THE DIVERGENCE-FREE JACOBIAN CONJECTURE IN DIMENSION TWO

Size: px
Start display at page:

Download "THE DIVERGENCE-FREE JACOBIAN CONJECTURE IN DIMENSION TWO"

Transcription

1 THE DIVERGENCE-FREE JACOBIAN CONJECTURE IN DIMENSION TWO J. W. NEUBERGER Abtract. A pecial cae, called the divergence-free cae, of the Jacobian Conjecture in dimenion two i proved. Thi note outline an argument for a pecial cae of the Jacobian conjecture in dimenion two: Suppoe F : C 2 C 2 i a polnomial o that F (0) = 0, F (0) = I, det(f (z)) = 1, z C 2. (1) where I i the identit tranformation on C 2.Write r(x, )+x F (x, ) =, (x, ) C 2 (x, )+ where r, have no non-zero contant or linear term and oberve that det F = {r, } + +1 o that (1) give {r, } + = 0 (2) with {r, } = r 1 2 r 2 1, = r 1 + 2, the Poion bracket and divergence repectivel of the vector field (r, ), ubcript in thee intance indicating partial derivative in firt and econd argument. The main purpoe of thi note i to prove the following Theorem 1. Suppoe in addition to the above that {r, } =0, = 0. (3) Then F i bijective, i.e., the Jacobian conjecture hold in thi cae. Date: 18 November Mathematic Subject Claification. 14R15. Ke word and phrae. Jacobian Conjecture, Divergence-Free. 1

2 2 J.W.NEUBERGER We haten to point out that (3) doe not follow (no matter what thi writer ma have upected for ome time) automaticall. The following example communicated b Hman Ba howed the author expectation to be fale. Example 1. Suppoe each of a and b i a poitive integer greater than one and ( (x a + ) b ) + x F (x, ) = x a, (x, ) C 2. + It i ea to check that (1) hold but that (3) doe not. Neverthele the following indicate intance in which (3) hold. Corollar 1. Suppoe that all term of F of degree higher than one are even. Then (3) hold. Corollar 2. Suppoe that m>nare poitive integer and (n 1) 2 >m 1. If F i uch that all of it term of degree higher than one have their degree in [n, m], then(3) hold. In both cae there i no term in {, r} whichhaadegreeincommonwitha term of (r ). Hence thee two quantitie that um to zero mut each be zero. Therefore (2) implie (3) in thee two cae. Reference on the Jacobian Conjecture are [1],[4],[5]. An argument for Theorem 1 i baed on the following. Theorem 2. In order for (3) to hold, it i necear and ufficient that there be a linear tranformation L : C 2 C and a polnomial Q : C C 2 o that F (z) =z + Q(Lz) and L(Q(Lz)) = 0, z C 2. (4) