Distinct 8-QAM+ Perfect Arrays Fanxin Zeng 1, a, Zhenyu Zhang 2,1, b, Linjie Qian 1, c

Similar documents
APPLICATIONS OF SEMIGENERALIZED -CLOSED SETS

Generating Functions, Weighted and Non-Weighted Sums for Powers of Second-Order Recurrence Sequences

Groupoid and Topological Quotient Group

Set of square-integrable function 2 L : function space F

COMPLEMENTARY ENERGY METHOD FOR CURVED COMPOSITE BEAMS

Multistage Median Ranked Set Sampling for Estimating the Population Median

GENERALIZATION OF AN IDENTITY INVOLVING THE GENERALIZED FIBONACCI NUMBERS AND ITS APPLICATIONS

If there are k binding constraints at x then re-label these constraints so that they are the first k constraints.

P 365. r r r )...(1 365

Exact Simplification of Support Vector Solutions

ON THE FRESNEL SINE INTEGRAL AND THE CONVOLUTION

8 Baire Category Theorem and Uniform Boundedness

Engineering Mechanics. Force resultants, Torques, Scalar Products, Equivalent Force systems

Correspondence Analysis & Related Methods

UNIT10 PLANE OF REGRESSION

Contact, information, consultations

Energy in Closed Systems

Optimal System for Warm Standby Components in the Presence of Standby Switching Failures, Two Types of Failures and General Repair Time

ONE-POINT CODES USING PLACES OF HIGHER DEGREE

SOME NEW SELF-DUAL [96, 48, 16] CODES WITH AN AUTOMORPHISM OF ORDER 15. KEYWORDS: automorphisms, construction, self-dual codes

Rigid Bodies: Equivalent Systems of Forces

A Study about One-Dimensional Steady State. Heat Transfer in Cylindrical and. Spherical Coordinates

The Forming Theory and the NC Machining for The Rotary Burs with the Spectral Edge Distribution

Numerical approximation to ζ(2n+1)

(8) Gain Stage and Simple Output Stage

A. Thicknesses and Densities

Some Approximate Analytical Steady-State Solutions for Cylindrical Fin

Closed-loop adaptive optics using a CMOS image quality metric sensor

Scalars and Vectors Scalar

A Study of C-Reducible Finsler Space. With Special Cases

Multi-element based on proxy re-encryption scheme for mobile cloud computing

New problems in universal algebraic geometry illustrated by boolean equations

Khintchine-Type Inequalities and Their Applications in Optimization

Thermodynamics of solids 4. Statistical thermodynamics and the 3 rd law. Kwangheon Park Kyung Hee University Department of Nuclear Engineering

The Greatest Deviation Correlation Coefficient and its Geometrical Interpretation

A Brief Guide to Recognizing and Coping With Failures of the Classical Regression Assumptions

Vanishing lines in generalized Adams spectral sequences are generic

A Method of Reliability Target Setting for Electric Power Distribution Systems Using Data Envelopment Analysis

Power Harmonic Analysis Based on Orthogonal Trigonometric Functions Family

Gradient-based Neural Network for Online Solution of Lyapunov Matrix Equation with Li Activation Function

Efficiency of the principal component Liu-type estimator in logistic

A new Approach for Solving Linear Ordinary Differential Equations

Ranks of quotients, remainders and p-adic digits of matrices

The Order Relation and Trace Inequalities for. Hermitian Operators

Experimental study on parameter choices in norm-r support vector regression machines with noisy input

Using T.O.M to Estimate Parameter of distributions that have not Single Exponential Family

A method for solving dynamic problems for cylindrical domains

COLLAPSING WALLS THEOREM

Tian Zheng Department of Statistics Columbia University

VISUALIZATION OF THE ABSTRACT THEORIES IN DSP COURSE BASED ON CDIO CONCEPT

Re-Ranking Retrieval Model Based on Two-Level Similarity Relation Matrices

Links in edge-colored graphs

PO with Modified Surface-normal Vectors for RCS calculation of Scatterers with Edges and Wedges

