Open Access Paper
15 January 2025 The design of spectrally-constrained sequences with periodic zero-correlation zone
Shicheng Liu, Xiuping Peng, Shide Wang
Author Affiliations +
Proceedings Volume 13513, The International Conference Optoelectronic Information and Optical Engineering (OIOE2024); 135132O (2025) https://doi.org/10.1117/12.3045744
Event: The International Conference Optoelectronic Information and Optical Engineering (OIOE2024), 2024, Wuhan, China
Abstract
Spectrally-constrained sequences (SCSs) are primarily used in emerging systems operating over non-contiguous spectrum such as cognitive radio and cognitive radar. In order to obtain more SCSs, firstly, a novel type of SCS called periodic zero correlation zone spectrally-constrained sequence(PZCZ-SCS) is proposed in this paper. Then, based on time-frequency synthesis analysis, the conditions that the PZCZ-SCSs must satisfy in terms of “spectral constraint” are derived. Specifically, it is a divisible difference set with parameters λ1 = k and λ1 > λ2. Finally, the construction of PZCZ-SCSs is presented by using the Chinese remainder theorem. Through this research, a new class of SCS is provided for cognitive radio.

1.

INTRODUCTION

The design of sequences with good correlation properties has remained a classical research subject [1]. The traditional design of sequence assumes that the entire frequency band is available and divide it uniformly into multiple frequency segments assigned to different applications. However, with the rise of the number of wireless devices and their related applications, leading to explosive growth in mobile data traffic. An increasingly prominent contradiction has resulted between the enormous demand for wireless spectrum resources and the limited availability of spectrum resources. Cognitive radio [2-3] (cognitive radar [4]) can effectively improve spectrum utilization by dynamically allocating spectrum resources and utilizing idle spectrum resources.The direct application of traditional sequences to cognitive radio systems would lead to significant degradation of their correlation properties [5]. Therefore, researching for designing sequences under spectral constraints is of significant theoretical importance. When designing SCSs, the specific performance demands of sequence design can be summarized as follows [5]: (1) good correlation performance, (2) flexibility in spectrum holes, and (3) low peak-to-average power ratio (PAPR), ideally equal to 1.

The correlation properties are the key focus in the design of SCSs. One aspect involves considering the low correlation properties of SCSs. He et al. [6] proposed a SCAN numerical optimization algorithm to construct SCSs with low sidelobe values in correlation function. Aubry et al. [7] addressed the non-convex quadratic optimization problem in SCS design. Building upon this work, the design methods of single-channel and multi-channel sequence under spectral constraints were proposed by Song et al. [8, 9]. However, designing long-period SCS and large sets of SCSs using numerical optimization algorithms incurs high computational complexity. Hence, the theoretical analytical methods for SCS design has attracted significant attention from experts both domestically and internationally. In [5], single-carrier binary sequences under dynamic spectral hole constraints were constructed based on the time-domain Kronecker product. Based on cyclic difference set and the principles of maximum-length linear shift register sequences, a design method for spectrally-constrained single binary sequences that meet the theoretical bounds was proposed in [10]. In [11], new spectrally-constrained complementary sequence sets with low PAPR values were generated by using orthogonal complementary sets as seed sequences. In [12], a family of spectrally-constrained single-channel sequences was constructed using theoretical analytical methods. On the other hand, sequences with ZCZ can be used as pilot sequences in multiple-input multiple-output (MIMO) channel estimation [13]. Considering the spectrum constraints, Popovi et al. [14] proposed a transform domain method for generating sets of single-channel SNC-ZCZ sequences. SNC-ZCZ sequences and SNC-Z complementary sequences were constructed in [15], filling the gap in spectrum-constrained Z-complementary sequences. In [16], a framework was introduced based on cyclic Florentine rectangles and interleaving techniques to construct sets of ZCZ-SCS sequences. The new theoretical bounds for evaluating ZCZ-SCS sequence sets were proposed, providing new design insights for ZCZ-SCS sequence research.

The research on SCSs is very limited and relatively challenging, and the space for the existence of SCSs is also relatively small. Motivated by this, in this paper, a new class of SCS called PZCZ-SCSs is proposed, and the properties of PZCZ-SCSs are analyzed and studied. Then, a construction for PZCZ_SCSs is proposed from the perspective of the transform domain. To the best of our knowledge, there is currently no relevant research defining PZCZ-SCS. The proposed PZCZ-SCSs can also be used as spreading sequences in communication systems[16]. This research provides a theoretical foundation for the design of PZCZ-SCSs and PZCZ-SCS sets in the future.

