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S (
d ) , where
S (
d ) denotes the space of tempered
R
R
non-integer s
0 and u
distributions,
2 ) s ˆ
u(ξ )
2
2
H s (
+ |
|
u
d ) :=
( 1
ξ
d ξ.
(16.8)
R
d
R
Similarly, we can define anisotropic Sobolev spaces H s (
d ) with norm
R
· H s
given by
d
ξ j ) s j ˆ
u(ξ )
2
2
H s (
u
d ) :=
( 1
+
d ξ,
(16.9)
R
d
R
j =
1
for any multi-index s
0. The consideration of certain symbol classes will be useful
for the definition of the variable order Sobolev spaces. We set
2 ) 1 / 2
ξ := ( 1
+| ξ |
for notational convenience.
C (
d ) be a real-valued
Definition 16.2.1 Let 0
δ<ρ
1 and let m(x)
R
d
function with bounded derivatives on
R
of arbitrary order. Then, the symbol
ψ(x,ξ) belongs to the class S m(x)
ρ,δ
of symbols of variable order m(x) if ψ(x,ξ)
C (
d
d ) and m(x)
d ) a tempered function, and if,
R
× R
=
+
S
R
s
m(x) with
m
(
d
0
for every α, β
∈ N
there is a constant c α,β such that
d
D x D ξ ψ(x,ξ)
m(x)
ρ
|
α
|+
δ
|
β
| .
x,ξ
∈ R
:
|
|≤
c α,β
ξ
(16.10)
Ψ m(x)
ρ,δ
The variable order pseudodifferential operators
A
(x, D)
correspond to
S m(x)
ρ,δ
symbols ψ(x,ξ)
by
1
2 π
e i x y,ξ ψ(x,ξ)u(y) d y d ξ,
C 0
d ).
(16.11)
A
:=
R
(x, D)u(x)
u
(
d
d
R
R
We are now able to define an isotropic Sobolev space of variable order
H m(x) (
d ) , m(x)
0, using the variable order Riesz potential Λ m(x)
R
with sym-
m(x) . Clearly, ψ(x,ξ) is an element of S m(x)
1
bol ψ(x,ξ) = ξ
for δ ( 0 , 1 ) .The
norm on H m(x) (
d ) is given as
R
2
H m(x) (
Λ 2 m(x) u
2
L 2 ( R
2
L 2 ( R
u
d ) :=
d ) +
u
d ) .
R
1, we obtain the usual L 2 (
d ) -norm. For ψ(x,ξ)
Note that for ψ(x,ξ)
=
R
=
( 1
+
s ) , we obtain the norm given in ( 16.8 ), which follows by applying Plancherel's
theorem. Now we turn to the definition of anisotropic variable order Sobolev spaces.
In analogy to Definition 16.2.1 , we start with the definition of an appropriate symbol
class.
|
ξ
|
d
d
Definition 16.2.2 Let m (x)
=
s
+
m (x) ,
m (x)
: R
→ R
with each component of
d
+
m (x) being a tempered function and s
∈ R
,0
δ<ρ
1. We define the symbol
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