordered Field.

Step 1 (a ball inside UU). Since a∈Ua\in U and UU is open, there is rr with 0<r0<r such that every point of Rn\mathbb{R}^{n} at Euclidean distance less than rr from aa lies in UU.

Step 2 (telescoping). Let h=(h1,…,hn)∈Rnh=(h_{1},\dots,h_{n})\in\mathbb{R}^{n} with βˆ₯hβˆ₯<r\lVert h\rVert<r. Define points p0,…,pnp_{0},\dots,p_{n} by p0=ap_{0}=a and pm=pmβˆ’1[m:am+hm]p_{m}=p_{m-1}[m{:}a_{m}+h_{m}] for m∈{1,…,n}m\in\{1,\dots,n\}, so that pmp_{m} has llth coordinate al+hla_{l}+h_{l} for l≀ml\le m and ala_{l} for l>ml>m; in particular pn=a+hp_{n}=a+h.

More generally, for m∈{1,…,n}m\in\{1,\dots,n\} and uu between ama_{m} and am+hma_{m}+h_{m} inclusive, the point pmβˆ’1[m:u]p_{m-1}[m{:}u] differs from aa only in coordinates l≀ml\le m, by hlh_{l} for l<ml<m and by uβˆ’amu-a_{m} for l=ml=m, and ∣uβˆ’amβˆ£β‰€βˆ£hm∣|u-a_{m}|\le|h_{m}|; so the square of its distance to aa is at most βˆ‘lhl2=βˆ₯hβˆ₯2\sum_{l}h_{l}^{2}=\lVert h\rVert^{2}, whence that distance is at most βˆ₯hβˆ₯<r\lVert h\rVert<r and the point lies in UU. In particular every pmp_{m} lies in UU, and

f(a+h)βˆ’f(a)=βˆ‘m=1n(f(pm)βˆ’f(pmβˆ’1)).f(a+h)-f(a)=\sum_{m=1}^{n}\bigl(f(p_{m})-f(p_{m-1})\bigr).

Step 3 (a mean value point in each coordinate). Fix mm. If hm=0h_{m}=0 then pm=pmβˆ’1p_{m}=p_{m-1} and f(pm)βˆ’f(pmβˆ’1)=0=βˆ‚mf(qm)hmf(p_{m})-f(p_{m-1})=0=\partial_{m}f(q_{m})h_{m} with qm=pmβˆ’1q_{m}=p_{m-1}.

Suppose hmβ‰ 0h_{m}\ne0. Since βˆ₯hβˆ₯<r\lVert h\rVert<r, claim 1 gives 0<rβˆ’βˆ₯hβˆ₯0<r-\lVert h\rVert, so by claim 8 the element ρ=(rβˆ’βˆ₯hβˆ₯)β‹…2βˆ’1\rho=\bigl(r-\lVert h\rVert\bigr)\cdot2^{-1} satisfies 0<ρ0<\rho and ρ+ρ=rβˆ’βˆ₯hβˆ₯\rho+\rho=r-\lVert h\rVert, that is βˆ₯hβˆ₯+ρ+ρ=r\lVert h\rVert+\rho+\rho=r; adding βˆ₯hβˆ₯+ρ\lVert h\rVert+\rho to 0<ρ0<\rho gives βˆ₯hβˆ₯+ρ<r\lVert h\rVert+\rho<r, again by claim 1. Let JJ be the open interval consisting of those uu with amβˆ’(∣hm∣+ρ)<ua_{m}-\bigl(|h_{m}|+\rho\bigr)<u and u<am+(∣hm∣+ρ)u<a_{m}+\bigl(|h_{m}|+\rho\bigr).

