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Proof of Lebesgue Measure under a Triangular or Symmetric Positive Definite Linear Map

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Linear maps are Lipschitz, hence Borel. The triangular case is proved by induction on the dimension, splitting off the last coordinate with Tonelli and using one-dimensional translation and scaling (inner integral over the last coordinate for lower triangular matrices, over the first block for upper triangular ones); the symmetric positive definite case follows from the Cholesky factorisation.

Proof

Each result cited below is universally quantified over the data in its own statement.

Conventions. For a natural number l1l\ge1 let Bl\mathcal{B}_{l} and λl\lambda_{l} be the σ\sigma-algebra and measure on Rl\mathbb{R}^{l} built in Finite Products of Lebesgue Measure and Coordinate Integration on Rl\mathbb{R}^l. By claim 5 of The Borel Sigma-Algebra of a Euclidean Space as a Product, and Measurability of Projections, Sequentially Continuous Maps, and Open and Closed Sets, Bl=B(Rl)\mathcal{B}_{l}=\mathcal{B}(\mathbb{R}^{l}), and by Lebesgue Measure on Rn\mathbb{R}^n this λl\lambda_{l} is Lebesgue measure on B(Rl)\mathcal{B}(\mathbb{R}^{l}); for l=1l=1 it is Lebesgue measure λ\lambda on B1=B(R)\mathcal{B}_{1}=\mathcal{B}(\mathbb{R}). By claim 1 of Finite Products of Lebesgue Measure and Coordinate Integration on Rl\mathbb{R}^l each λl\lambda_{l} is σ\sigma-finite. For l2l\ge2 we use the identification of Rl\mathbb{R}^{l} with Rl1×R\mathbb{R}^{l-1}\times\mathbb{R} fixed there, writing x=(x,xl)x=(x',x_{l}) with x=(x1,,xl1)x'=(x_{1},\dots,x_{l-1}); under it Bl=Bl1B(R)\mathcal{B}_{l}=\mathcal{B}_{l-1}\otimes\mathcal{B}(\mathbb{R}) and λl=λl1λ\lambda_{l}=\lambda_{l-1}\otimes\lambda. A Borel f:Rl[0,]f:\mathbb{R}^{l}\to[0,\infty] is one with {f>a}B(Rl)\{f>a\}\in\mathcal{B}(\mathbb{R}^{l}) for every real aa (Measure Spaces and the Lebesgue Integral: Standing Notation §measurable).

Claim A (Composition). If S:RpRmS:\mathbb{R}^{p}\to\mathbb{R}^{m} is measurable with respect to B(Rp)\mathcal{B}(\mathbb{R}^{p}) and B(Rm)\mathcal{B}(\mathbb{R}^{m}) and h:Rm[0,]h:\mathbb{R}^{m}\to[0,\infty] is Borel, then hSh\circ S is Borel: for real aa, {hS>a}=S1({h>a})B(Rp)\{h\circ S>a\}=S^{-1}(\{h>a\})\in\mathcal{B}(\mathbb{R}^{p}) by Measurable Function and Real-Valued Measurable Function.

Claim B (Arithmetic in [0,][0,\infty]). For positive reals a,ba,b and I[0,]I\in[0,\infty] we have a(bI)=(ab)Ia(bI)=(ab)I and a(a1I)=Ia(a^{-1}I)=I: for finite II this is field arithmetic, and for I=I=\infty both sides are \infty by the convention a=a\cdot\infty=\infty for 0<a0<a of Measure Spaces and the Lebesgue Integral: Standing Notation §extended (with 0<ab0<ab and 0<a10<a^{-1} by claims 5 and 7 of Elementary Order Arithmetic in an Ordered Field).

