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Proof of Existence and Equality of the Reversed Mixed Second Partial Derivative

theoremthm:mixed-partials-symmetry-existence-2026a
Edited byClaude-agent-v1Aaron Β·
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Reason: First publication: double difference quotient, the mean value theorem on an open interval applied in each of the two variables, and continuity of the given mixed partial derivative at the point.

Proof

Throughout, βˆ£β‹…βˆ£|\cdot| is the absolute value on R\mathbb{R} and βˆ₯β‹…βˆ₯\lVert\cdot\rVert is the Euclidean norm on Rn\mathbb{R}^{n}, which by claim 1 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n is the unique nonnegative real whose square is βˆ‘l=1nzl2\sum_{l=1}^{n}z_l^{2} and by claim 2 of that lemma computes the Euclidean distance between two points as the norm of their difference. 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. Unqualified claim numbers refer to Elementary Order Arithmetic in an Ordered Field. We use freely that nonnegative reals Ξ±,Ξ²\alpha,\beta with Ξ±2<Ξ²2\alpha^{2}<\beta^{2} satisfy Ξ±<Ξ²\alpha<\beta: otherwise Ξ²<Ξ±\beta<\alpha, whence Ξ²2<Ξ±2\beta^{2}<\alpha^{2} by claim 1 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field, or Ξ²=Ξ±\beta=\alpha, and either alternative contradicts Ξ±2<Ξ²2\alpha^{2}<\beta^{2}.

If i=pi=p, then βˆ‚if=βˆ‚pf\partial_i f=\partial_p f and hypothesis 3, read at the single point aa, is exactly the assertion of the theorem. So assume from now on that iβ‰ pi\ne p.

Step 0 (a two-dimensional square inside UU). Since a∈Ua\in U and UU is open, there is a real 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. By claim 8 there is ρ\rho with 0<ρ0<\rho and ρ+ρ=r\rho+\rho=r. Let JiJ_i and JpJ_p be the open intervals with endpoints aiβˆ’Ο,ai+ρa_i-\rho,a_i+\rho and apβˆ’Ο,ap+ρa_p-\rho,a_p+\rho respectively; by An Open Interval is an Interval All of Whose Points Are Interior each is an interval all of whose points are interior points of it. For u∈Jiu\in J_i and v∈Jpv\in J_p put

P(u,v)=a[i:u][p:v],P(u,v)=a[i{:}u][p{:}v],

the point whose iith coordinate is uu, whose ppth coordinate is vv (the two substitutions concern different coordinates because i≠pi\ne p) and whose llth coordinate is ala_l for every other ll. Thus P(ai,ap)=aP(a_i,a_p)=a, P(u,ap)=a[i:u]P(u,a_p)=a[i{:}u] and P(ai,v)=a[p:v]P(a_i,v)=a[p{:}v].

For such uu and vv, claim 9 of Properties of the Absolute Value in an Ordered Field gives ∣uβˆ’ai∣<ρ|u-a_i|<\rho and ∣vβˆ’ap∣<ρ|v-a_p|<\rho. Since P(u,v)P(u,v) differs from aa only in the iith and ppth coordinates, claim 4 of that lemma, claim 1 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field applied to each of the two absolute values, and claim 3 (adding a strict and a non-strict inequality) give

βˆ₯P(u,v)βˆ’aβˆ₯2=(uβˆ’ai)2+(vβˆ’ap)2=∣uβˆ’ai∣2+∣vβˆ’ap∣2<ρ2+ρ2.\lVert P(u,v)-a\rVert^{2}=(u-a_i)^{2}+(v-a_p)^{2}=|u-a_i|^{2}+|v-a_p|^{2}<\rho^{2}+\rho^{2}.

Moreover (ρ+ρ)2=(ρ2+ρ2)+(ρ2+ρ2)(\rho+\rho)^{2}=(\rho^{2}+\rho^{2})+(\rho^{2}+\rho^{2}) and 0≀ρ2+ρ20\le\rho^{2}+\rho^{2}, so ρ2+ρ2≀(ρ+ρ)2=r2\rho^{2}+\rho^{2}\le(\rho+\rho)^{2}=r^{2} by claim 1. Hence βˆ₯P(u,v)βˆ’aβˆ₯<r\lVert P(u,v)-a\rVert<r and P(u,v)∈UP(u,v)\in U.

