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Function Spaces as Dirichlet Spaces (About a Paper by Maz'ya and ...

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14 N. Jacob <strong>and</strong> R. L. Schilling<br />

with a me<strong>as</strong>ure ν on (0, ∞) such that ∫ 1<br />

0+ s−n/2 ν(ds) + ∫ ∞<br />

1<br />

s −n/2−1 ν(ds) < ∞.<br />

According to Lemma 2.1 we have ψ(ξ) = f(|ξ| 2 ) where f is given <strong>by</strong> (15).<br />

Moreover we know, cf. (16), that<br />

∫<br />

R n |û(ξ)| 2 f(|ξ| 2 ) dξ = 1 2<br />

∫∫<br />

R n ×R n |u(x + y) − u(x)| 2 m(|y| 2 ) dy dx<br />

holds. On the other h<strong>and</strong>, for a completely monotone function g we know from<br />

Lemma 3.3 that<br />

∫<br />

∫∫<br />

( 1<br />

) dx dy<br />

|û(ξ)| 2 µ(|ξ| 2 ) dξ ∼ |u(x + y) − u(x)| 2 g<br />

R n R n ×R |y| n 2 |y| n<br />

in the sense of equivalent (semi-)norms where µ(t) is <strong>as</strong> in Lemma 3.3, i.e.,<br />

µ(t) =<br />

∫ t<br />

0<br />

( ∫ ∞<br />

r<br />

g(s) ds<br />

s 2 )<br />

dr.<br />

Both m(r) <strong>and</strong> r ↦→ r −n/2 g ( 1<br />

r<br />

)<br />

are completely monotone functions. Our first<br />

aim is to compare these two functions. From Lemma 3.4 we know that<br />

( 1<br />

)<br />

r −n/2 g =<br />

r<br />

∫ ∞<br />

0<br />

e −xr h(x) dx<br />

where<br />

h(x) = xn/2<br />

Γ ( )<br />

n<br />

2<br />

∫ ∞<br />

0+<br />

( ∫ 1<br />

e −x/s t n/2 e<br />

0<br />

tx/s dt<br />

) ρ(ds)<br />

.<br />

t s<br />

Lemma 4.1. If µ(1) < ∞, then ∫ 1<br />

0 x−n/2 h(x) dx + ∫ ∞<br />

1<br />

x −n/2−1 h(x) dx < ∞.<br />

Proof. Assume that µ(1) < ∞. Then<br />

∫ 1<br />

0<br />

x −n/2 h(x) dx =<br />

∫ 1<br />

x −n/2 xn/2<br />

0 Γ ( n<br />

2<br />

∫ 1<br />

= 1<br />

Γ ( )<br />

n<br />

2<br />

= 1 )<br />

Γ ( n<br />

2<br />

= 1<br />

Γ ( n<br />

2<br />

)<br />

0<br />

∫ ∞<br />

0+<br />

∫ ∞<br />

0+<br />

( ∫ ∞<br />

[ ∫ 1<br />

]<br />

) e −x/s t n/2 tx/s dt ρ(ds)<br />

e<br />

0+<br />

0 t s<br />

( ∫ ∞<br />

[ ∫ 1<br />

] ) ρ(ds)<br />

e −x(1−t)/s t n/2−1 dt dx<br />

0+ 0<br />

s<br />

( ∫ 1<br />

[ ] x=1 ) −s<br />

ρ(ds)<br />

0 1 − t e−x(1−t)/s t n/2−1 dt<br />

x=0<br />

s<br />

( ∫ 1<br />

)<br />

1<br />

1 − t (1 − e−(1−t)/s ) t n/2−1 dt ρ(ds).<br />

0<br />

)<br />

dx

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