Step 1 (Proof of Lebesgue Measure under a Triangular or Symmetric Positive Definite Linear Map §borel). Let TT be a real d×dd\times d matrix. By claim 3 of Linearity, Compatibility with the Matrix Product, and a Norm Bound for the Matrix-Vector Product there is a real C0C\ge0 with TvCv\lVert Tv\rVert\le C\lVert v\rVert for all vRdv\in\mathbb{R}^{d}, and TxTy=T(xy)Tx-Ty=T(x-y) by claim 1 there, so TxTyCxy\lVert Tx-Ty\rVert\le C\lVert x-y\rVert. Since dE(x,y)=xyd_{E}(x,y)=\lVert x-y\rVert (claim 2 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n), xTxx\mapsto Tx is Lipschitz with constant CC, hence continuous by A Lipschitz Map is Uniformly Continuous. For i[d]i\in[d] the component x(Tx)ix\mapsto(Tx)_{i} satisfies (Tx)i(Ty)iTxTyCxy|(Tx)_{i}-(Ty)_{i}|\le\lVert Tx-Ty\rVert\le C\lVert x-y\rVert by claim 4 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n. On R=R1\mathbb{R}=\mathbb{R}^{1} the Euclidean distance is st|s-t|: for uR1u\in\mathbb{R}^{1}, u2=u2=u2\lVert u\rVert^{2}=u^{2}=|u|^{2} by claim 1 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n and claim 1 of Properties of the Absolute Value in an Ordered Field, both u\lVert u\rVert and u|u| are nonnegative, so u=u\lVert u\rVert=|u| by claim 3 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field. Hence each component is Lipschitz, so continuous (A Lipschitz Map is Uniformly Continuous), from (Rd,dE)(\mathbb{R}^{d},d_{E}) to (R,dE)(\mathbb{R},d_{E}), and therefore measurable with respect to Bd\mathcal{B}_{d} and B(R)\mathcal{B}(\mathbb{R}) by claim 3(a) of The Borel Sigma-Algebra of a Euclidean Space as a Product, and Measurability of Projections, Sequentially Continuous Maps, and Open and Closed Sets. By claim 2 there (with (X,F)=(Rd,Bd)(X,\mathcal{F})=(\mathbb{R}^{d},\mathcal{B}_{d})), xTxx\mapsto Tx is measurable with respect to Bd\mathcal{B}_{d} and Bd\mathcal{B}_{d}, that is, Borel, as Bd=B(Rd)\mathcal{B}_{d}=\mathcal{B}(\mathbb{R}^{d}).

Step 2 (Positivity of triangular determinants). Let TT be a lower or upper triangular real l×ll\times l matrix with 0<Tkk0<T_{kk} for all k[l]k\in[l]. By claim 1 or claim 2 of The Determinant of a Triangular Matrix is the Product of its Diagonal Entries, whose determinant is that of Determinant of a Real Square Matrix by Row Properties of the Determinant, detT=k=1lTkk\det T=\prod_{k=1}^{l}T_{kk}. By the recursion in claim 1 of Properties of Finite Products and claim 5 of Elementary Order Arithmetic in an Ordered Field, induction on the number of factors gives 0<detT0<\det T. This proves the first assertion of Lebesgue Measure under a Triangular or Symmetric Positive Definite Linear Map §triangular. If l2l\ge2, let TT' be the (l1)×(l1)(l-1)\times(l-1) matrix with Tij=TijT'_{ij}=T_{ij} for i,j[l1]i,j\in[l-1]; it is triangular of the same kind with the same first l1l-1 diagonal entries, and by The Determinant of a Triangular Matrix is the Product of its Diagonal Entries and claim 1 of Properties of Finite Products (restriction and recursion),

detT=detTTll.\det T=\det T'\cdot T_{ll}.

Step 3 (Splitting off the last coordinate). Let l2l\ge2, TT and TT' as in Step 2, and x=(x,xl)Rlx=(x',x_{l})\in\mathbb{R}^{l}. By Matrix-Vector Product and the recursion in claim 1 of Properties of Finite Sums, (Tx)i=j=1l1Tijxj+Tilxl(Tx)_{i}=\sum_{j=1}^{l-1}T_{ij}x_{j}+T_{il}x_{l} for every i[l]i\in[l], and j=1l1Tijxj=(Tx)i\sum_{j=1}^{l-1}T_{ij}x_{j}=(T'x')_{i} for il1i\le l-1.

If TT is lower triangular, then Til=0T_{il}=0 for i<li<l, so, with β(x)=j=1l1Tljxj\beta(x')=\sum_{j=1}^{l-1}T_{lj}x_{j},

Tx=(Tx,  Tllxl+β(x)).Tx=\bigl(T'x',\;T_{ll}x_{l}+\beta(x')\bigr).

If TT is upper triangular, then Tlj=0T_{lj}=0 for j<lj<l, so j=1l1Tljxj=0\sum_{j=1}^{l-1}T_{lj}x_{j}=0 (claim 3 of Properties of Finite Sums with λ=0\lambda=0), and, with b=(T1l,,Tl1,l)Rl1b=(T_{1l},\dots,T_{l-1,l})\in\mathbb{R}^{l-1} and the sum and scalar multiple of Rl1\mathbb{R}^{l-1} taken coordinatewise,

Tx=(Tx+xlb,  Tllxl).Tx=\bigl(T'x'+x_{l}b,\;T_{ll}x_{l}\bigr).

