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By Lemma 1,
f ( β ))
η
1
p n
ψ ( f ( ξ + ξ τ + ω )
f ( ξ )) =
ψ ( f ( β + ξ τ + ω )
ψ ( η ( ξ
β )) .
β
F p n
F p n
We get
ψ ( f ( ξ + ξ τ + ω )
f ( ξ ))
ξ∈P ω
f ( β ))
η∈ F p n
1
p n
=
ψ ( f ( β + ξ τ + ω )
ψ ( η ( ξ
β ))
ξ∈P ω
β∈ F p n
1
p n
ψ ( f ( β + ξ τ + ω )
f ( β )
ηβ )
ψ ( ηξ )
.
η∈ F p n
β∈ F p n
ξ∈P ω
By Lemmas 2 and 5,
1) p n/ 2
/p n
ψ ( f ( ξ + ξ τ + ω )
f ( ξ ))
max
ξ
=0 (deg( g ξ )
ψ ( ηξ )
ξ∈P ω
η∈ F p n
ξ∈P ω
1) p n/ 2 (1 + ln p ) n− 1 .
max
ξ =0 (deg( g ξ )
Similarly, we have
1) p n/ 2 (1 + ln p ) n− 1 .
ψ ( f ( ξ + ξ τ )
f ( ξ ))
max
ξ =0
(deg( g ξ )
ξ∈P ω
Finally, by (2),
2(2 n− 1
1) p n/ 2 (1 + ln p ) n− 1 +max
1) p n/ 2 .
|
C S ( τ )
|≤
ξ =0 (deg( g ξ )
ξ =0 (deg( g ξ )
1) max
Remark 1. The bound in Theorem 2 is applicable only when p is large. The basic
idea in the proof above is from [7]. Note that the approach for establishing The-
orem 3 in [1] is also from [7]. Unfortunately, this technique cannot be extended
to the case of p = 2, because one needs to consider the number of nonzero ω
which is 2 n− 1 .
Theorem 3. For any 0 <τ <p n , we have the following bound for the autocor-
relation of the sequence S =
s i } i =0 defined by (1) with A ( x )= Tr ( x p n 2 )
{
< 4(2 n− 1
p n/ 2 +1)(1+ln p ) n− 1 +2
p n/ 2 +3 .
|
C S ( τ )
|
1)(2
·
·
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