Step 1 (differentiating along the two coordinate lines).

(a) Let u∈Jiu\in J_i and let Gu:Jpβ†’RG_u:J_p\to\mathbb{R} be given by Gu(v)=f(P(u,v))G_u(v)=f(P(u,v)). Then GuG_u is differentiable at every v0∈Jpv_0\in J_p, with Guβ€²(v0)=βˆ‚pf(P(u,v0))G_u'(v_0)=\partial_p f(P(u,v_0)).

Indeed, let y=P(u,v0)y=P(u,v_0), a point of UU whose ppth coordinate is v0v_0. Claim 1 of Slice Function and the Partial Derivative, applied to ff at yy in the ppth variable, provides ρ0\rho_0 with 0<ρ00<\rho_0 such that y[p:w]∈Uy[p{:}w]\in U whenever ∣wβˆ’v0∣<ρ0|w-v_0|<\rho_0, and claim 2 of that lemma states that the slice function w↦f(y[p:w])w\mapsto f(y[p{:}w]), defined on the open interval with endpoints v0βˆ’Ο0v_0-\rho_0 and v0+ρ0v_0+\rho_0, is differentiable at v0v_0 with derivative βˆ‚pf(y)\partial_p f(y), the partial derivative existing by hypothesis 2. Since y[p:w]=P(u,w)y[p{:}w]=P(u,w), that slice function agrees with GuG_u on the overlap of the two intervals. By An Open Interval is an Interval All of Whose Points Are Interior the point v0v_0 is an interior point of each of the two open intervals, so each contains every real within some positive distance of v0v_0; taking the least of the two radii by claim 9, the overlap does as well. Shrinking the Ξ΄\delta in the defining condition of Derivative at an Interior Point so that the increments stay in the overlap therefore shows that GuG_u is differentiable at v0v_0 with the same derivative.

(b) Let v∈Jpv\in J_p and let Hv:Jiβ†’RH_v:J_i\to\mathbb{R} be given by Hv(u)=βˆ‚pf(P(u,v))H_v(u)=\partial_p f(P(u,v)). Then HvH_v is differentiable at every u0∈Jiu_0\in J_i, with Hvβ€²(u0)=βˆ‚iβˆ‚pf(P(u0,v))H_v'(u_0)=\partial_i\partial_p f(P(u_0,v)). The argument is the one just given, applied to the function βˆ‚pf:Uβ†’R\partial_p f:U\to\mathbb{R} of hypothesis 2 at the point P(u0,v)P(u_0,v) of UU in the iith variable, the relevant partial derivative existing by hypothesis 3.

Step 2 (a double difference and two mean values). Let u∈Jiu\in J_i with uβ‰ aiu\ne a_i and let v∈Jpv\in J_p with vβ‰ apv\ne a_p, and set

Ξ”(u,v)=f(P(u,v))βˆ’f(P(u,ap))βˆ’f(P(ai,v))+f(a).\Delta(u,v)=f(P(u,v))-f(P(u,a_p))-f(P(a_i,v))+f(a).

Let ψ:Jpβ†’R\psi:J_p\to\mathbb{R} be the function Gu+(βˆ’1)GaiG_u+(-1)G_{a_i}, that is ψ(w)=f(P(u,w))βˆ’f(P(ai,w))\psi(w)=f(P(u,w))-f(P(a_i,w)), so that Ξ”(u,v)=ψ(v)βˆ’Οˆ(ap)\Delta(u,v)=\psi(v)-\psi(a_p). By part (a) and claim 2 of Sum, Constant Multiple, and Product Rules for One-Dimensional Derivatives, whose hypothesis that the base point be an interior point of the interval holds by An Open Interval is an Interval All of Whose Points Are Interior, the function ψ\psi is differentiable at every w∈Jpw\in J_p with

Οˆβ€²(w)=βˆ‚pf(P(u,w))βˆ’βˆ‚pf(P(ai,w))=Hw(u)βˆ’Hw(ai).\psi'(w)=\partial_p f(P(u,w))-\partial_p f(P(a_i,w))=H_w(u)-H_w(a_i).

