Quadratic forms, volumes and separation

This companion retains AN03-P001 Sections 4–5 and supplies the connecting finite-dimensional facts used by the selected metric and multiplier proofs.

This is a separate modified selection from the earlier AN-03 programme. Original principal author and publisher: AN-03 course-writing task / AN-03 local course project, 2026. Earlier modification: AN-03 course-writing task and OpenAI Codex. Selection and the identified connecting proofs: GPT-6 Astra (OpenAI), Ultra, 4 October 2026; publisher: AN-04 local course project.

Original text: CC0.

0. Exact earlier inputs

The measure companion, M0–M8 supplies the declared choice principle, rational enumeration, completed measure and convergence theorems. The Fourier companion, L0–L3 supplies the full L2L^2 extension and distributional compatibility. The exact U001 Schwartz and spectral proofs, Q3–Q5 supply all finite-dimensional Fourier and spectral steps. The finite-dimensional compactness, algebra and differential inputs are the exact earlier proofs named in that companion's F0 contract. Smooth cutoffs are U001 P14.3. Compact and affine substitution, with every determinant, is U001 P21.3–P21.4. M8 proves compatibility of these integrals with the Lebesgue integrals.

1. Positive forms and coordinate maps

Let Q(X)=XTGXQ(X)=X^{\mathsf T}GX, where GG is real symmetric positive definite. U001 Q5 gives G=Udiag⁡(λj)UTG=U\operatorname{diag}(\lambda_j)U^{\mathsf T}, λj>0\lambda_j>0. Put L=Udiag⁡(λj−1/2)L=U\operatorname{diag}(\lambda_j^{-1/2}). Then LTGL=IL^{\mathsf T}GL=I, G−1=LLTG^{-1}=LL^{\mathsf T}, and J=∣det⁡L∣=(det⁡G)−1/2>0J=|\det L|=(\det G)^{-1/2}>0, by direct multiplication and the proved determinant rules. Thus Q(Ly)=∣y∣2Q(Ly)=|y|^2 and Q−1(Ξ)=ΞTG−1Ξ=∣LTΞ∣2Q^{-1}(\Xi)=\Xi^{\mathsf T}G^{-1}\Xi=|L^{\mathsf T}\Xi|^2. The Euclidean Cauchy–Schwarz inequality follows by expanding ∣v−tv′∣2≥0|v-tv'|^2\geq0 and minimizing in the real scalar tt; the zero-vector case is immediate. Transfer this inequality by LL to obtain the triangle inequality for Q1/2Q^{1/2}.

If BB is another real symmetric matrix, its expression under these maps is L−1BL−TL^{-1}BL^{-\mathsf T}, which is again symmetric and hence has an orthonormal eigenbasis by Q5. This proves the simultaneous normalization used in the multiplier companion, without a new spectral or Gram-matrix theorem. The chain rule gives the corresponding directional derivative identities. In an orthonormal basis each coordinate of a unit direction has absolute value at most one; expansion of a kk-linear form then compares its directional norm and its maximum coordinate coefficient with factors at most dkd^k.

2. Lebesgue volume of each ellipsoid

Let K={Q(X)<r2}K=\{Q(X)<r^2\}, r>0r>0. Choose a smooth function b:R→[0,1]b:\mathbb R\to[0,1], zero for t≤0t\leq0 and one for t≥1t\geq1, using the supplied flat cutoff, and set fk(X)=b(k(r2−Q(X)))f_k(X)=b(k(r^2-Q(X))). Each fkf_k is compact smooth, is supported in the closed ellipsoid, and converges pointwise to 1K\mathbf1_K. All supports lie in a fixed cube: positivity of the eigenvalues bounds ∣X∣|X| on them. Compact substitution, followed by M8 and dominated convergence on that cube and its inverse image, therefore gives

∣K∣=J ∣{y:∣y∣<r}∣=Jrd ∣{y:∣y∣<1}∣.(F1) |K|=J\,|\{y:|y|<r\}|=Jr^d\,|\{y:|y|<1\}|. \tag{F1}

The second equality uses the same argument for y=rzy=rz. The unit ball has positive finite measure, since it contains a positive-volume cube and lies in a bounded cube. Translations have Jacobian one. Consequently every ellipsoid volume comparison used in the covering and counting proofs follows from (F1), inclusions, and countable additivity. No unproved general measure substitution theorem is being invoked for indicator functions.

3. Dual ellipsoids and phase distances

Suppose B:E∗→EB:E^*\to E is symmetric and A(Ξ)=⟨BΞ,Ξ⟩A(\Xi)=\langle B\Xi,\Xi\rangle. Use Section 1 to make QQ Euclidean and B=diag⁡(βj)B=\operatorname{diag}(\beta_j). On the range of BB, write

QA(Z)=∑βj≠0Zj2/βj2;QA(Z)=+∞(Z∉ran⁡B).(F2) Q^A(Z)=\sum_{\beta_j\ne0}Z_j^2/\beta_j^2; \qquad Q^A(Z)=+\infty\quad(Z\notin\operatorname{ran}B). \tag{F2}

This is exactly the supremum defining the phase-dual form: put wj=βjΞjw_j=\beta_j\Xi_j, apply Cauchy–Schwarz to ∑Zjwj/βj\sum Z_jw_j/\beta_j, and approach the unit vector in that direction. A nonzero coordinate in ker⁡B\ker B makes the supremum infinite by scalar dilation. This proves both directions, including B=0B=0.