Physics Exam II Chapters 25-29

FACTORIZATION IN KRULL MONOIDS WITH INFINITE CLASS GROUP

Mean Curvature and Shape Operator of Slant Immersions in a Sasakian Space Form

Chapter 3: Theory of Modular Arithmetic 38

To Feel a Force Chapter 7 Static equilibrium - torque and friction

A Bijective Approach to the Permutational Power of a Priority Queue

THE ISOMORPHISM PROBLEM FOR CAYLEY GRAPHS ON THE GENERALIZED DICYCLIC GROUP

arxiv: v1 [math.co] 12 Sep 2014

An efficient algorithm for multivariate Maclaurin Newton transformation

On Maneuvering Target Tracking with Online Observed Colored Glint Noise Parameter Estimation

A NOVEL DWELLING TIME DESIGN METHOD FOR LOW PROBABILITY OF INTERCEPT IN A COMPLEX RADAR NETWORK

Chapter 23: Electric Potential

Central Coverage Bayes Prediction Intervals for the Generalized Pareto Distribution

Detection and Estimation Theory

VParC: A Compression Scheme for Numeric Data in Column-Oriented Databases

Transport Coefficients For A GaAs Hydro dynamic Model Extracted From Inhomogeneous Monte Carlo Calculations

Test 1 phy What mass of a material with density ρ is required to make a hollow spherical shell having inner radius r i and outer radius r o?

Pearson s Chi-Square Test Modifications for Comparison of Unweighted and Weighted Histograms and Two Weighted Histograms

General viscosity iterative method for a sequence of quasi-nonexpansive mappings

INTERVAL ESTIMATION FOR THE QUANTILE OF A TWO-PARAMETER EXPONENTIAL DISTRIBUTION

Beyond Zudilin s Conjectured q-analog of Schmidt s problem

Uniqueness of Weak Solutions to the 3D Ginzburg- Landau Model for Superconductivity

by numerous studies); ii) MSWT spectrum is symmetric with respect to point while numerical methods give asymmetrical spectrum with gap = = 2.

Matrix Elements of Many-Electron Wavefunctions. noninteger principal quantum number. solutions to Schröd. Eq. outside sphere of radius r

Hamiltonian multivector fields and Poisson forms in multisymplectic field theory

EE 5337 Computational Electromagnetics (CEM)

Perron Vectors of an Irreducible Nonnegative Interval Matrix

FREE TRANSVERSE VIBRATIONS OF NON-UNIFORM BEAMS

On Polynomials Construction

arxiv: v1 [math.co] 1 Apr 2011

DOI: /jos Tel/Fax: by Journal of Software. All rights reserved. , )

On the ratio of maximum and minimum degree in maximal intersecting families

Integral Vector Operations and Related Theorems Applications in Mechanics and E&M

Chapter Fifiteen. Surfaces Revisited

Vibration Input Identification using Dynamic Strain Measurement

COMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD

Power efficiency and optimum load formulas on RF rectifiers featuring flow-angle equations

On a New Definition of a Stochastic-based Accuracy Concept of Data Reconciliation-Based Estimators

Asymptotic Waves for a Non Linear System

V. Principles of Irreversible Thermodynamics. s = S - S 0 (7.3) s = = - g i, k. "Flux": = da i. "Force": = -Â g a ik k = X i. Â J i X i (7.

The Chromatic Villainy of Complete Multipartite Graphs

SOME SOLVABILITY THEOREMS FOR NONLINEAR EQUATIONS

New Condition of Stabilization of Uncertain Continuous Takagi-Sugeno Fuzzy System based on Fuzzy Lyapunov Function

An Approach to Inverse Fuzzy Arithmetic

Method for Approximating Irrational Numbers

k. s k=1 Part of the significance of the Riemann zeta-function stems from Theorem 9.2. If s > 1 then 1 p s

