243 research outputs found

    Construction of pp-ary Sequence Families of Period (pnโˆ’1)/2(p^n-1)/2 and Cross-Correlation of pp-ary m-Sequences and Their Decimated Sequences

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    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ์ „๊ธฐยท์ปดํ“จํ„ฐ๊ณตํ•™๋ถ€, 2015. 2. ๋…ธ์ข…์„ .This dissertation includes three main contributions: a construction of a new family of pp-ary sequences of period pnโˆ’12\frac{p^n-1}{2} with low correlation, a derivation of the cross-correlation values of decimated pp-ary m-sequences and their decimations, and an upper bound on the cross-correlation values of ternary m-sequences and their decimations. First, for an odd prime p=3modโ€‰โ€‰4p = 3 \mod 4 and an odd integer nn, a new family of pp-ary sequences of period N=pnโˆ’12N = \frac{p^n-1}{2} with low correlation is proposed. The family is constructed by shifts and additions of two decimated m-sequences with the decimation factors 2 and d=Nโˆ’pnโˆ’1d = N-p^{n-1}. The upper bound on the maximum value of the magnitude of the correlation of the family is shown to be 2N+1/2=2pn2\sqrt{N+1/2} = \sqrt{2p^n} by using the generalized Kloosterman sums. The family size is four times the period of sequences, 2(pnโˆ’1)2(p^n-1). Second, based on the work by Helleseth \cite{Helleseth1}, the cross-correlation values between two decimated m-sequences by 2 and 4pn/2โˆ’24p^{n/2}-2 are derived, where pp is an odd prime and n=2mn = 2m is an integer. The cross-correlation is at most 4-valued and their values are {โˆ’1ยฑpn/22,โˆ’1+3pn/22,โˆ’1+5pn/22}\{\frac{-1\pm p^{n/2}}{2}, \frac{-1+3p^{n/2}}{2}, \frac{-1+5p^{n/2}}{2}\}. As a result, for pmโ‰ 2modโ€‰โ€‰3p^m \neq 2 \mod 3, a new sequence family with the maximum correlation value 52N\frac{5}{\sqrt{2}} \sqrt{N} and the family size 4N4N is obtained, where N=pnโˆ’12N = \frac{p^n-1}{2} is the period of sequences in the family. Lastly, the upper bound on the cross-correlation values of ternary m-sequences and their decimations by d=34k+2โˆ’32k+1+24+32k+1d = \frac{3^{4k+2}-3^{2k+1}+2}{4}+3^{2k+1} is investigated, where kk is an integer and the period of m-sequences is N=34k+2โˆ’1N = 3^{4k+2}-1. The magnitude of the cross-correlation is upper bounded by 12โ‹…32k+3+1=4.5N+1+1\frac{1}{2} \cdot 3^{2k+3}+1 = 4.5 \sqrt{N+1}+1. To show this, the quadratic form technique and Bluher's results \cite{Bluher} are employed. While many previous results using quadratic form technique consider two quadratic forms, four quadratic forms are involved in this case. It is proved that quadratic forms have only even ranks and at most one of four quadratic forms has the lowest rank 4kโˆ’24k-2.Abstract i Contents iii List of Tables vi List of Figures vii 1. Introduction 1 1.1. Background 1 1.2. Overview of Dissertation 9 2. Sequences with Low Correlation 11 2.1. Trace Functions and Sequences 11 2.2. Sequences with Low Autocorrelation 13 2.3. Sequence Families with Low Correlation 17 3. A New Family of p-ary Sequences of Period (p^nโˆ’1)/2 with Low Correlation 21 3.1. Introduction 22 3.2. Characters 24 3.3. Gaussian Sums and Kloosterman Sums 26 3.4. Notations 28 3.5. Definition of Sequence Family 29 3.6. Correlation Bound 30 3.7. Size of Sequence Family 35 3.8. An Example 38 3.9. Related Work 40 3.10. Conclusion 41 4. On the Cross-Correlation between Two Decimated p-ary m-Sequences by 2 and 4p^{n/2}โˆ’2 44 4.1. Introduction 44 4.2. Decimated Sequences of Period (p^nโˆ’1)/2 49 4.3. Correlation Bound 53 4.4. Examples 59 4.5. A New Sequence Family of Period (p^nโˆ’1)/2 60 4.6. Discussions 61 4.7. Conclusion 67 5. On the Cross-Correlation of Ternary m-Sequences of Period 3^{4k+2} โˆ’ 1 with Decimation (3^{4k+2}โˆ’3^{2k+1}+2)/4 + 3^{2k+1} 69 5.1. Introduction 69 5.2. Quadratic Forms and Linearized Polynomials 71 5.3. Number of Solutions of x^{p^s+1} โˆ’ cx + c 78 5.4. Notations 79 5.5. Quadratic Form Expression of the Cross-Correlation Function 80 5.6. Ranks of Quadratic Forms 83 5.7. Upper Bound on the Cross-Correlation Function 89 5.8. Examples 93 5.9. Related Works 94 5.10. Conclusion 94 6. Conclusions 96 Bibliography 98 ์ดˆ๋ก 109Docto

