Abstract
In 2006, Hubert, Mauduit and Sárközy extended the notion of binary sequences to n-dimensional binary lattices and introduced the measures of pseudorandomness of binary lattices. In 2011, Gyarmati, Mauduit and Sárközy extended the notions of family complexity, collision and avalanche effect from binary sequences to binary lattices. In this paper, we construct pseudorandom binary lattices by using cyclotomic classes in finite fields and study the pseudorandom measure of order k, family complexity, collision and avalanche effect. Results indicate that such binary lattices are “good,” and their families possess a nice structure in terms of family complexity, collision and avalanche effect.
1 Introduction
The need for pseudorandom binary lattices arises in many applications, so numerous papers have been written on this subject. In these papers, some measures are introduced and studied. For example, Hubert, Mauduit and Sárközy [1] extended the notion of binary sequences to n-dimensional binary lattices and introduced the measures of pseudorandomness of binary lattices. For details, let
A function of the type
Let
where the maximum is taken over all n-dimensional vectors
An n-dimensional binary N-lattice
with probability greater than
In 2011, Gyarmati, Mauduit and Sárközy [2] extended the notions of family complexity, collision and avalanche effect from binary sequences to binary lattices.
Assume that
Obviously, we have the trivial bound
Assume that
Definition 1.1
If
Definition 1.2
If
Definition 1.3
If
If
Clearly,
Many pseudorandom binary lattices have been obtained and studied by using the subsets in finite fields (see [1,2,3,4,5,6,7,8,9,10,11]). Suppose that
where
In this paper, we shall give large families of binary lattices by using the cyclotomic classes in finite fields and study their properties. Our results are the following.
Theorem 1.1
Suppose that
where
Then we have
Theorem 1.2
Suppose that
and
Theorem 1.3
Suppose that
and
Corollary 1.1
Let
then
then
2 Estimates for character sums of polynomials
We need the following lemmas to prove the theorems.
Lemma 2.1
Suppose that
Proof
This is Lemma 4A of [12].□
Lemma 2.2
Suppose that
Proof
This is Theorem 2C′ of [12].□
Lemma 2.3
Suppose that
Then
is not a constant times of a dth power of a polynomial.
Proof
This is Lemma 5 of [11].□
Lemma 2.4
Suppose that
where
Proof
This is Theorem 2 of [13].□
Lemma 2.5
Suppose that
Proof
This is Lemma 1 of [14].□
Lemma 2.6
Suppose that T is a field and
where
Proof
This is Lemma 6 of [15].□
3 Pseudorandom measure of order k
Now we prove Theorem 1.1.
Let
Write
Define
Let
Then
by Lemma 2.5. It follows that
which proves Theorem 1.1.
4 Family complexity
We will adopt the methods used in [15, 16] to prove Theorem 1.2. We shall show that for any specification of length K
where
Note that
Let
and let
where
For
It is well known that
is a representation of the unique interpolating polynomial
Note that
where
It follows that
where
and thus
Then by (3.1) and (4.2) we have
where
and
5 Collision and avalanche effect
Now we study collision and avalanche effect of the family
The last part of the sum in Eq. (5.1) can be written as:
Let
Then
It follows that
and
which proves Theorem 1.3.
References
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© 2020 Xiaolin Chen, published by De Gruyter
This work is licensed under the Creative Commons Attribution 4.0 International License.
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