Christian Aebi Collège Calvin, Geneva, Switzerland

Transcription:

nd Intenatonal Confeence on Electcal Compute Engneeng and Electoncs (ICECEE 15) Dstnct 8-QAM+ Pefect Aays Fanxn Zeng 1 a Zhenyu Zhang 1 b Lnje Qan 1 c 1 Chongqng Key Laboatoy of Emegency Communcaton Chongqng Communcaton Insttute Chongqng 435 Chna College of Communcaton Engneeng Chongqng Unvesty Chongqng 444 Chna emal: a fzengx@163.com b zhenyu.zhang@cqu.edu.cn c chalge@16.com Keywods: pefect aays 8-QAM+ constellaton famly sze Abstact. Ths pape nvestgates the constucton of 8-QAM+ pefect aays wth at least an odd ntege n the szes and gves the suffcent condton poducng dstnct 8-QAM+ pefect aays. Fo dffeent choces of odd nteges n a gven sze of at least an odd ntege the esultant dstnct 8-QAM+pefect aays have the own szes. Fo each choce the numbe of the esultant dstnct 8-QAM+pefect aays s exactly equvalent to ths chosen odd ntege. Ths pape can povde moe canddates fo the applcatons of 8-QAM+ pefect aays n communcatons ada and so foth. Intoducton Pefect aays have the popety of mpulse-le autocoelaton whch esults n the fact that pefect aays ae wdely appled to communcatons ada tme-fequency-codng map matchng synchonzaton bult-n tests of VLSI-ccuts and so on [1]. Thee ae a lage numbe of pefect bnay tenay and ployphase aay [1]. Howeve 8-QAM+ pefect aays ae ae whose man eason les at the late ntoducton of 8-QAM+ constellaton []. In 1 Boztas and Paampall ntoduced the defnton of 8-QAM+ sgnal set []. Fom that tme on the sequences ove 8-QAM+ constellaton ae apdly developed. Pefect and odd pefect 8-QAM+ sequences ae gven n 1 and 14 espectvely [3] [4]. 8-QAM+ complementay sequences ae pesented n 1 and 14 espectvely [5] [6]. ZCZ 8-QAM+ sequences appeaed n 1 [7]. Recently 8-QAM+ pefect aays ae poposed n 14 and 15 [8] [9]. The am of ths pape s to nvestgate 8-QAM+ pefect aays to ncease the famly sze and to eflect the state-of-the-at of ths aea. A suffcent condton poducng dstnct 8-QAM+ pefect aays wll be ntoduced. The numbe of the esultant 8-QAM+ pefect aays wll be mpoved. The est of ths pape wll oganzed as follows. In Secton we wll evew some necessay concepts and the nown esults on the constuctons of 8-QAM+ pefect aays. In Secton 3 a suffcent condton poducng dstnct 8-QAM+ pefect aays wll be gven. The examples wll appea n Secton 4. Fnally we conclude ths pape n Secton 5. Necessay Concepts and Known Constuctons of 8-QAM+ Pefect Aays In a mathematcal tem an aay A of n - dmenson wth the sze N1 N Nn s A= a 1 1 n < N n (1) whose peodc autocoelaton s defned by N1 1N 1 Nn 1 * RAA ( τ1 τ τn) = a 1 a n 1 τ 1 τ n τ + + + n () 1= = n = whee the symbol x * denotes the complex-conjugate of x and the subscpt addton + τ (1 s pefomed modulo N. If the autocoelaton of an aay A of n - dmenson satsfes 15. The authos - Publshed by Atlants Pess 43

