256 CHAPTER 10. REGULAR MEASURES

which proves 10.10. This formula continues to hold if f is in L1 (Rp) by consideration ofpositive and negative parts of real and imaginary parts.

Finally, if f ≥ 0 or in L1 (Rn) and is Borel measurable, the Borel sets denoted as B (Rp)then one can write the following. 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. ■

Note that the above equals∫

Ā×[0,∞) f(hp

(⃗φ ,θ ,ρ

))ρ p−1Φ

(⃗φ ,θ

)dmp and the iter-

ated integral is also equal to∫[0,∞)

ρp−1

∫Ā

f(hp

(⃗φ ,θ ,ρ

))Φ

(⃗φ ,θ

)dmp−1dm

because the difference is just a set of measure zero.

Notation 10.9.2 Often this is written differently. Note that from the spherical coordinateformulas, f

(h(⃗

φ ,θ ,ρ))

= f (ρω) where |ω| = 1. Letting Sp−1 denote the unit sphere,{ω ∈ Rp : |ω|= 1} , the inside integral in the above formula is sometimes written as∫

Sp−1f (ρω)dσ

where σ is a measure on Sp−1. See “Real and Abstract Analysis” for another descriptionof this measure. It isn’t an important issue here. Either 10.11 or the formula∫

p−1(∫

Sp−1f (ρω)dσ

)dρ

will be referred to as polar coordinates and is very useful in establishing estimates. Hereσ(Sp−1

)≡∫

A Φ

(⃗φ ,θ

)dmp−1.

Example 10.9.3 For what values of s is the integral∫

B(0,R)

(1+ |x|2

)sdy bounded inde-

pendent of R? Here B(0,R) is the ball, {x ∈ Rp : |x| ≤ R} .

I think you can see immediately that s must be negative but exactly how negative? Itturns out it depends on p and using polar coordinates, you can find just exactly what isneeded. From the polar coordinates formula above,∫

B(0,R)

(1+ |x|2

)sdy =

∫ R

0

∫Sp−1

(1+ρ

2)sρ

p−1dσdρ

= Cp

∫ R

0

(1+ρ

2)sρ

p−1dρ

Now the very hard problem has been reduced to considering an easy one variable prob-lem of finding when

∫ R0 ρ p−1

(1+ρ2

)s dρ is bounded independent of R. You need 2s+(p−1)<−1 so you need s <−p/2.

256 CHAPTER 10. REGULAR MEASURESwhich proves 10.10. This formula continues to hold if f is in L! (R?) by consideration ofpositive and negative parts of real and imaginary parts.Finally, if f > 0 or in L! (R”) and is Borel measurable, the Borel sets denoted as & (R”)then one can write the following. From the definition of mp[cout (Pe (9.6.0) ) p? (9.6) dmy[on fi (t (3.0.p) )p” ' (4.0) dmy—dm[Le lm (4.0.p)) (4,6) dmp jdmNow 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.Note that the above equals JAx[0,00) f (rp (6. 6.p)) p?-'® (6. 0) dm, and the iter-ated integral is also equal toI. pP-! [es (rp (9.6,p)) ® (6. ) dimy_dmbecause the difference is just a set of measure zero.Notation 10.9.2 Often this is written differently. Note that from the spherical coordinateformulas, f (n (9.6.p)) = f (pw) where |w| = 1. Letting S?~' denote the unit sphere,{w €R? : |w| =1}, the inside integral in the above formula is sometimes written asf(pw)dosp-lwhere o is a measure on S?—'. See “Real and Abstract Analysis” for another descriptionof this measure. It isn’t an important issue here. Either 10.11 or the formula[er (f.. f(pw)ao ) dpwill be referred to as polar coordinates and is very useful in establishing estimates. Hereo (SP!) = f,® (6, 0) dmp-1.SsExample 10.9.3 For what values of s is the integral { B(0,R) (1 + iz!) dy bounded inde-pendent of R? Here B(0,R) is the ball, {a € R? : |x| < R}.I think you can see immediately that s must be negative but exactly how negative? Itturns out it depends on p and using polar coordinates, you can find just exactly what isneeded. From the polar coordinates formula above,Ss R1 ‘Va = [| 1 +p2)° p?-dodroe +a » 0 Joy! +P ) P oe“Rc | (1+p°)’p? dpNow the very hard problem has been reduced to considering an easy one variable prob-lem of finding when fe pr! (1 + p’)'dp is bounded independent of R. You need 2s +(p—1) <—1 so you need s < —p/2.