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Proof of First- and Second-Order Conditions at a Local Extremum of a Function of Class C2C^2

lemmalem:c2-local-extremum-conditions-2026b
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Reason: Proof of lem:c2-local-extremum-conditions-2026b, carried forward and re-versioned onto thm:second-order-taylor-peano-2026b, lem:c2-difference-constant-2026b and thm:hessian-symmetric-2026b, with the index order of the Taylor quadratic term reconciled explicitly via symmetry of the Hessian. Exposure-clean.

Proof

Notation. For y,hRny,h\in\mathbb{R}^n write y+hy+h for the point of Rn\mathbb{R}^n whose iith coordinate is yi+hiy_i+h_i; this is the coordinatewise addition used in Second-Order Taylor Expansion with Peano Remainder. For tRt\in\mathbb{R} and zRnz\in\mathbb{R}^n write tztz for the point whose iith coordinate is tzitz_i, and write z-z for (1)z(-1)z. For yRny\in\mathbb{R}^n write y=dE(y,0Rn)\lVert y\rVert=d_E(y,0_{\mathbb{R}^n}), as in Second-Order Taylor Expansion with Peano Remainder. Write t2t^2 for ttt\cdot t.

Write iw\partial_i w for the partial derivative of ww with respect to the iith variable, and use the second-order notation 2wxixj=ijw\frac{\partial^2 w}{\partial x_i\,\partial x_j}=\partial_i\partial_j w of Hessian Matrix of a C^2 Function, the iterated partial derivative of clause 4 of C^k Maps on a Euclidean Open Set. Set

αi=wxi(x),βij=2wxixj(x)(i,j{1,,n}),\alpha_i=\frac{\partial w}{\partial x_i}(x),\qquad \beta_{ij}=\frac{\partial^2 w}{\partial x_i\,\partial x_j}(x)\qquad (i,j\in\{1,\dots,n\}),

and for z=(z1,,zn)Rnz=(z_1,\dots,z_n)\in\mathbb{R}^n set

L(z)=i=1nαizi,Q(z)=21i=1nj=1nβijzizj.L(z)=\sum_{i=1}^n \alpha_i z_i,\qquad Q(z)=2^{-1}\sum_{i=1}^n\sum_{j=1}^n \beta_{ij}z_iz_j .

By the definition of the gradient and the definition of the dot product, L(z)=Dw(x)zL(z)=Dw(x)\cdot z. By the definition of the Hessian matrix, the definition of the matrix-vector product and the definition of the dot product,

z(D2w(x)z)=i=1nzij=1nβijzj=i=1nj=1nβijzizj,z\cdot\bigl(D^2w(x)z\bigr)=\sum_{i=1}^n z_i\sum_{j=1}^n \beta_{ij}z_j=\sum_{i=1}^n\sum_{j=1}^n \beta_{ij}z_iz_j,

so Q(z)=21z(D2w(x)z)Q(z)=2^{-1}\,z\cdot(D^2w(x)z). By distributivity in the field R\mathbb{R} we have, for all tRt\in\mathbb{R} and zRnz\in\mathbb{R}^n,

L(tz)=tL(z),Q(tz)=t2Q(z),L(tz)=tL(z),\qquad Q(tz)=t^2Q(z),

and in particular L(z)=L(z)L(-z)=-L(z); also L(0Rn)=0L(0_{\mathbb{R}^n})=0 and Q(0Rn)=0Q(0_{\mathbb{R}^n})=0.

Step 0 (elementary facts). References to numbered claims below are to Elementary Order Arithmetic in an Ordered Field unless another item is named.

(a) For every yRny\in\mathbb{R}^n, 0y0\le\lVert y\rVert and y2=i=1nyi2\lVert y\rVert^2=\sum_{i=1}^n y_i^2. Indeed, by the definition of the Euclidean distance, y\lVert y\rVert is the nonnegative square root of i=1n(yi0)2=i=1nyi2\sum_{i=1}^n (y_i-0)^2=\sum_{i=1}^n y_i^2, so this holds by Existence and Uniqueness of the Nonnegative Square Root.

