Homepage Solution manuals Terence Tao An Introduction to Measure Theory Exercise 1.1.11 (Jordan measure and linear transformations)

Exercise 1.1.11 (Jordan measure and linear transformations)

Let L : d d be a linear transformation.

(i)
Show that there exists a non-negative real number D such that fon every elementary set E we have m(L(E)) = D m(E)

(why is L(E) Jordan measurable?)

(ii)
Show that if E is Jordan measurable, then L(E) is alse, and m(L(E)) = D m(E).

(iii)
Show that D = |det (L)|.

Answers

Pick an arbitrary Jordan measurable set E d. By Exercise 1.1.5 this is equivalent to the fact that for any 𝜖 > 0 we can find two elementary sets E1,E2 d such that

E1 E E2,m(E2) m(E1) 𝜖 det (T)

This implies

T(E1) T(E) T(E2)

If we manage to demonstrate that T(E1) and T(E2) are elementary as well, with m(T(E2)) m(T(E1)) = det (T) (m(E1) m(E2)) 𝜖, then we are done. Thus, it suffices to prove the theorem assertion only for elementary sets. By Lemma 1.1.2 we can write represent an elementary set E as a disjoint union of boxes E = n=1NEn. Knowing that a finite union of Jordan measurable sets T( n=1NBn) = n=1NT(Bn) is again Jordan measurable by Exercise 1.1.6, it is sufficient to demonstrate that T(Bn) is Jordan measurable for any box Bn.

We use the strategy of expanding the proof to an always more general case with respect to the type of T.

(i)
T is an elementary linear transformation
We have further three cases (we only consider the cases with respect to matrix rows; the cases with columns follow analogously):
  • T is a Type I linear transformation
    In other words, T exchanges any two rows i,j of a point, and it can be represented by a matrix which is an identity matrix with rows i and j switched:

    [T] = [ 1 0 1 1 0 1 ]

    Notice that T transforms any box B = [a1,b1] × × [ad,bd] into another box, which is Jordan measurable; namely, it is easy to verify pointwise that

    T ([a1,b1] × × [ai,bi] × × [aj,bj] × × [ad,bd]) = [a1,b1] × × [aj,bj] × × [ai,bi] × × [ad,bd].

    It is only left to demonstrate how T changes the magnitude of the Jordan measure:

    B boxes(d) : m(T(B)) = |det T|× m(B).

    But this follows directly from the fact that T only switches two intervals of B; thus, leaving the measure of T(B) unchanged. Since det (T) = 1 (Linear Algebra, Theorem 4.5), and thus m(T(B)) = m(B) 1.

  • T is a Type II linear transformation
    Now suppose that T multiplies the ith row of the input with a non-zero scalar k, i.e.,

    [ 1 1 k 1 1 ]

    Then it is easy to verify pointwise that

    T ([a1,b1] × × [ai,bi] × × [ad,bd]) = [a1,b1] × × [kai,kbi] × × [ad,bd].

    As it was in the previous case, T maps a box to a box, which is Jordan measurable. We need to demonstrate the change in the magnitude of the Jordan measure:

    B boxes(d) : m(T(B)) = |det T|× m(B).

    But this follows directly from the fact that T only enlarges the Ii interval of B; thus, leaving the measure of m(T(B)) = (b1 a1) (kbi kai) (bd ad) = k m(B). Since det (T) = m (Linear Algebra, Theorem 4.6), the assertion follows.

  • T is a Type III linear transformation
    In other words, T adds a row i of the input to its another row j.

    [ 1 1 1 1 1 ]

    In this case, T does not map a box into another box; we have to improvise here. The trick is to look closer at what T maps a box into (the answer is parallelepiped). If the image is Jordan measurable, then we can simply spend another 𝜖 and approximate this set by another elementary set from below (in case the elementary set is E1) or from above (in case the elementary set is E2). If we denote by T1(i,j) an elementary linear transformation that interchanges ith and jth columns, then:

    T(B) = { (x1,x2,,xi,,xi + xj,,xd) : xl [al,bl]} = Ti,11T j,21 { (x i,xi + xj,x1,,x2,,xd) : xl [al,bl]} = Ti,11T j,21 { (x,x + y) : x I i,y Ij} × I3 × × Ii1× × I1 × Ii+1 × Ij1 × I2 × Ij+1 × × Id

