364 CHAPTER 13. LEBESGUE MEASURE

where Φ is a continuous function of φ⃗ and θ .1 Then if f is nonnegative and Lebesguemeasurable,∫

Rpf (y)dmp =

∫hp(A)

f (y)dmp =∫

Af(

hp

(⃗φ ,θ ,ρ

))ρ

p−1Φ

(⃗φ ,θ

)dmp (13.9.21)

Furthermore whenever f is Borel measurable and nonnegative, one can apply Fubini’stheorem and write∫

Rpf (y)dy =

∫∞

p−1∫

Af(

h(⃗

φ ,θ ,ρ))

Φ

(⃗φ ,θ

)dφ⃗dθdρ (13.9.22)

where here dφ⃗ dθ denotes dmp−1 on A. The same formulas hold if f ∈ L1 (Rp) .

Proof: Formula 13.9.20 is obvious from the definition of the spherical coordinatesbecause in the matrix of the derivative, there will be a ρ in p−1 columns. The first claimis also clear from the definition and math induction or from the geometry of the abovedescription. It remains to verify 13.9.21 and 13.9.22. It is clear hp maps Ā× [0,∞) ontoRp. Since hp is differentiable, it maps sets of measure zero to sets of measure zero. Then

Rp = hp (N∪A× (0,∞)) = hp (N)∪hp (A× (0,∞)) ,

the union of a set of measure zero with hp (A× (0,∞)) . Therefore, from the change ofvariables formula,∫

Rpf (y)dmp =

∫hp(A×(0,∞))

f (y)dmp

=∫

A×(0,∞)f(

hp

(⃗φ ,θ ,ρ

))ρ

p−1Φ

(⃗φ ,θ

)dmp

which proves 13.9.21. This formula continues to hold if f is in L1 (Rp). Finally, if f ≥ 0or in L1 (Rn) and is Borel measurable, then it is F p measurable as well. Recall that F p

includes the smallest σ algebra which contains products of open intervals. Hence F p

includes the Borel sets B (Rp). Thus from the definition of mp∫A×(0,∞)

f(

hp

(⃗φ ,θ ,ρ

))ρ

p−1Φ

(⃗φ ,θ

)dmp

=∫(0,∞)

∫A

f(

hp

(⃗φ ,θ ,ρ

))ρ

p−1Φ

(⃗φ ,θ

)dmp−1dm

=∫(0,∞)

ρp−1

∫A

f(

hp

(⃗φ ,θ ,ρ

))Φ

(⃗φ ,θ

)dmp−1dm

Now the claim about f ∈ L1 follows routinely from considering the positive and negativeparts of the real and imaginary parts of f in the usual way.

1Actually it is only a function of the first but this is not important in what follows.

364 CHAPTER 13. LEBESGUE MEASUREwhere ® is a continuous function of d and @.' Then if f is nonnegative and Lebesguemeasurable,[,fodame= [iF aiamy = | F (hn (9.8.0) 0” '&(4.8) amp 139.21)Furthermore whenever f is Borel measurable and nonnegative, one can apply Fubini’stheorem and write[ fyav= [pr | r(n (9.0.p) ) (4,6) ddaedp (13.9.22)where here do d@ denotes dmp_, on A. The same formulas hold if f € L' (R?).Proof: Formula 13.9.20 is obvious from the definition of the spherical coordinatesbecause in the matrix of the derivative, there will be a p in p—1 columns. The first claimis also clear from the definition and math induction or from the geometry of the abovedescription. It remains to verify 13.9.21 and 13.9.22. It is clear h, maps A x [0,°°) ontoR?. Since hp is differentiable, it maps sets of measure zero to sets of measure zero. ThenR? = hy (NUA x (0,2) =hy (N) Uhy (A x (0,2),the union of a set of measure zero with h, (A x (0,°°)). Therefore, from the change ofvariables formula,dm, = I dapt (y)dmp hy(ave(0ve)) (y)dmpIreoayt ($.0.p)) p? (9.0) ampwhich proves 13.9.21. This formula continues to hold if f is in L! (IR”). Finally, if f > 0or in L! (IR”) and is Borel measurable, then it is 4? measurable as well. Recall that F?includes the smallest o algebra which contains products of open intervals. Hence ¥?includes the Borel sets A(R”). Thus from the definition of m,Dow! (h, (9.6.0) p?'® (3.0) dmp[on Li (m (9.0.9) )p” '® (4,0) dmp—1dm[0° [Fl (4.0.p))®(4,0) dmp1dmNow the claim about f € L! follows routinely from considering the positive and negativeparts of the real and imaginary parts of f in the usual way. J' Actually it is only a function of the first but this is not important in what follows.