(b) For all y,hRny,h\in\mathbb{R}^n, dE(y,y+h)=hd_E(y,y+h)=\lVert h\rVert. Indeed (yi(yi+hi))2=(hi)(hi)=hi2(y_i-(y_i+h_i))^2=(-h_i)\cdot(-h_i)=h_i^2 for every ii, so both sides are the nonnegative square root of i=1nhi2\sum_{i=1}^n h_i^2.

(c) If z0Rnz\ne 0_{\mathbb{R}^n} then 0<z0<\lVert z\rVert and 0<z20<\lVert z\rVert^2. Indeed dEd_E is a metric by Euclidean Distance is a Metric on Rn\mathbb{R}^n, so by the definition of a metric space z=dE(z,0Rn)=0\lVert z\rVert=d_E(z,0_{\mathbb{R}^n})=0 would force z=0Rnz=0_{\mathbb{R}^n}; with (a) this gives 0<z0<\lVert z\rVert, and then 0<zz=z20<\lVert z\rVert\cdot\lVert z\rVert=\lVert z\rVert^2 by claim 5.

(d) If 0<t0<t and zRnz\in\mathbb{R}^n then tz=tz\lVert tz\rVert=t\lVert z\rVert. Indeed by (a) and field arithmetic tz2=i=1n(tzi)2=t2i=1nzi2=t2z2=(tz)2\lVert tz\rVert^2=\sum_{i=1}^n (tz_i)^2=t^2\sum_{i=1}^n z_i^2=t^2\lVert z\rVert^2=(t\lVert z\rVert)^2. Both tz\lVert tz\rVert and tzt\lVert z\rVert are nonnegative: the first by (a), and for the second, either z=0\lVert z\rVert=0 and then tz=0t\lVert z\rVert=0, or 0<z0<\lVert z\rVert and then 0<tz0<t\lVert z\rVert by claim 5. Claim 3 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field now gives the asserted equality.

(e) If pqp\le q and 0<c0<c then cpcqcp\le cq. Indeed, if p=qp=q this is an equality, and if p<qp<q then cp<cqcp<cq by claim 10.

(f) If pqp\le q and rsr\le s then p+rq+sp+r\le q+s. This follows from the compatibility of \le with addition in an ordered field, which gives p+rq+rp+r\le q+r and q+rq+sq+r\le q+s, together with transitivity of \le.

Step 1 (the basic inequality). Assume that ww has a local maximum at xx relative to UU. Then for every εR\varepsilon\in\mathbb{R} with 0<ε0<\varepsilon and every zRnz\in\mathbb{R}^n with z0Rnz\ne 0_{\mathbb{R}^n} there is τR\tau\in\mathbb{R} with 0<τ0<\tau such that

L(z)+tQ(z)εtz2for every tR with 0<t<τ.L(z)+tQ(z)\le \varepsilon\, t\,\lVert z\rVert^2\qquad\text{for every } t\in\mathbb{R}\text{ with } 0<t<\tau .

By the definition of a local maximum relative to UU there is δ1R\delta_1\in\mathbb{R} with 0<δ10<\delta_1 such that every yUy\in U with dE(x,y)<δ1d_E(x,y)<\delta_1 satisfies w(y)w(x)w(y)\le w(x). Let ε\varepsilon be given with 0<ε0<\varepsilon. By Second-Order Taylor Expansion with Peano Remainder, applied to ww at xx, there is δ2R\delta_2\in\mathbb{R} with 0<δ20<\delta_2 such that every hRnh\in\mathbb{R}^n with h<δ2\lVert h\rVert<\delta_2 satisfies x+hUx+h\in U and

w(x+h)w(x)L(h)Q(h)εh2,\bigl|\,w(x+h)-w(x)-L(h)-Q(h)\,\bigr|\le\varepsilon\lVert h\rVert^2,

where |\cdot| is the absolute value on R\mathbb{R}. The first sum appearing in that theorem is i=1niw(x)hi=L(h)\sum_{i=1}^n\partial_i w(x)h_i=L(h). Its second sum is 21i=1nj=1njiw(x)hihj2^{-1}\sum_{i=1}^n\sum_{j=1}^n\partial_j\partial_i w(x)h_ih_j, and by claim 1 of Equality of Mixed Second Partial Derivatives and Symmetry of the Hessian we have jiw(x)=ijw(x)=βij\partial_j\partial_i w(x)=\partial_i\partial_j w(x)=\beta_{ij} for all i,ji,j, so that sum is exactly Q(h)Q(h). By claim 9 let δ3\delta_3 be the smaller of δ1\delta_1 and δ2\delta_2, so 0<δ30<\delta_3.