    This representation has nice properties. Since T1 is proven to map a Jordan measurable set to a Jordan measurable set, while preserving the original volume, it suffices to demonstrate that the set

    { (x,x + y) : x Ii,y Ij}×I3××Ii1×I1×Ii+1×Ij1×I2×Ij+1××Id

    is Jordan measurable, and has a measure equal to the original set. Knowing how Jordan measure interacts with Cartesian products from Exercise 1.1.16, it suffices to demonstrate that the parallelepiped in 2 given by

    { (x,x + y) : x Ii,y Ij}

    is Jordan measurable.

         
    Figure 1: Parrallepiped as a disjoint union of two triangles and a box, and its generalisation to higher dimensions.

    Assuming b1 < b1 without loss of generality, it can be tediously verified (exercise) that a parallelepiped can be partitioned into two triangles and a box.

    { (x,x + y) : x Ii,y Ij} = ((a1,a1 + a2) (a1,a2 + b1) (b1,a2 + b1)) [a1,b1] × [a2 + b1,b2 + a1] ((a1,b2 + a1) (b1,b2 + b1) (b1,b2 + b1))

    Since all of these figures are Jordan measurable by Exercise 1.1.8, their union must be Jordan measurable as well, and its measure is

    m ( { (x,x + y) : x Ii,y Ij}) = (b1 a1) (b2 a2).

    Hence, the set

    { (x,x + y) : x Ii,y Ij}×I3××Ii1×I1×Ii+1×Ij1×I2×Ij+1××Id

    is Jordan measurable, with a measure of det (T)m(B) = m(B) by Exercise 1.1.16. The rest of the proof can be finished by choosing an elementary set with covers from inner and from outer, and by adjusting 𝜖 accordingly.

(ii)
T is an invertible linear transformation.
By Linear Algebra, Corollary 3.6 (3), T can be represented as a sequence of elementary transformations T = T1Tn. On one hand, by Theorem 4.7 we have det (T) = det (T1) det (Tn). On the other hand, by the previous part of this exercise m(T(B)) = m(T1((Tn(B)))) = det (T1)( (det (Tn)m(B))) = det (T1) det (Tn)m(B), and we are done.
(iii)
T is a linear transformation.only class of linear transformation for which the theorem assertion is left to verify are non-invertible linear transformations. Recall from Linear Algebra, Theorem 3.6., that using elementary linear transformations T1,,Tn we can transform T into a block matrix of the form T = T1Tn [ Ir×r 0r×(dr) 0(dr)×r0(dr)×(dr) ] ,

where Ir×r is an identity matrix of size r, and the rest are zero matrices. The last block matrix Tn+1 will send any box into a lower dimensional box

Tn+1(B) = Tn+1 ([a1,b1] × × [ar,br] × × [ad,bd]) = [a1,b1]××[ar,br]×{0}××{0}

and the Jordan measure of the above box is obviously zero. On one hand, applying the elementary transformations T1Tn to obtain the end result will only multiply the sets Jordan measure by scaled determinants, so the result will remain zero. Hence, m(T(B)) = 0. On the other hand, the determinant of the non-invertible linear transformation is zero det (T) = 0 (Linear Algebra, Corollary 4.7), and we are done.

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2020-08-20 00:00
Comments

Proof. If E is an elementary set, then L(E) is Jordan measurable. Indeed, recall that any invertible matrix L can be written as a product of elementary operation matrices: L = T1Tn where each Tj is either multiplication of a row by a scalar c, addition of one row to another row, or swapping of two rows. That is, Tj is in one of the following families of matrices:

Mc,j = [ 10 0 c 0 1 ]Ri,j = [ 10 0 01 0 1 ]Si,j = [ 10 0 01 1 0 0 1 ]

That is Mc,j is obtain by multiplying the j-th row of the identity matrix by c;Ri,j is obtained by adding the i-th row in the identity matrix to the j-th row; Si,j is obtained by swapping the i-th and j-th rows of the identity matrix.