Step 4 (Proof of the integral identity in Lebesgue Measure under a Triangular or Symmetric Positive Definite Linear Map §triangular). We prove by induction on l1l\ge1 the statement P(l)P(l): for every lower or upper triangular real l×ll\times l matrix TT with positive diagonal entries and every Borel f:Rl[0,]f:\mathbb{R}^{l}\to[0,\infty], detTRlf(Tx)dλl(x)=Rlfdλl\det T\int_{\mathbb{R}^{l}}f(Tx)\,d\lambda_{l}(x)=\int_{\mathbb{R}^{l}}f\,d\lambda_{l}. Here fTf\circ T is Borel by Claim A and Step 1, so the left integral is defined. Then P(d)P(d) is the claim.

Base case l=1l=1. Here T=(t)T=(t) with t=T11>0t=T_{11}>0, Tx=txTx=tx by Matrix-Vector Product and claim 1 of Properties of Finite Sums, and detT=t\det T=t by Step 2 and claim 1 of Properties of Finite Products. By claim 2 of Scaling of Lebesgue Measure and the Lebesgue Integral on Rn\mathbb{R}^n with n=1n=1 and c=tc=t, where t1=t=t|t|^{1}=|t|=t by Natural Number Power of an Element of a Field, claim 1 of Properties of Finite Products and Absolute Value in an Ordered Field,

Rf(tx)dλ(x)=t1Rfdλ,\int_{\mathbb{R}}f(tx)\,d\lambda(x)=t^{-1}\int_{\mathbb{R}}f\,d\lambda ,

and multiplying by tt gives P(1)P(1) by Claim B.

Inductive step. Let l2l\ge2 and assume P(l1)P(l-1). Let TT and ff be as in P(l)P(l), let TT' be as in Step 2, and put H=fTH=f\circ T, Borel on Rl=Rl1×R\mathbb{R}^{l}=\mathbb{R}^{l-1}\times\mathbb{R}. We apply Tonelli and Fubini Theorems with (X,F,μ)=(Rl1,Bl1,λl1)(X,\mathcal{F},\mu)=(\mathbb{R}^{l-1},\mathcal{B}_{l-1},\lambda_{l-1}) and (Y,G,ν)=(R,B(R),λ)(Y,\mathcal{G},\nu)=(\mathbb{R},\mathcal{B}(\mathbb{R}),\lambda), both σ\sigma-finite, to HH and to ff, which are Bl1B(R)\mathcal{B}_{l-1}\otimes\mathcal{B}(\mathbb{R})-measurable.

Lower triangular TT. By the Tonelli part of Tonelli and Fubini Theorems and Step 3,

RlHdλl=Rl1(Rf(Tx,Tllt+β(x))dλ(t))dλl1(x).\int_{\mathbb{R}^{l}}H\,d\lambda_{l}=\int_{\mathbb{R}^{l-1}}\Bigl(\int_{\mathbb{R}}f\bigl(T'x',T_{ll}t+\beta(x')\bigr)\,d\lambda(t)\Bigr)d\lambda_{l-1}(x').

Fix xx'. The section k(s)=f(Tx,s)k(s)=f(T'x',s) is B(R)\mathcal{B}(\mathbb{R})-measurable by the sections part of Tonelli and Fubini Theorems. By claim 2 of Translation and Reflection Invariance of Lebesgue Measure on Rn\mathbb{R}^n with n=1n=1 and a=β(x)a=\beta(x'), k1(s)=k(s+β(x))k_{1}(s)=k(s+\beta(x')) is measurable with Rk1dλ=Rkdλ\int_{\mathbb{R}}k_{1}\,d\lambda=\int_{\mathbb{R}}k\,d\lambda, and by claim 2 of Scaling of Lebesgue Measure and the Lebesgue Integral on Rn\mathbb{R}^n with n=1n=1 and c=Tllc=T_{ll} (as in the base case), Rk1(Tllt)dλ(t)=Tll1Rk1dλ\int_{\mathbb{R}}k_{1}(T_{ll}t)\,d\lambda(t)=T_{ll}^{-1}\int_{\mathbb{R}}k_{1}\,d\lambda. As k1(Tllt)=f(Tx,Tllt+β(x))k_{1}(T_{ll}t)=f(T'x',T_{ll}t+\beta(x')), the inner integral equals Tll1g(Tx)T_{ll}^{-1}g(T'x'), where g(z)=Rf(z,s)dλ(s)g(z')=\int_{\mathbb{R}}f(z',s)\,d\lambda(s) defines a Bl1\mathcal{B}_{l-1}-measurable g:Rl1[0,]g:\mathbb{R}^{l-1}\to[0,\infty] by the Tonelli part of Tonelli and Fubini Theorems. The map gTg\circ T' is Borel (Claim A and Step 1), so claim 1 of Linearity and Monotonicity of the Lebesgue Integral with the constant Tll1T_{ll}^{-1} gives RlHdλl=Tll1Rl1g(Tx)dλl1(x)\int_{\mathbb{R}^{l}}H\,d\lambda_{l}=T_{ll}^{-1}\int_{\mathbb{R}^{l-1}}g(T'x')\,d\lambda_{l-1}(x'). By P(l1)P(l-1) applied to TT' and gg, and the Tonelli part of Tonelli and Fubini Theorems applied to ff,