> ( τ1 τ τn) = ( ) RAA ( τ1 τ τn) = ( τ1 τ τn) ( ) (3) we efe to ths aay as pefect aay. Let the symbol T denote the n -dmensonal cyclcal shft opeato n othe wods fo a gven aay say A n (1) and gven n nteges µ s (1 unde ths opeato a new aay T( µ µ µ ) A can be gven by 1 n T( µ 1 µ µ n) A= a 1+ µ 1 + µ 1 n+ µ n < N n (4) whee the subscpt addton + µ (1 s counted modulo N. Let A and B be two aays wth the same sze. If thee exst n nteges µ s (1 so that T( µ 1 µ µ n) A= B (5) we say these two aays to be equvalent o else to be dstnct. The 8-QAM+ constellaton means the sgnal set []: + Ω 8 = { 11 j j 1 j1 + j1 j 1 + j}. (6) Based on the dect poduct { 1 1} { 1 1} the 8-QAM+ constellaton can be poduced by the followng mappngs: [3] + π : { 1 1} { 1 1} Ω8 (7) ( ab ) π ( ab ) whee π1( a b) = aj + b and π( a b) = aj b. (8) By the afoementoned mappngs a tenay aay can be conveted an 8-QAM+aay [8] [9]. The constucton methods efeed to n ths pape ae gven by the followng two Theoems. Theoem 1 [8] [9]: Let A be the pefect tenay aay (PTA) wth the sze N1 N Nn and η and δ (1 ae the nteges satsfyng N η δ N 1. If all the nteges N s (1 ae even and we have η d (mod N / ) (1 (9) the 8-QAM+ aay Q= q 1 1 n < N n wth the sze N1 N Nn s pefect whee q 1 = π 1 ( a 1 1 1 1 ) n + η + η a n+ ηn + δ + δ n+ δ. (1) n Theoem [8] [9]: Let A and B be two PTAs wth the same sze N1 N Nn whee at least an ntege n the set { N 1 n} s odd say N. Set the nteges η s δ s ζ s and λ s (1 satsfy N η δ ζ λ N 1. Constuct the 8-QAM+ aay P below. P= p 1 1 1 1 {1} n N n tt + < = + p 1 1 1 1 ( 1 1 1 1 1 1 1 1 1 1 1 1 ) f p a n η η η η b n ηn δ δ δ δ n δn + = + + + + + + + + + + + + + + =.(11) p = p ( a b ) f = 1 1 n 1 + ζ 1 1 + ζ 1 + ζ + ζ n+ ζn 1 + λ 1 1 + λ 1 + λ + λ+ 1 n+ λn If we have d η λ ζ mod N (1 n) ζ d η λ mod N (1 n ) (1) ζ d η λ mod N the 8-QAM+ aay P wth the sze N1 N 1 N N+ 1 Nn s pefect. Theoem 3 [8] [9]: The equaton system (11) has the soluton: 44

ζ η (mod N) η (1 n ) λ δ (mod N) δ (1 n ) N. (13) ζ η + (mod N) η N λ δ + (mod N) δ Poducton Pocedue of New Aays In ths secton we nvestgate the constucton method poducng dstnct 8-QAM+ pefect aays based on Theoem. Assume we need such aays wth the sze N1 N 1 N N+ 1 Nn whee N s odd numbe. The dstnct 8-QAM+ pefect aays can be educed by followng the gven steps below. Step 1: Choose two PTAs A and B wth the sze N1 N 1 N N+ 1 Nn Step : Intalzaton. Abtaly choose the nteges η s δ s ζ s and λ s (1 n ) Step 3: Intalzaton. Abtaly choose the nteges δ s (1 Step 4: Intalzaton. Detemne the ntege λ by Step 5: Iteaton tmes: t 1 Step 6: Set η = t 1 N d (mod N) λ + N 1 Step 7: Detemne the ntege ζ by + ζ η + (mod N) Step 8: Poduce 8-QAM+ aay P denoted by P t by Eq. (11) n Theoem Step 9: If t N 1 tun to Step 6 wth t t o else tun to Step 1 Step 1: End. Summazng the above we can obtan N dstnct 8-QAM+ pefect aays. Incdentally fo the eade who wants to now the detaled devaton of ths pocedue please efe to [8]. Examples Consde the poducton of 8-QAM+ pefect aays wth the sze 3 7. Choose the PTA wth the sze 3 7 below. 1 1 1 1 1 1 1 1 1 1. (14) 1 1 1 1 1 1 Note that = 1. In accodance wth ou steps we ntalze that ( δ1 δ ) = (1 ) ( η ζ ) = () and ( λ1 λ ) = (). Now we pefom ou pocedue as follows. (1) When the teaton tmes t = 1 we have ( η1 ζ ) = ( ). The esultant 8-QAM+ pefect aay s j 1 1 1+ j 1 1+ j 1+ 1 j j 1 j j 1 j 1 j 1+ j 1+ j 1 j 1+ j 1 j 1 j P =. (15) j 1 1 1+ j 1 1+ j 1+ j 1 j j 1 j j 1 j 1 j 1+ j 1+ j 1 j 1+ j 1 j 1 () When the teaton tmes t = we have ( η1 ζ ) = (1 ). The esultant 8-QAM+ pefect aay s gven by 45