2.

PRELIMINARIES

2.1

Theory of Difference Set.

Definition 1[10]: Let C = {c1, c2,···, cn–1} be subset of ZN ={0,1, ···, N – 1}, and the difference function of C is denoted by dC (τ) =| C ∩ (C + τ)|, where τZN and C + τ = {c + τ | cC}. C is called an (N, n, σ) “cyclic difference set” if dC (τ) takes on the value σ for N – 1 times when τ ranges over the nonzero elements of ZN.

Definition 2 [18]: Let G be an mq = N -order multiplicative group, and Q be a q -order subset of G. The k -order subset D of G is called divisible difference set (DDS) with parameter (m, q, k,λ1, λ2) relative to Q if {(di·– dj) mod N,0 ≤ ijk – 1 diD, djD} contains exactly λ1 copies of each nonidentity element of Q and exactly λ2 copies of each element of the set GQ. If λ1 = 0, then D is called a relative difference set in G relative to Q.

Lemma 1 [18]: A subset D of mq = N -order multiplicative group G is an (m, q, k, λ1, λ2) DDS. Furthermore, G\D is also an (m, q, mqk, mqλ1, λ2) DDS.

Lemma 2 [18]: An (m, q, k, λ1, λ2) DDS D relative to Q = {0, m, 2m,···, (q – 1)m} is the subset of mq = N -order multiplicative group G. For τ ∈ {1,···, N – 1}, we have

00096_PSISDG13513_135132O_page_2_1.jpg

2.2

Basic Knowledge.

00096_PSISDG13513_135132O_page_2_2.jpg is a (scaled) discrete Fourier transform (DFT) matrix of order N. The conjugate transpose of FN is 00096_PSISDG13513_135132O_page_2_3.jpg represented the inverse DFT. fi,j is defined by

00096_PSISDG13513_135132O_page_2_4.jpg

where 00096_PSISDG13513_135132O_page_2_5.jpg. The frequency domain dual of the sequence b = [b0, b1,⋯bi,⋯bN–1]T is calculated as B = bFN = [B0, B1,⋯,Bd,⋯BN–1]T.

Definition 3[17]: For any two length- N sequences a and b, the periodic cross-correlation function is defined as

00096_PSISDG13513_135132O_page_3_1.jpg

where b* denotes the complex conjugation of b. if a = b, it is called periodic auto-correlation function which is denoted by θb (τ). If θb (τ ≠ 0) = 0, b is referred to as optimal sequence.

Definition 4[17]: The PAPR value of length- N sequence b is calculated as

00096_PSISDG13513_135132O_page_3_2.jpg

where |bi| is the modulus of the i -th element of b. If |b0| = |b1| = ⋯ = |bN–1|, b is referred to as constant modulus sequence with PAPR=1.

According to time-frequency duality, the relationship between the optimal sequence and the constant modulus sequence as follows.

Lemma 3 [20]: A sequence is optimal in the frequency domain, then it is a constant-modulus sequence in the time domain.

For a CR system whose entire frequency band is uniformly divided into N carriers, let M = [m0, m1, ⋯, mN-1 ] denote “carrier marking vector”, which is capable of implying the dynamic state of N carriers. More specifically, mt = 1 if the i -th carrier is not occupied, furthermore, mi = 0. Ω = {i|mi = 0} represents the set of all occupied carrier. Note that Ω is called the “spectral constraint,” and 00096_PSISDG13513_135132O_page_3_3.jpg.

Definition 5[17]: For any sequence b, denote by B its frequency-domain dual. b is said to be a SCS if Bd = 0 for d ∈ Ω.

Definition 6[17]: b is an ideal SCS if both of the following conditions are met: 1) b is a constant-modulus sequence; 2) the spectral constraint Ω of b is a cyclic difference set with parameter (N, n, σ).

Definition 7 : The length-N SCS b is a PZCZ-SCS if the periodic auto-correlation function satisfies

00096_PSISDG13513_135132O_page_3_4.jpg

where K is an integer and γ is a constant.

3.

ANALYSIS ON THE PROPERTY OF PZCZ-SCS

Based on the time-frequency synthesis analysis, this section will discuss the property that the spectral constraint of PZCZ-SCSs.