    On the List-Decodability of Random Linear Codes

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    For every fixed finite field \F_q, pโˆˆ(0,1โˆ’1/q)p \in (0,1-1/q) and ฯต>0\epsilon > 0, we prove that with high probability a random subspace CC of \F_q^n of dimension (1โˆ’Hq(p)โˆ’ฯต)n(1-H_q(p)-\epsilon)n has the property that every Hamming ball of radius pnpn has at most O(1/ฯต)O(1/\epsilon) codewords. This answers a basic open question concerning the list-decodability of linear codes, showing that a list size of O(1/ฯต)O(1/\epsilon) suffices to have rate within ฯต\epsilon of the "capacity" 1โˆ’Hq(p)1-H_q(p). Our result matches up to constant factors the list-size achieved by general random codes, and gives an exponential improvement over the best previously known list-size bound of qO(1/ฯต)q^{O(1/\epsilon)}. The main technical ingredient in our proof is a strong upper bound on the probability that โ„“\ell random vectors chosen from a Hamming ball centered at the origin have too many (more than ฮ˜(โ„“)\Theta(\ell)) vectors from their linear span also belong to the ball.Comment: 15 page

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    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ์ „๊ธฐยท์ปดํ“จํ„ฐ๊ณตํ•™๋ถ€, 2017. 2. ๋…ธ์ข…์„ .In this dissertation, the cross-correlation between two differently decimated sequences of a pp-ary m-sequence is considered. Two main contributions are as follows. First, for an odd prime pp, n=2mn=2m, and a pp-ary m-sequence of period pnโˆ’1p^n -1, the cross-correlation between two decimated sequences by 22 and dd are investigated. Two cases of dd, d=(pm+1)22d=\frac{(p^m +1)^2}{2} with pmโ‰ก1(mod4)p^m \equiv 1 \pmod4 and d=(pm+1)2pe+1d=\frac{(p^m +1)^2}{p^e +1} with odd m/em/e are considered. The value distribution of the cross-correlation function for each case is completely deterimined. Also, by using these decimated sequences, two new families of pp-ary sequences of period pnโˆ’12\frac{p^n -1}{2} with good correlation property are constructed. Second, an upper bound on the magnitude of the cross-correlation function between two decimated sequences of a pp-ary m-sequence is derived. The two decimation factors are 22 and 2(pm+1)2(p^m +1), where pp is an odd prime, n=2mn=2m, and pmโ‰ก1(mod4)p^m \equiv 1 \pmod4. In fact, these two sequences corresponds to the sequences used for the construction of pp-ary Kasami sequences decimated by 22. The upper bound is given as 32pm+12\frac{3}{2}p^m + \frac{1}{2}. Also, using this result, an upper bound of the cross-correlation magnitude between a pp-ary m-sequence and its decimated sequence with the decimation factor d=(pm+1)22d=\frac{(p^m +1)^2}{2} is derived.1 Introduction 1 1.1 Background 1 1.2 Overview of This Dissertation 7 2 Preliminaries 9 2.1 Finite Fields 9 2.2 Trace Functions and Sequences 11 2.3 Cross-Correlation Between Two Sequences 13 2.4 Characters and Weils Bound 15 2.5 Trace-Orthogonal Basis 16 2.6 Known