1+ j 1+ j 1 j 1+ j 1 j 1 1 j 1 j 1 j 1 j + + + + 1+ j 1+ j 1 j 1+ j 1 j 1 j P1 =. (16) 1+ j 1+ j 1 j 1+ j 1 j 1 j 1+ j 1+ j 1+ j 1+ j 1+ j 1+ j 1 j 1+ j 1 j 1 (3) When the teaton tmes t = 3 we have ( η1 ζ ) = (1). The esultant 8-QAM+ pefect aay s equvalent to 1+ j 1+ j 1 j 1+ j 1 j 1 1 j j 1 j j 1 j 1 j j 1 1 1+ j 1 1+ j 1+ j P =. (17) 1+ j 1+ j 1 j 1+ j 1 j 1 j 1 j j 1 j j 1 j 1 j j 1 1 1+ j 1 1+ j 1+ The autocoelaton functons of all the aays P - P ae depcted n Fg.1 below. Appaently t s an mpulse-le functon as pomsed n ou pocedue. 7 6 5 Autocoelaton 4 3 1 5 tau1-5 -1-5 tau 5 1 Concluson Fg.1 Autocoelaton of the esultant 8-QAM+ pefect aays. Ths pape gves the poducton pocedue of 8-QAM+ pefect aays and some examples show ts valdaton. Howeve the flaw of ths pocedue les at the expanson of the sze of the esultant aays n compason wth the sze of the aays employed. It s ou futue wo to exploe new method so as to constuct the 8-QAM+ pefect aays wth the sze unalteed. Acnowledgement Ths wo was suppoted by Chongqng Scence and Technology Commttee (cstc14pt-sy43) and Natonal Natual Scence Foundaton of Chna (NSFC) unde Gants 687164 6134 61713 and 61471336 Chna Postdoctoal Scence Foundaton Gant 14M55318 Natual Scence Foundaton Poject of CQ Gant cstc14jcyj A45 and 46

Chongqng Postdoctoal Scence Specal Foundaton Gant Xm1431. Refeences [1] Pngzh Fan Mchael Danell. Sequence desgn fo communcatons applcatons. John Wley & Sons INC. 1996 Ch. 1. [] Seda Boztas Udaya Paampall. Nonbnay sequences wth pefect and nealy pefect autocoelatons. Poceedngs Intenatonal Symposum on Infomaton Theoy Austn Texas U.S.A. 1 13-134. [3] Fanxn Zeng et al. Pefect 8-QAM+ sequences. IEEE Weless Commun. Lett. 1 1(4) 388-391. [4] Yubo L et al. Odd pefect sequences and sequence sets wth zeo odd coelaton zone ove the 8-QAM+ constellaton. IEICE Tans. Fundamentals 14 E97-A(1) 45-48. [5] Fanxn Zeng et al. 8-QAM+ peodc complementay sequence sets IEEE Commun. Lett. 1 16(1) 83-85. [6] Fanxn Zeng et al. A note on 8-QAM+ sequences IEICE Tans. Fundamentals 14 E97-A(3) 888-893. [7] Yubo L et al. Zeo coelaton zone sequence sets ove the 8-QAM+ constellaton. IEEE Commun. Lett. 1 16(11) 1844-1847. [8] Fanxn Zeng et al. Pefect aays ove the 8-QAM+ constellaton. IEICE Tans. Fundamentals. 15 E98-A(4) 138-143. [9] Fanxn Zeng et al. Desgn of 8-QAM+ pefect aays fom pefect tenay aays. Poceedngs 14 7th Intenatonal Congess on Image and Sgnal Pocessng Dalan Chna 14 1185-119. 47