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Change of variables for an injective C1C^1 map on a compact Jordan set

Statement

Let n1n\ge1, let URnU\subseteq\mathbb R^n be open, let g:URng:U\to\mathbb R^n be injective and C1C^1, and suppose Dg(x)Dg(x) is invertible for every xUx\in U. Let KUK\subseteq U be compact and Jordan measurable. For a bounded function f:g(K)Rf:g(K)\to\mathbb R, the following are equivalent:

  1. ff is Riemann integrable on g(K)g(K);
  2. xf(g(x))detDg(x)x\mapsto f(g(x))|\det Dg(x)| is Riemann integrable on KK.

When either condition holds, g(K)f(y)dy=Kf(g(x))detDg(x)dx.\int_{g(K)}f(y)\,dy=\int_K f(g(x))|\det Dg(x)|\,dx.

Facts & Assumptions

Given: The map gg, compact Jordan set KK, and bounded ff in the statement.

[L1]

For each fixed n1n\ge1, the function det:Mn(R)R\det:M_n(\mathbb R)\to\mathbb R is evaluation of a polynomial in the n2n^2 matrix-entry variables (For every fixed finite size at least one, the determinant of a real square matrix is a polynomial in its matrix entries), and componentwise continuity gives continuity of maps assembled from finitely many continuous components (A vector-valued function has a limit, or is continuous, if and only if each of its components does; with the algebra of continuous vector-valued functions).

[L2]

Local C1C^1 volume distortion is bounded by factors arbitrarily close to the absolute determinant of the derivative (On a small cube, a C1C^1 diffeomorphism distorts Jordan content by factors arbitrarily close to its linearized absolute determinant), with finite Jordan cover bounds controlling upper and lower sums (Finite Jordan covers bound upper integrals, while interior-disjoint Jordan subfamilies bound lower integrals).

[L3]

The image g(K)g(K) is compact Jordan (An injective C1C^1 map with invertible derivative sends compact Jordan sets to compact Jordan sets), while the inverse function theorem supplies local C1C^1 inverses (The Euclidean inverse function theorem).

[L4]

The chain rule multiplies derivatives (The chain rule for total derivatives: D(gf)(a)=Dg(f(a))Df(a)D(g\circ f)(a)=Dg(f(a))\circ Df(a)), and for n1n\ge1 and A,BMn(R)A,B\in M_n(R) over a commutative ring one has det(AB)=det(A)det(B)\det(AB)=\det(A)\det(B) (For same-sized finite square matrices over a commutative ring, det(AB)=det(A)det(B)\det(AB)=\det(A)\det(B)).

[L5]

The Riemann integral is linear, monotone, and stable under absolute value (Linearity, monotonicity, the absolute-value estimate and coordinate-slice additivity for the Riemann integral in Rm\mathbb{R}^m), with Jordan-set values independent of the bounding rectangle (The Riemann integral over a Jordan set is independent of the bounding rectangle).

[L6]

Every continuous real function on a compact Jordan set is Riemann integrable there (A continuous real function on a compact Jordan measurable set is Riemann integrable over that set).

[L7]

Finite Jordan covers bound upper integrals, and interior-disjoint Jordan subfamilies bound lower integrals (Finite Jordan covers bound upper integrals, while interior-disjoint Jordan subfamilies bound lower integrals).

Proof

technique · local-to-global
1.1

The entries of DgDg are continuous; [L1] therefore makes detDg\det Dg and detDg|\det Dg| continuous on KK, and [L6] makes the absolute determinant bounded and Riemann integrable. By [L3], g(K)g(K) is also a compact Jordan set.

L1L3L6
1.2

Global injectivity and [L3] patch the local inverses into a C1C^1 inverse G:g(U)UG:g(U)\to U. By [L4], DG(g(x))Dg(x)=IDG(g(x))Dg(x)=I and detDG(g(x))detDg(x)=1|\det DG(g(x))|\,|\det Dg(x)|=1.

L3L4
2.1

Let EKE\subseteq K be compact Jordan. Cover it by finitely many cubes on which [L2] gives volume factors detDg(a)(1±ε)n|\det Dg(a)|(1\pm\varepsilon)^n and on which detDg|\det Dg| has arbitrarily small oscillation. A common interior-disjoint grid refinement and [L7] compare cont(g(E))\operatorname{cont}(g(E)) with the lower and upper sums of detDg|\det Dg| over EE. Letting the mesh and ε\varepsilon tend to zero gives cont(g(E))=EdetDg\operatorname{cont}(g(E))=\int_E|\det Dg|.

L2L7step 1.1step 1.2
3.1

First take f0f\ge0 integrable on g(K)g(K). A fine rectangular grid of a bounding rectangle cuts g(K)g(K), up to content-zero shared faces, into compact Jordan pieces FjF_j on which the lower and upper Darboux step functions have arbitrarily small integral gap. Their preimages Ej=G(Fj)E_j=G(F_j) are compact Jordan by [L3]. Step 2.1 turns every coefficient times cont(Fj)\operatorname{cont}(F_j) into the integral of that coefficient times detDg|\det Dg| over EjE_j. Hence the pulled-back lower and upper step functions squeeze (fg)detDg(f\circ g)|\det Dg| with the same arbitrarily small gap, proving its integrability and the formula. Applying this implication to GG and using step 1.2 proves the converse.

L3L5step 1.2step 2.1
4.1

For signed ff, apply step 3.1 to f+=max(f,0)f^+=\max(f,0) and f=max(f,0)f^-=\max(-f,0). Stability under absolute value and linearity in [L5] give both integrability implications and the formula for f=f+ff=f^+-f^-. Bounding-rectangle independence also follows from [L5].

L5step 3.1

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