Exponential Sums 17 2.7 Cross-Correlation of pp-ary Kasami Sequence Family 18 2.8 Previous Results on the Cross-Correlation for Decimations with gcdโก(pnโˆ’1,d)=pn/2+12\gcd(p^n -1, d)=\frac{p^{n/2}+1}{2} 20 2.9 Cross-Correlation Between Two Decimated Sequences by 22 and d=4d=4 or pn+12\frac{p^n +1}{2} 23 3 New pp-ary Sequence Families of Period pnโˆ’12\frac{p^n -1}{2} with Good Correlation Property Using Two Decimated Sequences 26 3.1 Cross-Correlation for the Case of d=(pm+1)22d=\frac{(p^m +1)^2}{2} 27 3.2 Cross-Correlation for the Case of d=(pm+1)2pe+1d=\frac{(p^m +1)^2}{p^e +1} 37 3.3 Construction of New Sequence Families 43 4 Upper Bound on the Cross-Correlation Between Two Decimated pp-ary Sequences 52 4.1 Cross-Correlation Between s(2t+i)s(2t+i) and s(2(pm+1)t+j)s(2(p^m +1)t +j) 53 4.2 Cross-Correlation Between s(t)s(t) and s((pm+1)22t)s(\frac{(p^m +1)^2}{2} t) 66 5 Conclusions 69 Bibliography 72 Abstract (In Korean) 80Docto

    Secondary constructions of vectorial pp-ary weakly regular bent functions

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    In \cite{Bapic, Tang, Zheng} a new method for the secondary construction of vectorial/Boolean bent functions via the so-called (PU)(P_U) property was introduced. In 2018, Qi et al. generalized the methods in \cite{Tang} for the construction of pp-ary weakly regular bent functions. The objective of this paper is to further generalize these constructions, following the ideas in \cite{Bapic, Zheng}, for secondary constructions of vectorial pp-ary weakly regular bent and plateaued functions. We also present some infinite families of such functions via the pp-ary Maiorana-McFarland class. Additionally, we give another characterization of the (PU)(P_U) property for the pp-ary case via second-order derivatives, as it was done for the Boolean case in \cite{Zheng}

    Replacing the Soft FEC Limit Paradigm in the Design of Optical Communication Systems

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    The FEC limit paradigm is the prevalent practice for designing optical communication systems to attain a certain bit-error rate (BER) without forward error correction (FEC). This practice assumes that there is an FEC code that will reduce the BER after decoding to the desired level. In this paper, we challenge this practice and show that the concept of a channel-independent FEC limit is invalid for soft-decision bit-wise decoding. It is shown that for low code rates and high order modulation formats, the use of the soft FEC limit paradigm can underestimate the spectral efficiencies by up to 20%. A better predictor for the BER after decoding is the generalized mutual information, which is shown to give consistent post-FEC BER predictions across different channel conditions and modulation formats. Extensive optical full-field simulations and experiments are carried out in both the linear and nonlinear transmission regimes to confirm the theoretical analysis