Let u∈Ju\in J. Adding βˆ’am-a_{m} to both inequalities, claim 1 gives βˆ’(∣hm∣+ρ)<uβˆ’am-\bigl(|h_{m}|+\rho\bigr)<u-a_{m} and uβˆ’am<∣hm∣+ρu-a_{m}<|h_{m}|+\rho, so ∣uβˆ’am∣<∣hm∣+ρ|u-a_{m}|<|h_{m}|+\rho by claim 9 of Properties of the Absolute Value in an Ordered Field. The point pmβˆ’1[m:u]p_{m-1}[m{:}u] agrees with aa in the coordinates l>ml>m and differs from it by hlh_{l} in the coordinates l<ml<m and by uβˆ’amu-a_{m} in the coordinate mm; hence the square of its Euclidean distance to aa equals βˆ‘l<mhl2+(uβˆ’am)2\sum_{l<m}h_{l}^{2}+(u-a_{m})^{2}. Here βˆ‘l<mhl2≀βˆ₯hβˆ₯2βˆ’hm2\sum_{l<m}h_{l}^{2}\le\lVert h\rVert^{2}-h_{m}^{2}, since the omitted terms hl2h_{l}^{2} with l>ml>m are nonnegative, and (uβˆ’am)2=∣uβˆ’am∣2≀(∣hm∣+ρ)2(u-a_{m})^{2}=|u-a_{m}|^{2}\le\bigl(|h_{m}|+\rho\bigr)^{2} by claim 4 of that lemma and the monotonicity of squares. Moreover ∣hmβˆ£Οβ‰€βˆ₯hβˆ₯ρ|h_{m}|\rho\le\lVert h\rVert\rho: this is claim 10 when ∣hm∣<βˆ₯hβˆ₯|h_{m}|<\lVert h\rVert, and an equality when ∣hm∣=βˆ₯hβˆ₯|h_{m}|=\lVert h\rVert. Using ∣hm∣2=hm2|h_{m}|^{2}=h_{m}^{2}, again by claim 4, we get

βˆ‘l<mhl2+(uβˆ’am)2≀βˆ₯hβˆ₯2βˆ’hm2+(∣hm∣+ρ)2=βˆ₯hβˆ₯2+∣hm∣ρ+∣hm∣ρ+ρ2≀(βˆ₯hβˆ₯+ρ)2.\sum_{l<m}h_{l}^{2}+(u-a_{m})^{2}\le\lVert h\rVert^{2}-h_{m}^{2}+\bigl(|h_{m}|+\rho\bigr)^{2}=\lVert h\rVert^{2}+|h_{m}|\rho+|h_{m}|\rho+\rho^{2}\le\bigl(\lVert h\rVert+\rho\bigr)^{2}.

By the monotonicity of squares the distance from pmβˆ’1[m:u]p_{m-1}[m{:}u] to aa is therefore at most βˆ₯hβˆ₯+ρ\lVert h\rVert+\rho, hence less than rr; so pmβˆ’1[m:u]∈Up_{m-1}[m{:}u]\in U for every u∈Ju\in J.

Let G:Jβ†’RG:J\to\mathbb{R} be given by G(u)=f(pmβˆ’1[m:u])G(u)=f\bigl(p_{m-1}[m{:}u]\bigr). For each u0∈Ju_{0}\in J, apply Slice Function and the Partial Derivative to ff at the point pmβˆ’1[m:u0]p_{m-1}[m{:}u_{0}] of UU in the mmth variable: it gives a positive radius ρ0\rho_{0} and identifies the slice function on (u0βˆ’Ο0,u0+ρ0)(u_{0}-\rho_{0},u_{0}+\rho_{0}), which agrees with GG there, as differentiable at u0u_{0} with derivative βˆ‚mf(pmβˆ’1[m:u0])\partial_{m}f\bigl(p_{m-1}[m{:}u_{0}]\bigr), the partial derivative existing because ff is of class C1C^{1}. By An Open Interval is an Interval All of Whose Points Are Interior both intervals have all points interior, so shrinking the Ξ΄\delta in the defining condition confines the increments to the overlap, where the two functions agree; hence GG is differentiable at u0u_{0} with Gβ€²(u0)=βˆ‚mf(pmβˆ’1[m:u0])G'(u_{0})=\partial_{m}f\bigl(p_{m-1}[m{:}u_{0}]\bigr).

Both ama_{m} and am+hma_{m}+h_{m} lie in JJ: indeed 0β‰€βˆ£hm∣0\le|h_{m}| and 0<ρ0<\rho give 0<∣hm∣+ρ0<|h_{m}|+\rho and ∣hm∣<∣hm∣+ρ|h_{m}|<|h_{m}|+\rho by claim 1, so claim 9 of Properties of the Absolute Value in an Ordered Field, applied to 00 and to hmh_{m} with c=∣hm∣+ρc=|h_{m}|+\rho, yields the two pairs of strict inequalities required. Applying Mean Value Theorem on an Open Interval to GG on JJ with these two points in increasing order yields ΞΎm\xi_{m} strictly between them with G(am+hm)βˆ’G(am)=Gβ€²(ΞΎm)hmG(a_{m}+h_{m})-G(a_{m})=G'(\xi_{m})h_{m}, that is, with qm=pmβˆ’1[m:ΞΎm]q_{m}=p_{m-1}[m{:}\xi_{m}],

f(pm)βˆ’f(pmβˆ’1)=βˆ‚mf(qm) hm.f(p_{m})-f(p_{m-1})=\partial_{m}f(q_{m})\,h_{m}.

