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V ( f )=
f
μ
K ,where
· K is the norm that corresponds to the scalar product
of
H
,and D ( P n )thatsatisfies
D 2 ( P n )
K ( u i , v ) d v +
[0 , 1] 2 s
n− 1
n− 1
n− 1
1
n 2
2
n
=
K ( u i , u j )
K ( u , v ) d u d v (4)
[0 , 1] s
i =0
j =0
i =0
(see [11,12]). When K ( u , v ) can be computed in O ( s ) time for an arbitrary
( u , v ), then this D ( P n ) can be computed in O ( n 2 s ) time, but this assumption
does not always hold.
One important type of kernel has the form
K ( u , v )=
h Z
w ( h ) e 2 πι h t ( u v )
(5)
s
where ι =
1, the t means “transposed”, and the w ( h ) are non-negative
weights such that h Z s w ( h ) <
. The corresponding square variation is
V 2 ( f )=
0
f ( h )
2 /w ( h ) ,
s |
|
=
h Z
where the f ( h ) are the Fourier coecients of f . The corresponding discrepancy
is easily computable only for special shapes of the weights.
For example, if
s
h j | 2 α ) ,
w ( h )=
min(1 j |
(6)
j =1
for some integer α
1 and positive real numbers (weights) γ j , then the kernel
becomes
1
v j ) mod 1) ,
s
4 π 2 ) α
(2 α )!
γ j (
K α ( u , v )=
B 2 α (( u j
(7)
j =1
where B 2 α is the Bernoulli polynomial of degree 2 α [20]. This kernel can be
computed in O ( s ) time, so the discrepancy can be computed in O ( n 2 s )time.
The corresponding V ( f ) in this case satisfies
j∈ u
(4 π 2 ) −α| u |
2
V 2 ( f )=
φ = u ⊆S
α| u | f
u α
u
γ −α
j
( u ) d u u
d u u ,
[0 , 1] | u |
[0 , 1] s−| u |
(8)
where u u represents the coordinates of u whose indices are in the set
u
and u u
represents those whose indices are not in
. This RKHS contains only periodic
functions f of period 1, with f (0) = f (1), and the variability measures the
smoothness via the partial derivatives of f .
u
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