Without loss of generality, for a sequence b, we have 00096_PSISDG13513_135132O_page_3_5.jpg, as is widely known from the Parseval’ s theorem that 00096_PSISDG13513_135132O_page_3_6.jpg for the frquency-domain dual B. Let B has a uniformly distributed energy, i.e., 00096_PSISDG13513_135132O_page_3_7.jpg. Recalling equation (7) in[17], the magnitude of periodic auto-correlation function of b can be further expressed as

00096_PSISDG13513_135132O_page_4_1.jpg

where 00096_PSISDG13513_135132O_page_4_2.jpg

Recalling Definition 7, for PZCZ-SCSs, the following identity needs to be satisfied.

00096_PSISDG13513_135132O_page_4_3.jpg

Combining Lemma 2, b is a PZCZ-SCS if and only if 00096_PSISDG13513_135132O_page_4_4.jpg of b is an (m, q, k, λ1, λ2) DDS relative to Q = {0, m, 2m,···, (q – 1)m}, λ1 = k and λ2 < λ1. the magnitude of periodic auto-correlation function of b is calculated as

00096_PSISDG13513_135132O_page_4_5.jpg

Taking into account the practical implications of nonlinear effects, the design of spectrum-limited sequences with an ideal PAPR value holds significant practical value. We have Q = {0, m, 2m,···, (q – 1)m}, λ1 = k and λ2 < λ1.

Definition 8 : b is an ideal PZCZ-SCS if both of the following conditions are met: 1) b is a constant-modulus sequence; 2) the spectral constraint Ω of b is an (m, q, k, λ1, λ2) DDS relative to Q = {0, m, 2m,···, (q – 1)m}, λ1 = k and λ2 < λ1

4.

THE CONSTRUCTION OF PZCZ-SCS

In order to obtain ideal PZCZ-SCS, a construction of PZCZ-SCS will be proposed from the transform domain in this section. The specific construction is as follows.

Construction 1 : Step 1, generate the Matrix M of order q × m based on sequences xt1 = [x0, xl,⋯, xm–l] and yt2 = [y0, yl,⋯, yq–l] where gcd(m, q) = 1.

00096_PSISDG13513_135132O_page_4_6.jpg

where 0 ≤ jq – 1 and 0 ≤ im – 1. The row vector and column vector of M are denoted as sj(t1) = yjxt1 and ri(t2) = xiyt2, respectively, where 0 ≤ t1m – 1 and 0 ≤ t2q – 1.

Step 2, the elements of length-N frequency domain sequence B = [B0, B1,⋯, Bd,⋯, Bmq–1] is defined as follows.

00096_PSISDG13513_135132O_page_4_7.jpg

where

00096_PSISDG13513_135132O_page_5_1.jpg

Step 3, performing the inverse discrete Fourier transform (IDFT) on B yields the time-domain sequence b = [b0, b1,⋯, bi,⋯, bmq–1].we have

00096_PSISDG13513_135132O_page_5_2.jpg

where i = d

Theorem 1: b is an ideal PZCZ-SCS if and only if xt1 = [x0, xl,⋯, xm–l] is an ideal SCS with the spectral constraint C is an (N, n, σ) cyclic difference set and yt2 = [y0, yl,⋯, yq–l] is an optimal constant-modulus sequence. In addition, the spectral constraint of ideal PZCZ-SCS b is expressed as 00096_PSISDG13513_135132O_page_5_2a.jpg.

Proof : The properties of b are analyzed as follows.

Analyzing the magnitude homogeneity of b. Let t = (t1, t2), τ = (τ1, τ2), and note that τ = (τ1, τ2), (t1, t2) ∈ Zm × Zq, the following cases are to be considered.

Case 1: when τ1 = 0, τ2 = 0, the auto-correlation function of B can be obtained by summing the zero-shifted auto-correlation function of sj(t1) = yjxt1. The specific process is as follows.

00096_PSISDG13513_135132O_page_5_3.jpg

Case 2: when τ1 ≠ 0, τ2=0, the auto-correlation function of B can be obtained by summing the non-zero-shifted auto-correlation function of sj(t1) = yjxt1. We have

00096_PSISDG13513_135132O_page_5_4.jpg

since xt1 = [x0, xl,⋯, xm–l] is an ideal SCS, 00096_PSISDG13513_135132O_page_5_4a.jpg. Therefore, θB (τ1, 0) = 0.

Case 3: when τ1 ≠ 0, τ2=0, the auto-correlation function of B can be obtained by summing the non-zero-shifted cross-correlation function of ri(t2) = xiyt2. We have

00096_PSISDG13513_135132O_page_5_5.jpg

since yt1 = [y0, yl,⋯, yq–l] is an optimal constant-modulus sequence, we have θyt2 (τ2) = 0. Therefore, θβ (0, τ2) = 0.