Since ∣ξmβˆ’am∣<∣hm∣|\xi_{m}-a_{m}|<|h_{m}|, Step 2 shows qmq_{m} is at distance at most βˆ₯hβˆ₯\lVert h\rVert from aa.

Step 4 (the estimate). Combining Steps 2 and 3,

f(a+h)βˆ’f(a)βˆ’βˆ‘m=1nβˆ‚mf(a)hm=βˆ‘m=1n(βˆ‚mf(qm)βˆ’βˆ‚mf(a))hm.f(a+h)-f(a)-\sum_{m=1}^{n}\partial_{m}f(a)h_{m}=\sum_{m=1}^{n}\bigl(\partial_{m}f(q_{m})-\partial_{m}f(a)\bigr)h_{m}.

Let Ρ∈R\varepsilon\in\mathbb{R} with 0<Ξ΅0<\varepsilon. Since nβ‰₯1n\ge1, the element nn, a sum of copies of 11, is positive by claims 6 and 3, so Ξ΅β€²=Ρ nβˆ’1\varepsilon'=\varepsilon\,n^{-1} is positive by claims 7 and 5. Each βˆ‚mf\partial_{m}f is continuous at aa, by the definition of class C1C^{1}; taking the least of the finitely many radii by repeated use of claim 9, there is ΞΈ\theta with 0<ΞΈ0<\theta such that every z∈Uz\in U at distance less than ΞΈ\theta from aa satisfies βˆ£βˆ‚mf(z)βˆ’βˆ‚mf(a)∣<Ξ΅β€²|\partial_{m}f(z)-\partial_{m}f(a)|<\varepsilon' for every mm.

Let Ξ΄\delta be the least, by claim 9, of rr and ΞΈ\theta, so 0<Ξ΄0<\delta. Suppose h∈Rnh\in\mathbb{R}^{n} satisfies 0<βˆ‘ihi2<Ξ΄20<\sum_{i}h_{i}^{2}<\delta^{2} and a+h∈Ua+h\in U. Then βˆ₯hβˆ₯<Ξ΄\lVert h\rVert<\delta by the monotonicity of squares, so βˆ₯hβˆ₯<r\lVert h\rVert<r and Steps 2 and 3 apply, and each qmq_{m} is at distance at most βˆ₯hβˆ₯<ΞΈ\lVert h\rVert<\theta from aa, so βˆ£βˆ‚mf(qm)βˆ’βˆ‚mf(a)∣<Ξ΅β€²|\partial_{m}f(q_{m})-\partial_{m}f(a)|<\varepsilon'.

Writing cm=βˆ‚mf(qm)βˆ’βˆ‚mf(a)c_{m}=\partial_{m}f(q_{m})-\partial_{m}f(a) and using claim 5 of Properties of the Absolute Value in an Ordered Field repeatedly, then claim 4 of that lemma and claim 10 together with ∣hmβˆ£β‰€βˆ₯hβˆ₯|h_{m}|\le\lVert h\rVert,

βˆ£βˆ‘m=1ncmhmβˆ£β‰€βˆ‘m=1n∣cmβˆ£β€‰βˆ£hmβˆ£β‰€βˆ‘m=1nΞ΅β€²βˆ₯hβˆ₯=n Ρ′βˆ₯hβˆ₯=Ρ βˆ₯hβˆ₯.\Bigl|\sum_{m=1}^{n}c_{m}h_{m}\Bigr|\le\sum_{m=1}^{n}|c_{m}|\,|h_{m}|\le\sum_{m=1}^{n}\varepsilon'\lVert h\rVert=n\,\varepsilon'\lVert h\rVert=\varepsilon\,\lVert h\rVert .

Both sides are nonnegative, so squaring and using claim 4 of Properties of the Absolute Value in an Ordered Field and the monotonicity of squares,

(f(a+h)βˆ’f(a)βˆ’βˆ‘m=1nβˆ‚mf(a)hm)2≀Ρ2βˆ₯hβˆ₯2=Ξ΅2βˆ‘i=1nhi2.\Bigl(f(a+h)-f(a)-\sum_{m=1}^{n}\partial_{m}f(a)h_{m}\Bigr)^{2}\le\varepsilon^{2}\lVert h\rVert^{2}=\varepsilon^{2}\sum_{i=1}^{n}h_{i}^{2}.

This is exactly the defining condition of differentiability of ff at aa, with m=1m=1 there, the required partial derivatives existing because ff is of class C1C^{1}.

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