Let z0Rnz\ne 0_{\mathbb{R}^n}. By (c), 0<z0<\lVert z\rVert, so by claim 7 the inverse z1\lVert z\rVert^{-1} exists and is positive, and by claim 5 the element τ=δ3z1\tau=\delta_3\lVert z\rVert^{-1} satisfies 0<τ0<\tau. Let tRt\in\mathbb{R} with 0<t<τ0<t<\tau and put h=tzh=tz. By claim 10, zt<zδ3z1=δ3\lVert z\rVert t<\lVert z\rVert\delta_3\lVert z\rVert^{-1}=\delta_3, so by (d) we get h=tz<δ3\lVert h\rVert=t\lVert z\rVert<\delta_3, whence h<δ1\lVert h\rVert<\delta_1 and h<δ2\lVert h\rVert<\delta_2 by claim 2.

Since h<δ2\lVert h\rVert<\delta_2, we have x+hUx+h\in U and the displayed Taylor estimate holds for this hh. Since dE(x,x+h)=h<δ1d_E(x,x+h)=\lVert h\rVert<\delta_1 by (b), the choice of δ1\delta_1 gives w(x+h)w(x)w(x+h)\le w(x), hence w(x+h)w(x)0w(x+h)-w(x)\le 0 by claim 1.

Put R=w(x+h)w(x)L(h)Q(h)R=w(x+h)-w(x)-L(h)-Q(h). From Rεh2|R|\le\varepsilon\lVert h\rVert^2 and claim 6 of Properties of the Absolute Value in an Ordered Field we get εh2R-\varepsilon\lVert h\rVert^2\le R, hence Rεh2-R\le\varepsilon\lVert h\rVert^2 by claim 4. Since L(h)+Q(h)=(w(x+h)w(x))+(R)L(h)+Q(h)=\bigl(w(x+h)-w(x)\bigr)+(-R), (f) gives

L(h)+Q(h)0+εh2=εh2.L(h)+Q(h)\le 0+\varepsilon\lVert h\rVert^2=\varepsilon\lVert h\rVert^2 .

By (d) and (a), h2=(tz)2=t2z2\lVert h\rVert^2=(t\lVert z\rVert)^2=t^2\lVert z\rVert^2, while L(h)=tL(z)L(h)=tL(z) and Q(h)=t2Q(z)Q(h)=t^2Q(z). Thus

tL(z)+t2Q(z)εt2z2.tL(z)+t^2Q(z)\le \varepsilon\,t^2\lVert z\rVert^2 .

Since 0<t0<t, claim 7 gives 0<t10<t^{-1}, so multiplying by t1t^{-1} and simplifying by field arithmetic, using (e), yields L(z)+tQ(z)εtz2L(z)+tQ(z)\le\varepsilon\,t\,\lVert z\rVert^2. This proves Step 1.

Step 2 (the gradient vanishes). Keep the hypothesis of claim 1 and let z0Rnz\ne 0_{\mathbb{R}^n}. Apply Step 1 with ε=1\varepsilon=1, which is admissible since 0<10<1 by claim 6, and let τ\tau be as there. Adding tQ(z)-tQ(z) to both sides of the inequality of Step 1 (compatibility of \le with addition in an ordered field) gives

L(z)t(z2Q(z))for every t with 0<t<τ.L(z)\le t\,\bigl(\lVert z\rVert^2-Q(z)\bigr)\qquad\text{for every } t\text{ with } 0<t<\tau .

Write M=z2Q(z)M=\lVert z\rVert^2-Q(z) and suppose, for contradiction, that 0<L(z)0<L(z).