    Applications of finite geometries to designs and codes

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    This dissertation concerns the intersection of three areas of discrete mathematics: finite geometries, design theory, and coding theory. The central theme is the power of finite geometry designs, which are constructed from the points and t-dimensional subspaces of a projective or affine geometry. We use these designs to construct and analyze combinatorial objects which inherit their best properties from these geometric structures. A central question in the study of finite geometry designs is Hamadaโ€™s conjecture, which proposes that finite geometry designs are the unique designs with minimum p-rank among all designs with the same parameters. In this dissertation, we will examine several questions related to Hamadaโ€™s conjecture, including the existence of counterexamples. We will also study the applicability of certain decoding methods to known counterexamples. We begin by constructing an infinite family of counterexamples to Hamadaโ€™s conjecture. These designs are the first infinite class of counterexamples for the affine case of Hamadaโ€™s conjecture. We further demonstrate how these designs, along with the projective polarity designs of Jungnickel and Tonchev, admit majority-logic decoding schemes. The codes obtained from these polarity designs attain error-correcting performance which is, in certain cases, equal to that of the finite geometry designs from which they are derived. This further demonstrates the highly geometric structure maintained by these designs. Finite geometries also help us construct several types of quantum error-correcting codes. We use relatives of finite geometry designs to construct infinite families of q-ary quantum stabilizer codes. We also construct entanglement-assisted quantum error-correcting codes (EAQECCs) which admit a particularly efficient and effective error-correcting scheme, while also providing the first general method for constructing these quantum codes with known parameters and desirable properties. Finite geometry designs are used to give exceptional examples of these codes

    Two-tuple balance of non-binary sequences with ideal two-level autocorrelation

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    AbstractLet p be a prime, q=pm and Fq be the finite field with q elements. In this paper, we will consider q-ary sequences of period qn-1 for q>2 and study their various balance properties: symbol-balance, difference-balance, and two-tuple-balance properties. The array structure of the sequences is introduced, and various implications between these balance properties and the array structure are proved. Specifically, we prove that if a q-ary sequence of period qn-1 is difference-balanced and has the โ€œcyclicโ€ array structure then it is two-tuple-balanced. We conjecture that a difference-balanced q-ary sequence of period qn-1 must have the cyclic array structure. The conjecture is confirmed with respect to all of the known q-ary sequences which are difference-balanced, in particular, which have the ideal two-level autocorrelation function when q=p

    Quantum error control codes

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    It is conjectured that quantum computers are able to solve certain problems more quickly than any deterministic or probabilistic computer. For instance, Shor's algorithm is able to factor large integers in polynomial time on a quantum computer. A quantum computer exploits the rules of quantum mechanics to speed up computations. However, it is a formidable task to build a quantum computer, since the quantum mechanical systems storing the information unavoidably interact with their environment. Therefore, one has to mitigate the resulting noise and decoherence effects to avoid computational errors. In this dissertation, I study various aspects of quantum error control codes - the key component of fault-tolerant quantum information processing. I present the fundamental theory and necessary background of quantum codes and construct many families of quantum block and convolutional codes over finite fields, in addition to families of subsystem codes. This dissertation is organized into three parts: Quantum Block Codes. After introducing the theory of quantum block codes, I establish conditions when BCH codes are self-orthogonal (or dual-containing) with respect to Euclidean and Hermitian inner products. In particular, I derive two families of nonbinary quantum BCH codes using the stabilizer formalism. I study duadic codes and establish the existence of families of degenerate quantum codes, as well as families of quantum codes derived from projective geometries. Subsystem Codes. Subsystem codes form a new class of quantum codes in which the underlying classical codes do not need to be self-orthogonal. I give an introduction to subsystem codes and present several methods for subsystem code constructions. I derive families of subsystem codes from classical BCH and RS codes and establish a family of optimal MDS subsystem codes. I establish propagation rules of subsystem codes and construct tables of upper and lower bounds on subsystem code parameters. Quantum Convolutional Codes. Quantum convolutional codes are particularly well-suited for communication applications. I develop the theory of quantum convolutional codes and give families of quantum convolutional codes based on RS codes. Furthermore, I establish a bound on the code parameters of quantum convolutional codes - the generalized Singleton bound. I develop a general framework for deriving convolutional codes from block codes and use it to derive families of non-catastrophic quantum convolutional codes from BCH codes. The dissertation concludes with a discussion of some open problems
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