It is immediate to compute that det Mc,j = c, |det Ri,j| = |det Si,j| = 1. Also, if B = I1 × × Id we have that Mc,j(B) = I1 × × cIj × × Id and for i < j, Si,j(B) = I1 ×Ij × × Ii × × Id. Thus, we have that for any box B, and any linear map L {Mc,j,Si,j} ,m(L(B)) = |det L| m(B). If E = B1 Bk is an elementary set, where (Bj) j=1k are boxes, then L(E) = L (B1) L (Bk), so L(E) is an elementary set and

m(L(E)) = j=1km (L (B j)) = j=1k|det L| m (B j) = |det L| m(E)

Finally, if A is Jordan measurable, the for any 𝜀 > 0 choose elementary sets E A F such that m(F) < m(E) + 𝜀. So, L(E) L(A) L(F) and

J(L(A)) m(L(F)) = |det L| m(F) |det L| m(E) + |det L| 𝜀 |det L| J(A) + |det L| 𝜀 |det L| m(F) + |det L| 𝜀 |det L| m(E) + |det L| 2𝜀 = m(L(E)) + |det L| 2𝜀 J(L(A)) + |det L| 2𝜀

Taking 𝜀 0 we have that J(L(A)) = J(L(A)) = |det L| J(A). This proves the theorem for the case that L {Mc,j,Si,j}.

Now for a somewhat more cumbersome computation:

Ri,j(B) = { (x1,,xi,,xi + xj,,xd) d : k,x k Ik}

which is the Cartesian product of the parallelepiped {(x,x + y) : x Ii,y Ij} with a box in d2. Indeed, if we apply S = Si,1Sj,2 to this set,

Ri,j(B) = { (x1,,xi,,xi + xj,,xd) d : k,x k Ik} = S { (xi,xi + xj,x3,,xi1,x1,xi+1,,xj1,x2,xj+1,,xd) d : k,x k Ik} = S ( {(x,x + y) : x Ii,y Ij} × I3 ×Ii1 × I1 × Ii+1 × × Ij1 × Ij × Ij+1 × × Id) .

Since S preserves Jordan measure (and measurability), it suffices to show the Jordan measurability of P := {(x,x + y) : x Ii,y Ij} and compute its Jordan measure. By translating P we may assume without loss of generality that the endpoints of Ii are 0 < a and the endpoints of Ij are 0,b. We may also write P = T1 B T2 where T1,T2 are right-angle triangles, with orthogonal sides parallel to the axes, and B is a box, as in Figure 1 In a previous exercise it was shown that triangles are Jordan measurable. A translation of T2 by the vector (0,b) shows that T1 T2 has the Jordan measure of the box Ii × Ii. Thus, P is Jordan measurable and has Jordan measure J(P) = |Ii| |Ij|, which consequently is J(P) = m (Ii × Ij).

PIC
Figure 1: Computation of the Jordan measure of the parallelepiped P.

Lemma 1. Let P = {(x,x + y) : x I,y J}, where I and J are intervals. Then P is Jordan measurable and that m(P) = |I|×|J|.

We conclude that Ri,j(B) is Jordan measurable, and that J (Ri,j(B)) = J(S(P ×B)) = J(P ×B) = J2(P)Jd2(B) = |Ii| |Ij| ki,j |Ik| = m(B), where P = {(x,x + y) : x Ii,y Ij} and B = I3 ×Ii1 × I1 × Ii+1 × × Ij1× Ij × Ij+1 × × Id d2. Since |det Ri,j| = 1 we have just proved that for any box B, the set Ri,j(B) is Jordan measurable and J (Ri,j(B)) = |det Ri,j| m(B).

Just as for Mc,j and Si,j we now use the fact that Ri,j(A B) = Ri,j(A) Ri,j(B) to prove the theorem for any L {Mc,j,Si,j,Ri,j}.

Finally, if L is a general invertible linear map, then L = L1Ln where Lk {Mc,j,Si,j,Ri,j} for all k. So for any A that is Jordan measurable, also Ln(A) is Jordan measurable, and thus Ln1Ln(A) is as well, and so on to get that L(A) = L1Ln(A) is Jordan measurable. We also compute the measure by

J(L(A)) = J (L1 (L2Ln(A))) = |det L1| J (L2Ln(A)) = = = |det L1| |det Ln| J(A) = |det L| J(A).

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2021-12-04 16:55
Comments
  • You did not address the non-invertible case.
    isn2024-12-11