If M0M\le 0, take t=τ21t=\tau\cdot 2^{-1}, which satisfies 0<t<τ0<t<\tau by claim 8. Then tMt0=0tM\le t\cdot 0=0 by (e), so L(z)0L(z)\le 0 by transitivity of \le, contradicting 0<L(z)0<L(z).

If 0<M0<M, then M1M^{-1} exists and 0<M10<M^{-1} by claim 7, and 0<L(z)M1210<L(z)M^{-1}\cdot 2^{-1} by claims 5 and 8. By claim 9 let tt be the smaller of τ21\tau\cdot 2^{-1} and L(z)M121L(z)M^{-1}\cdot 2^{-1}; then 0<t0<t and tτ21<τt\le\tau\cdot 2^{-1}<\tau, so tt is admissible by claim 2. By (e), tML(z)M121M=L(z)21tM\le L(z)M^{-1}\cdot 2^{-1}\cdot M=L(z)\cdot 2^{-1}, and L(z)21<L(z)L(z)\cdot 2^{-1}<L(z) by claim 8. Hence L(z)tML(z)21<L(z)L(z)\le tM\le L(z)\cdot2^{-1}<L(z), so L(z)<L(z)L(z)<L(z) by claim 2, which is impossible.

Therefore L(z)0L(z)\le 0 for every z0Rnz\ne 0_{\mathbb{R}^n}; and L(0Rn)=00L(0_{\mathbb{R}^n})=0\le 0. So L(z)0L(z)\le0 for every zRnz\in\mathbb{R}^n. Applying this to z-z and using L(z)=L(z)L(-z)=-L(z) gives L(z)0-L(z)\le 0, hence 0L(z)0\le L(z) by claim 4. Since \le is a total order and therefore antisymmetric, L(z)=0L(z)=0 for every zRnz\in\mathbb{R}^n.

For i{1,,n}i\in\{1,\dots,n\} let eiRne_i\in\mathbb{R}^n be the point whose iith coordinate is 11 and whose other coordinates are 00. Then L(ei)=αiL(e_i)=\alpha_i, so αi=0\alpha_i=0. By the definition of the gradient, Dw(x)=(α1,,αn)=0RnDw(x)=(\alpha_1,\dots,\alpha_n)=0_{\mathbb{R}^n}.

Step 3 (the Hessian is negative semidefinite). Keep the hypothesis of claim 1, let z0Rnz\ne 0_{\mathbb{R}^n} and let εR\varepsilon\in\mathbb{R} with 0<ε0<\varepsilon. Let τ\tau be as in Step 1 for this ε\varepsilon and zz, and take t=τ21t=\tau\cdot 2^{-1}, so 0<t<τ0<t<\tau by claim 8. By Step 2 we have L(z)=0L(z)=0, so Step 1 gives tQ(z)εtz2tQ(z)\le\varepsilon\,t\,\lVert z\rVert^2. Multiplying by t1t^{-1}, which is positive by claim 7, and using (e) and field arithmetic, we get

Q(z)εz2.Q(z)\le\varepsilon\lVert z\rVert^2 .

Suppose, for contradiction, that 0<Q(z)0<Q(z). By (c), 0<z20<\lVert z\rVert^2, so (z2)1(\lVert z\rVert^2)^{-1} exists and is positive by claim 7, and ε0=Q(z)(z2)121\varepsilon_0=Q(z)\,(\lVert z\rVert^2)^{-1}\cdot 2^{-1} satisfies 0<ε00<\varepsilon_0 by claims 5 and 8. Applying the previous inequality with ε0\varepsilon_0 in place of ε\varepsilon gives Q(z)Q(z)21Q(z)\le Q(z)\cdot 2^{-1}, while Q(z)21<Q(z)Q(z)\cdot2^{-1}<Q(z) by claim 8; by claim 2 this yields Q(z)<Q(z)Q(z)<Q(z), which is impossible. Hence Q(z)0Q(z)\le 0 for every z0Rnz\ne0_{\mathbb{R}^n}, and Q(0Rn)=00Q(0_{\mathbb{R}^n})=0\le0, so Q(z)0Q(z)\le0 for every zRnz\in\mathbb{R}^n.

