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α
(
, n ) or greater, the following inequality holds true:
Theorem 5. With probability 1
η
n
n
1 B ln N
ln
η
C
V
1
2 I
B
+ n + n
n
ln
η
. (41)
1
2 I
Theorem 6. With probability 1
α
(
η
, n ) or greater, the following inequality holds true:
2 n
n
1 + 1 B ln N
+ B n
ln
η
ln
η
V
C
.
(42)
2 I
2 I
3
The Relationship for an Infinite Set of Approximating Functions
The simplest case with a finite number of functions in the set has been generalized
by Vapnik [2,19,25] onto infinite sets with continuum of elements by introducing sev-
eral notions of the capacity of the set of functions: entropy , annealed entropy , growth
function , Vapnik-Chervonenkis dimension . We remind them in brief.
First of all, Vapnik defines N Ω ( z 1 ,..., z I ) which is the number of all possible di-
chotmies that can be achieved on a fixed sample
{
z 1 ,..., z I
}
using functions from
{
} ω Ω . Then, if we relax the sample the following notions of capacity can be
considered:
Q ( z ,
ω
)
1. expected value of ln N Ω Vapnik-Chervonenkis entropy :
H Ω ( I )=
ln N Ω ( z 1 ,..., z I )
z 1 Z ···
z I Z
·
p ( z 1 )
···
p ( z I ) dz 1 ···
dz I ,
2. ln of expected value of N Ω annealed entropy :
H ann ( I )= ln
N Ω ( z 1 ,..., z I )
z 1 Z ···
z I Z
·
p ( z 1 )
···
p ( z I ) dz 1 ···
dz I ,
3. ln of supremum of N Ω growth function
G Ω ( I )= ln sup
z 1 ,..., z I
N Ω ( z 1 ,..., z I ) .
It has been proved that:
G Ω ( I )= = ln 2 I ,
dla I
h ;
k = 0 k , dla I > h ,
(43)
h
ln
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