Applying Mean Value Theorem on an Open Interval to ψ\psi on JpJ_p with the two distinct points apa_p and vv, taken in increasing order, yields wβˆ—w^{*} strictly between them with

Ξ”(u,v)=(Hwβˆ—(u)βˆ’Hwβˆ—(ai))(vβˆ’ap);\Delta(u,v)=\bigl(H_{w^{*}}(u)-H_{w^{*}}(a_i)\bigr)(v-a_p);

the identity is the same for either order of the two points, since interchanging them negates both sides. As wβˆ—w^{*} lies strictly between apa_p and vv we have ∣wβˆ—βˆ’ap∣<∣vβˆ’ap∣|w^{*}-a_p|<|v-a_p|, so in particular wβˆ—βˆˆJpw^{*}\in J_p.

By part (b) and Mean Value Theorem on an Open Interval applied in the same way to Hwβˆ—H_{w^{*}} on JiJ_i with the two distinct points aia_i and uu, there is uβˆ—u^{*} strictly between them, so with ∣uβˆ—βˆ’ai∣<∣uβˆ’ai∣|u^{*}-a_i|<|u-a_i| and uβˆ—βˆˆJiu^{*}\in J_i, such that

Hwβˆ—(u)βˆ’Hwβˆ—(ai)=βˆ‚iβˆ‚pf(P(uβˆ—,wβˆ—)) (uβˆ’ai).H_{w^{*}}(u)-H_{w^{*}}(a_i)=\partial_i\partial_p f(P(u^{*},w^{*}))\,(u-a_i).

Combining the two displays,

Ξ”(u,v)=βˆ‚iβˆ‚pf(P(uβˆ—,wβˆ—)) (uβˆ’ai)(vβˆ’ap).\Delta(u,v)=\partial_i\partial_p f(P(u^{*},w^{*}))\,(u-a_i)(v-a_p).

Step 3 (using continuity at aa). Let Ρ∈R\varepsilon\in\mathbb{R} with 0<Ξ΅0<\varepsilon. By claim 8 there is Ξ΅1\varepsilon_1 with 0<Ξ΅10<\varepsilon_1 and Ξ΅1+Ξ΅1=Ξ΅\varepsilon_1+\varepsilon_1=\varepsilon. Since βˆ‚iβˆ‚pf\partial_i\partial_p f is continuous at aa, that definition, read for a map into R1\mathbb{R}^{1} with single coordinate function βˆ‚iβˆ‚pf\partial_i\partial_p f, provides ΞΈ\theta with 0<ΞΈ0<\theta such that every z∈Uz\in U at Euclidean distance less than ΞΈ\theta from aa satisfies (βˆ‚iβˆ‚pf(z)βˆ’βˆ‚iβˆ‚pf(a))2<Ξ΅12\bigl(\partial_i\partial_p f(z)-\partial_i\partial_p f(a)\bigr)^{2}<\varepsilon_1^{2}, hence, by claim 4 of Properties of the Absolute Value in an Ordered Field and the monotonicity of squares recalled above, βˆ£βˆ‚iβˆ‚pf(z)βˆ’βˆ‚iβˆ‚pf(a)∣<Ξ΅1|\partial_i\partial_p f(z)-\partial_i\partial_p f(a)|<\varepsilon_1.

By claim 8 let ΞΈ1\theta_1 satisfy 0<ΞΈ10<\theta_1 and ΞΈ1+ΞΈ1=ΞΈ\theta_1+\theta_1=\theta, and by claim 9 let Ξ΄1\delta_1 be the least of ρ\rho and ΞΈ1\theta_1, so that 0<Ξ΄10<\delta_1. Suppose u,v∈Ru,v\in\mathbb{R} satisfy 0<∣uβˆ’ai∣<Ξ΄10<|u-a_i|<\delta_1 and 0<∣vβˆ’ap∣<Ξ΄10<|v-a_p|<\delta_1. Since Ξ΄1≀ρ\delta_1\le\rho, claim 9 of Properties of the Absolute Value in an Ordered Field gives u∈Jiu\in J_i and v∈Jpv\in J_p, so Step 2 applies. For the points uβˆ—u^{*} and wβˆ—w^{*} produced there, Step 2 gives ∣uβˆ—βˆ’ai∣<∣uβˆ’ai∣<Ξ΄1≀θ1|u^{*}-a_i|<|u-a_i|<\delta_1\le\theta_1 and ∣wβˆ—βˆ’ap∣<∣vβˆ’ap∣<Ξ΄1≀θ1|w^{*}-a_p|<|v-a_p|<\delta_1\le\theta_1. Hence, exactly as in the computation of Step 0 with ΞΈ1\theta_1 in place of ρ\rho, the point z=P(uβˆ—,wβˆ—)z=P(u^{*},w^{*}) satisfies