Case 4: when τ1 ≠ 0, τ2 ≠ 0, the auto-correlation function of B can be obtained by summing the non-zero-shifted cross-correlation function of sj(t1) = yjxt1 or ri(t2) = xiyt2. We have

00096_PSISDG13513_135132O_page_6_1.jpg

since 00096_PSISDG13513_135132O_page_6_1a.jpg. Therefore, θB (τ1, τ2) = 0.

As summarized above, B is an optimal sequence, and b is a constant-modulus sequence.

Analyzing the spectral constraint of b. According to the mapping relationship from Zmq to Zm × Zq, the spectral constraint of b is 00096_PSISDG13513_135132O_page_6_1b.jpg. The difference function of Ω is

00096_PSISDG13513_135132O_page_6_2.jpg

The following four cases are to be considered.

Case 1 : when τ1 = 0, τ2 = 0, (17) can be calculated as

00096_PSISDG13513_135132O_page_6_3.jpg

Case 2: when τ1 = 0, τ2 ≠ 0, (17) can be recalculated as

00096_PSISDG13513_135132O_page_6_4.jpg

Case 3: when τ1 ≠ 0, τ2 = 0, (17) can be written as

00096_PSISDG13513_135132O_page_6_5.jpg

since C is an (N, n, σ) cyclic difference set, (20) can be calculated as follows.

00096_PSISDG13513_135132O_page_6_6.jpg

Case 4: when τ1 ≠ 0, τ2 ≠ 0, (17) can be written as

00096_PSISDG13513_135132O_page_6_7.jpg

the reasoning is similar to that of Case 3. (22) can be calculated as follows.

00096_PSISDG13513_135132O_page_6_8.jpg

In conclusion, we have

00096_PSISDG13513_135132O_page_6_9.jpg

the spectral constraint Ω of b isan (m, q, nq, nq, σq) DDS relative to Q = {0, m, 2m,···, (q – 1)m}.

Combining the above two situations, it can be conclude that b is an ideal PZCZ-SCS.

Example 2 : Let xt1 = [–1,0,0,1,0,1,1] and yt1 = [–1, –1, –1] where the spectral constraint of xt1 is as (7,3,1) cyclic difference set. According to Construction 1, M is written ast. (7,3,1)

00096_PSISDG13513_135132O_page_7_1.jpg

Then we obtain sequence B = [–1,0,0,–1,0,–1,–1,1,0,0,–1,0,1,–1,1,0,0,–1,0,–1,1,10,0,1,0,– 1,– 1] with the spectral constraint Ω = {1,2,4,8,9,11,15,16,18,22,23,25}. By calculating (12), we obtain the time domain sequence b. The correlation property of B and b is illustrated in Figure 1.

Figure. 1

Auto-correlation function of sequence.

00096_PSISDG13513_135132O_page_7_2.jpg

Clearly, B is optimal and the time domain dual is constant magnitude. The auto-correlation function value of b is 00096_PSISDG13513_135132O_page_7_3.jpg. In summary, b is an ideal PZCZ-SCS.

5.

SUMMARY

SCSs with good correlation properties have significant application value in CR-MIMO systems [16]. In order to expand the existing space of SCSs, the concept of PZCZ-SCS is introduced in this paper. Furthermore, based on the time-frequency synthesis analysis, the condition for spectral constraint of PZCZ-SCS is derived. Considering the practical applications, we present the definition of ideal PZCZ-SCS. Finally, the construction of ideal PZCZ-SCS is proposed based on matrix operation. The study in this paper provides a new research idea for the study of SCSs, and lays a theoretical foundation for the subsequent study of PZCZ-SCSs and PZCZ-SCS sets with periodic zero correlation zone.

6.

ACKNOWLEDGEMENT

This work was supported by China Natural Science Foundation (61601401, 62241110), by Natural Science Foundation of Hebei Province, China (F2021203040), by Science and Technology Program of Universities and Colleges in Hebei Province (ZD2019039) and Central government guides local science and technology development Foundation under Grant (236Z0403G).

7.

7.

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(2025) Published by SPIE. Downloading of the abstract is permitted for personal use only.
Shicheng Liu, Xiuping Peng, and Shide Wang "The design of spectrally-constrained sequences with periodic zero-correlation zone", Proc. SPIE 13513, The International Conference Optoelectronic Information and Optical Engineering (OIOE2024), 135132O (15 January 2025); https://doi.org/10.1117/12.3045744
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KEYWORDS
Autocorrelation

Design

Time-frequency analysis

Analytical research

Bismuth

Matrices

Mathematical optimization

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