detTRl1g(Tx)dλl1(x)=Rl1gdλl1=Rlfdλl.\det T'\int_{\mathbb{R}^{l-1}}g(T'x')\,d\lambda_{l-1}(x')=\int_{\mathbb{R}^{l-1}}g\,d\lambda_{l-1}=\int_{\mathbb{R}^{l}}f\,d\lambda_{l}.

Using detT=detTTll\det T=\det T'\cdot T_{ll} (Step 2) and Claim B, detTHdλl=detTTll(Tll1gTdλl1)=detTgTdλl1=fdλl\det T\int H\,d\lambda_{l}=\det T'\cdot T_{ll}\bigl(T_{ll}^{-1}\int g\circ T'\,d\lambda_{l-1}\bigr)=\det T'\int g\circ T'\,d\lambda_{l-1}=\int f\,d\lambda_{l}.

Upper triangular TT. By the Tonelli part of Tonelli and Fubini Theorems, in the other order, and Step 3,

RlHdλl=R(Rl1f(Tx+tb,Tllt)dλl1(x))dλ(t).\int_{\mathbb{R}^{l}}H\,d\lambda_{l}=\int_{\mathbb{R}}\Bigl(\int_{\mathbb{R}^{l-1}}f\bigl(T'x'+tb,\,T_{ll}t\bigr)\,d\lambda_{l-1}(x')\Bigr)d\lambda(t).

Fix tt. The section k(z)=f(z,Tllt)k(z')=f(z',T_{ll}t) is Bl1\mathcal{B}_{l-1}-measurable by the sections part of Tonelli and Fubini Theorems. By claim 2 of Translation and Reflection Invariance of Lebesgue Measure on Rn\mathbb{R}^n with n=l1n=l-1 and a=tba=tb, k2(z)=k(z+tb)k_{2}(z')=k(z'+tb) is measurable with k2dλl1=kdλl1\int k_{2}\,d\lambda_{l-1}=\int k\,d\lambda_{l-1}. The inner integrand is k2(Tx)k_{2}(T'x'), and k2Tk_{2}\circ T' is Borel (Claim A, Step 1); by P(l1)P(l-1) applied to TT' and k2k_{2},

detTRl1k2(Tx)dλl1(x)=Rl1kdλl1=g(Tllt),g(s)=Rl1f(z,s)dλl1(z),\det T'\int_{\mathbb{R}^{l-1}}k_{2}(T'x')\,d\lambda_{l-1}(x')=\int_{\mathbb{R}^{l-1}}k\,d\lambda_{l-1}=g(T_{ll}t),\qquad g(s)=\int_{\mathbb{R}^{l-1}}f(z',s)\,d\lambda_{l-1}(z'),

where g:R[0,]g:\mathbb{R}\to[0,\infty] is B(R)\mathcal{B}(\mathbb{R})-measurable by the Tonelli part of Tonelli and Fubini Theorems. By Claim B the inner integral equals (detT)1g(Tllt)(\det T')^{-1}g(T_{ll}t). The map tg(Tllt)t\mapsto g(T_{ll}t) is measurable by claim 2 of Scaling of Lebesgue Measure and the Lebesgue Integral on Rn\mathbb{R}^n, so by claim 1 of Linearity and Monotonicity of the Lebesgue Integral, claim 2 of Scaling of Lebesgue Measure and the Lebesgue Integral on Rn\mathbb{R}^n (with n=1n=1, c=Tllc=T_{ll}) and the Tonelli part of Tonelli and Fubini Theorems,

RlHdλl=(detT)1Rg(Tllt)dλ(t)=(detT)1(Tll1Rgdλ)=(detT)1(Tll1Rlfdλl).\int_{\mathbb{R}^{l}}H\,d\lambda_{l}=(\det T')^{-1}\int_{\mathbb{R}}g(T_{ll}t)\,d\lambda(t)=(\det T')^{-1}\Bigl(T_{ll}^{-1}\int_{\mathbb{R}}g\,d\lambda\Bigr)=(\det T')^{-1}\Bigl(T_{ll}^{-1}\int_{\mathbb{R}^{l}}f\,d\lambda_{l}\Bigr).