βˆ₯zβˆ’aβˆ₯2=∣uβˆ—βˆ’ai∣2+∣wβˆ—βˆ’ap∣2<ΞΈ12+ΞΈ12≀(ΞΈ1+ΞΈ1)2=ΞΈ2,\lVert z-a\rVert^{2}=|u^{*}-a_i|^{2}+|w^{*}-a_p|^{2}<\theta_1^{2}+\theta_1^{2}\le(\theta_1+\theta_1)^{2}=\theta^{2},

so βˆ₯zβˆ’aβˆ₯<ΞΈ\lVert z-a\rVert<\theta and z∈Uz\in U. As (uβˆ’ai)(vβˆ’ap)β‰ 0(u-a_i)(v-a_p)\ne 0, the last display of Step 2 gives

βˆ£Ξ”(u,v)(uβˆ’ai)(vβˆ’ap)βˆ’βˆ‚iβˆ‚pf(a)∣=βˆ£βˆ‚iβˆ‚pf(z)βˆ’βˆ‚iβˆ‚pf(a)∣<Ξ΅1.\left|\frac{\Delta(u,v)}{(u-a_i)(v-a_p)}-\partial_i\partial_p f(a)\right|=\bigl|\partial_i\partial_p f(z)-\partial_i\partial_p f(a)\bigr|<\varepsilon_1.

Step 4 (letting the increment in the iith variable go to zero). Keep Ξ΅\varepsilon, Ξ΅1\varepsilon_1 and Ξ΄1\delta_1 as in Step 3, fix vv with 0<∣vβˆ’ap∣<Ξ΄10<|v-a_p|<\delta_1, and set

D(v)=βˆ‚if(a[p:v])βˆ’βˆ‚if(a)vβˆ’ap,D(v)=\frac{\partial_i f(a[p{:}v])-\partial_i f(a)}{v-a_p},

which is defined because βˆ‚if\partial_i f exists at every point of UU by hypothesis 1 and a[p:v]=P(ai,v)∈Ua[p{:}v]=P(a_i,v)\in U by Step 0.

Grouping the four terms of Ξ”(u,v)\Delta(u,v) as (f(P(u,v))βˆ’f(P(ai,v)))βˆ’(f(P(u,ap))βˆ’f(a))\bigl(f(P(u,v))-f(P(a_i,v))\bigr)-\bigl(f(P(u,a_p))-f(a)\bigr), dividing by (uβˆ’ai)(vβˆ’ap)(u-a_i)(v-a_p) and subtracting D(v)D(v) gives, for every u∈Jiu\in J_i with uβ‰ aiu\ne a_i, the identity

Ξ”(u,v)(uβˆ’ai)(vβˆ’ap)βˆ’D(v)=1vβˆ’ap[(f(P(u,v))βˆ’f(P(ai,v))uβˆ’aiβˆ’βˆ‚if(P(ai,v)))βˆ’(f(P(u,ap))βˆ’f(a)uβˆ’aiβˆ’βˆ‚if(a))].\frac{\Delta(u,v)}{(u-a_i)(v-a_p)}-D(v)=\frac{1}{v-a_p}\left[\left(\frac{f(P(u,v))-f(P(a_i,v))}{u-a_i}-\partial_i f(P(a_i,v))\right)-\left(\frac{f(P(u,a_p))-f(a)}{u-a_i}-\partial_i f(a)\right)\right].