Since Q(z)=21z(D2w(x)z)Q(z)=2^{-1}\,z\cdot(D^2w(x)z) and 0<20<2 by claim 8, multiplying by 22 and using (e) gives z(D2w(x)z)0z\cdot(D^2w(x)z)\le 0 for every zRnz\in\mathbb{R}^n. By the definition of the matrix-vector product, (0nz)i=j=1n0zj=0(0_nz)_i=\sum_{j=1}^n 0\cdot z_j=0 for every ii, so 0nz=0Rn0_nz=0_{\mathbb{R}^n} and, by the definition of the dot product, z(0nz)=0z\cdot(0_nz)=0. Hence z(D2w(x)z)z(0nz)z\cdot(D^2w(x)z)\le z\cdot(0_nz) for every zRnz\in\mathbb{R}^n, which by the definition of the positive semidefinite ordering says D2w(x)0nD^2w(x)\preceq 0_n. Together with Step 2 this proves claim 1.

Step 4 (the local minimum case). Assume now that ww has a local minimum at xx relative to UU. Let k0:URk_0:U\to\mathbb{R} be the function with constant value 00. By claim 2 of Differences and Constants for Functions of Class C2C^2 on a Euclidean Open Set, k0k_0 is of class C2C^2 on UU with Dk0(y)=0RnDk_0(y)=0_{\mathbb{R}^n} and D2k0(y)=0nD^2k_0(y)=0_n for every yUy\in U. By claim 1 of that lemma the function v=k0wv=k_0-w, whose value at yUy\in U is 0w(y)=w(y)0-w(y)=-w(y), is of class C2C^2 on UU, and for every yUy\in U

Dv(y)=0RnDw(y),D2v(y)=0nD2w(y).Dv(y)=0_{\mathbb{R}^n}-Dw(y),\qquad D^2v(y)=0_n-D^2w(y).

By the definition of a local minimum relative to UU there is δR\delta\in\mathbb{R} with 0<δ0<\delta such that every yUy\in U with dE(x,y)<δd_E(x,y)<\delta satisfies w(x)w(y)w(x)\le w(y); by claim 4 this gives w(y)w(x)-w(y)\le -w(x), that is, v(y)v(x)v(y)\le v(x). Hence vv has a local maximum at xx relative to UU.

Applying claim 1, already proved, to vv in place of ww gives Dv(x)=0RnDv(x)=0_{\mathbb{R}^n} and D2v(x)0nD^2v(x)\preceq 0_n. By the definition of the difference of points of Rn\mathbb{R}^n, the iith coordinate of Dv(x)Dv(x) is 0w/xi(x)0-\partial w/\partial x_i(x); since it is 00, we get w/xi(x)=0\partial w/\partial x_i(x)=0 for every ii, and hence Dw(x)=0RnDw(x)=0_{\mathbb{R}^n} by the definition of the gradient.

By the definition of the difference of real matrices, (D2v(x))ij=0(D2w(x))ij(D^2v(x))_{ij}=0-(D^2w(x))_{ij}, so by the definitions of the matrix-vector product and of the dot product, together with distributivity in R\mathbb{R},

z(D2v(x)z)=(z(D2w(x)z))for every zRn.z\cdot\bigl(D^2v(x)z\bigr)=-\bigl(z\cdot(D^2w(x)z)\bigr)\qquad\text{for every } z\in\mathbb{R}^n .

Since D2v(x)0nD^2v(x)\preceq 0_n and z(0nz)=0z\cdot(0_nz)=0, this gives (z(D2w(x)z))0-\bigl(z\cdot(D^2w(x)z)\bigr)\le 0, hence 0z(D2w(x)z)0\le z\cdot(D^2w(x)z) by claim 4, that is, z(0nz)z(D2w(x)z)z\cdot(0_nz)\le z\cdot(D^2w(x)z) for every zRnz\in\mathbb{R}^n. By the definition of the positive semidefinite ordering, 0nD2w(x)0_n\preceq D^2w(x). This proves claim 2.

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