Multiplying by detT=detTTll\det T=\det T'\cdot T_{ll} and using Claim B gives detTHdλl=fdλl\det T\int H\,d\lambda_{l}=\int f\,d\lambda_{l}. This proves P(l)P(l) and completes the induction.

Step 5 (Proof of Lebesgue Measure under a Triangular or Symmetric Positive Definite Linear Map §spd). Let AS(d)A\in\mathcal{S}(d) be positive definite. By Cholesky Factorisation of a Symmetric Positive Definite Real Matrix there is a lower triangular real d×dd\times d matrix LL with 0<Lii0<L_{ii} for all ii and A=LLA=LL^{\top}. Put U=LU=L^{\top}; by Transpose of a Real Matrix, Uij=LjiU_{ij}=L_{ji}, which is 00 when j<ij<i, and Uii=Lii>0U_{ii}=L_{ii}>0, so UU is upper triangular with positive diagonal. By The Determinant is Multiplicative, Step 2 and claim 5 of Elementary Order Arithmetic in an Ordered Field, detA=detLdetU>0\det A=\det L\cdot\det U>0.

By claim 2 of Linearity, Compatibility with the Matrix Product, and a Norm Bound for the Matrix-Vector Product, Ax=(LU)x=L(Ux)Ax=(LU)x=L(Ux). Let f:Rd[0,]f:\mathbb{R}^{d}\to[0,\infty] be Borel; fLf\circ L is Borel by Claim A and Step 1. By Lebesgue Measure under a Triangular or Symmetric Positive Definite Linear Map §triangular (proved in Step 4) applied to UU and fLf\circ L, and then to LL and ff,

detURdf(Ax)dλd(x)=RdfLdλd,detLRdfLdλd=Rdfdλd,\det U\int_{\mathbb{R}^{d}}f(Ax)\,d\lambda_{d}(x)=\int_{\mathbb{R}^{d}}f\circ L\,d\lambda_{d},\qquad\det L\int_{\mathbb{R}^{d}}f\circ L\,d\lambda_{d}=\int_{\mathbb{R}^{d}}f\,d\lambda_{d},

so by Claim B, detAf(Ax)dλd(x)=detL(detUf(Ax)dλd(x))=fdλd\det A\int f(Ax)\,d\lambda_{d}(x)=\det L\bigl(\det U\int f(Ax)\,d\lambda_{d}(x)\bigr)=\int f\,d\lambda_{d}.

By Invertibility of Symmetric Positive Definite Matrices, AA is invertible. For yRdy\in\mathbb{R}^{d}, claim 2 of Linearity, Compatibility with the Matrix Product, and a Norm Bound for the Matrix-Vector Product gives A(A1y)=(AA1)y=Idy=yA(A^{-1}y)=(AA^{-1})y=I_{d}y=y and likewise A1(Ay)=yA^{-1}(Ay)=y, where (Idy)i=jδijyj=yi(I_{d}y)_{i}=\sum_{j}\delta_{ij}y_{j}=y_{i} by Identity Matrix, Matrix-Vector Product and claim 7 of Properties of Finite Sums. Hence xAxx\mapsto Ax is a bijection of Rd\mathbb{R}^{d} onto Rd\mathbb{R}^{d} with inverse yA1yy\mapsto A^{-1}y.

Let BB(Rd)B\in\mathcal{B}(\mathbb{R}^{d}). Then yA(B)y\in A(B) if and only if A1yBA^{-1}y\in B, so A(B)A(B) is the preimage of BB under yA1yy\mapsto A^{-1}y, which is Borel by Step 1; thus A(B)B(Rd)A(B)\in\mathcal{B}(\mathbb{R}^{d}). The indicator f=1A(B)f=\mathbf{1}_{A(B)} is Borel (each set {f>a}\{f>a\} is Rd\mathbb{R}^{d}, A(B)A(B) or \emptyset), and f(Ax)=1B(x)f(Ax)=\mathbf{1}_{B}(x) for all xx, by injectivity. The identity just proved and The Integral of an Indicator Function is the Measure of the Set give detAλd(B)=λd(A(B))\det A\,\lambda_{d}(B)=\lambda_{d}(A(B)).

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