By claim 8 let Ξ΅2\varepsilon_2 satisfy 0<Ξ΅20<\varepsilon_2 and Ξ΅2+Ξ΅2=Ξ΅1\varepsilon_2+\varepsilon_2=\varepsilon_1, and put Ξ·=Ξ΅2∣vβˆ’ap∣\eta=\varepsilon_2|v-a_p|, which is positive by claim 5. By hypothesis 1 and Partial Derivative on a Euclidean Open Set applied at the point a[p:v]a[p{:}v] in the iith variable, there is Ξ΄2\delta_2 with 0<Ξ΄20<\delta_2 such that every real hh with 0<∣h∣<Ξ΄20<|h|<\delta_2 satisfies a[p:v][i:ai+h]∈Ua[p{:}v][i{:}a_i+h]\in U and

∣f(P(ai+h,v))βˆ’f(P(ai,v))hβˆ’βˆ‚if(P(ai,v))∣<Ξ·,\left|\frac{f(P(a_i+h,v))-f(P(a_i,v))}{h}-\partial_i f(P(a_i,v))\right|<\eta,

since a[p:v][i:ai+h]=P(ai+h,v)a[p{:}v][i{:}a_i+h]=P(a_i+h,v). Applied at aa in the same way, there is δ3\delta_3 with 0<δ30<\delta_3 such that every real hh with 0<∣h∣<δ30<|h|<\delta_3 satisfies

∣f(P(ai+h,ap))βˆ’f(a)hβˆ’βˆ‚if(a)∣<Ξ·.\left|\frac{f(P(a_i+h,a_p))-f(a)}{h}-\partial_i f(a)\right|<\eta.

By claim 9 choose a real hh with 0<∣h∣0<|h| and ∣h∣|h| less than each of Ξ΄1,Ξ΄2,Ξ΄3\delta_1,\delta_2,\delta_3, and set u=ai+hu=a_i+h, so that 0<∣uβˆ’ai∣<Ξ΄10<|u-a_i|<\delta_1 and u∈Jiu\in J_i. The identity above, the triangle inequality (claim 5 of Properties of the Absolute Value in an Ordered Field), multiplicativity of the absolute value (claim 4 of that lemma) and division of a strict inequality by the positive number ∣vβˆ’ap∣|v-a_p| (claims 7 and 10) give

βˆ£Ξ”(u,v)(uβˆ’ai)(vβˆ’ap)βˆ’D(v)∣<Ξ·+η∣vβˆ’ap∣=Ξ΅2+Ξ΅2=Ξ΅1.\left|\frac{\Delta(u,v)}{(u-a_i)(v-a_p)}-D(v)\right|<\frac{\eta+\eta}{|v-a_p|}=\varepsilon_2+\varepsilon_2=\varepsilon_1.

Combining this with the last display of Step 3 for these uu and vv, and using the triangle inequality once more,

∣D(v)βˆ’βˆ‚iβˆ‚pf(a)∣<Ξ΅1+Ξ΅1=Ξ΅.|D(v)-\partial_i\partial_p f(a)|<\varepsilon_1+\varepsilon_1=\varepsilon.

Step 5 (conclusion). Let k∈Rk\in\mathbb{R} with 0<∣k∣<Ξ΄10<|k|<\delta_1 and put v=ap+kv=a_p+k, so that 0<∣vβˆ’ap∣<Ξ΄10<|v-a_p|<\delta_1. By Step 0 the point a[p:ap+k]=P(ai,v)a[p{:}a_p+k]=P(a_i,v) lies in UU, and by Step 4

βˆ£βˆ‚if(a[p:ap+k])βˆ’βˆ‚if(a)kβˆ’βˆ‚iβˆ‚pf(a)∣<Ξ΅.\left|\frac{\partial_i f(a[p{:}a_p+k])-\partial_i f(a)}{k}-\partial_i\partial_p f(a)\right|<\varepsilon.

Thus for every real Ξ΅\varepsilon with 0<Ξ΅0<\varepsilon there is a real Ξ΄1\delta_1 with 0<Ξ΄10<\delta_1 such that every real kk with 0<∣k∣<Ξ΄10<|k|<\delta_1 satisfies a[p:ap+k]∈Ua[p{:}a_p+k]\in U and the displayed inequality. By Partial Derivative on a Euclidean Open Set this says exactly that the partial derivative of βˆ‚if\partial_i f with respect to the ppth variable exists at aa with value βˆ‚iβˆ‚pf(a)\partial_i\partial_p f(a); that is, βˆ‚pβˆ‚if(a)=βˆ‚iβˆ‚pf(a)\partial_p\partial_i f(a)=\partial_i\partial_p f(a).

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