For η∈E∗\eta\in E^*, the support value of {Z:QA(Z)<a2}\{Z:Q^A(Z)<a^2\} is

a(∑jβj2ηj2)1/2=a Q(Bη)1/2.(F3) a\left(\sum_j\beta_j^2\eta_j^2\right)^{1/2} =a\,Q(B\eta)^{1/2}. \tag{F3}

Again Cauchy–Schwarz gives the upper bound. When the square root is positive, take ZjZ_j proportional to βj2ηj\beta_j^2\eta_j and approach the boundary from inside; when it is zero, every pairing vanishes and both sides are zero. The same calculation with the ordinary dual form gives support value rQ−1(η)1/2rQ^{-1}(\eta)^{1/2} for {Q<r2}\{Q<r^2\}. For Q1≤MQ2Q_1\leq M Q_2, inclusion of the defining ellipsoids and scaling gives Q1A≥M−1Q2AQ_1^A\geq M^{-1}Q_2^A on the common finite domain. Off it both sides are interpreted as infinite. Sections 4–5 below prove the separation and sum rules needed to use these support values.

4. Strict separation of an open convex set

Theorem 4.1 (Strict separation). Let VV be a finite-dimensional real vector space, let C⊂VC\subset V be nonempty, open and convex, and let x∉Cx\notin C. There is a nonzero real covector η\eta such that

η(y)<η(x)(y∈C),sup⁡y∈Cη(y)≤η(x). \eta(y)<\eta(x)\quad(y\in C), \qquad \sup_{y\in C}\eta(y)\leq\eta(x).

The second inequality includes xx on the boundary. The supremum need not be attained. The proof uses only finite-dimensional compactness and the inner product.

Choose an auxiliary Euclidean norm, put K=C‾K=\overline C, and fix c∈Cc\in C with B(c,r)⊂CB(c,r)\subset C, r>0r>0. First, if z∈Kz\in K and 0≤t<10\leq t<1, then

(1−t)c+tz∈C. (1-t)c+tz\in C.

For t=0t=0 this is immediate. For 0<t<10<t<1, choose zj∈Cz_j\in C tending to zz. Convexity gives a ball of radius (1−t)r(1-t)r centered at (1−t)c+tzj(1-t)c+tz_j inside CC. For sufficiently large jj, this ball contains (1−t)c+tz(1-t)c+tz, proving the assertion.

For ε>0\varepsilon>0, put zε=x+ε(x−c)z_\varepsilon=x+\varepsilon(x-c). This point lies outside KK: if it lay in KK, then

x=ε1+εc+11+εzε x=\frac{\varepsilon}{1+\varepsilon}c +\frac{1}{1+\varepsilon}z_\varepsilon

would lie in CC by the preceding assertion. The nonempty closed set KK has a point qεq_\varepsilon nearest to zεz_\varepsilon. To see existence without a compactness assumption on KK, take a minimizing sequence. Its distance to zεz_\varepsilon is bounded, so it has a convergent subsequence in finite dimensions; closedness places its limit in KK.

Write vε=zε−qε≠0v_\varepsilon=z_\varepsilon-q_\varepsilon\ne0. For y∈Ky\in K, the segment qε+t(y−qε)q_\varepsilon+t(y-q_\varepsilon), 0≤t≤10\leq t\leq1, lies in KK. Differentiating the squared distance at its minimum t=0t=0 gives

⟨vε,y−qε⟩≤0. \langle v_\varepsilon,y-q_\varepsilon\rangle\leq0.

Consequently, for uε=vε/∣vε∣u_\varepsilon=v_\varepsilon/|v_\varepsilon|,

⟨uε,y⟩≤⟨uε,zε⟩−∣vε∣≤⟨uε,zε⟩. \langle u_\varepsilon,y\rangle \leq\langle u_\varepsilon,z_\varepsilon\rangle -|v_\varepsilon| \leq\langle u_\varepsilon,z_\varepsilon\rangle.

Choose ε=1/k\varepsilon=1/k and a convergent subsequence of the unit vectors, with limit uu, ∣u∣=1|u|=1. Since zε→xz_\varepsilon\to x, the last inequality implies ⟨u,y⟩≤⟨u,x⟩\langle u,y\rangle\leq\langle u,x\rangle for every y∈Ky\in K. The same subsequence works for every yy: it was selected using only the unit vectors, and the inequality holds for every yy at every index.

Set η(y)=⟨u,y⟩\eta(y)=\langle u,y\rangle. It is nonzero. For y∈Cy\in C, openness gives y+δu∈Cy+\delta u\in C for some δ>0\delta>0, whence

η(y)+δ≤η(x). \eta(y)+\delta\leq\eta(x).

This proves strict pointwise separation. The supremum statement follows because η(C)\eta(C) is nonempty and bounded above. In dimension zero the hypotheses cannot occur, since the only nonempty open set is all of VV.

5. Support functions of Minkowski sums

Proposition 5.1. For nonempty A,B⊂VA,B\subset V, put

hA(η)=sup⁡a∈Aη(a)∈R∪{+∞}. h_A(\eta)=\sup_{a\in A}\eta(a)\in\mathbb R\cup\{+\infty\}.

Then hA+B(η)=hA(η)+hB(η)h_{A+B}(\eta)=h_A(\eta)+h_B(\eta), where A+B={a+b:a∈A,b∈B}A+B=\{a+b:a\in A,b\in B\}. Nonemptiness excludes −∞-\infty, so the right side is unambiguous.

Linearity first gives the inequality ≤\leq. If both right-hand suprema are finite, choose a,ba,b within ε/2\varepsilon/2 of the two suprema. Their sum gives the reverse inequality up to ε\varepsilon; let ε↓0\varepsilon\downarrow0. If hA(η)=+∞h_A(\eta)=+\infty, fix b0∈Bb_0\in B. The values η(a+b0)\eta(a+b_0) are unbounded above, so hA+B(η)=+∞h_{A+B}(\eta)=+\infty. Interchange A,BA,B for the other case. No boundedness, compactness or convexity is needed for this identity.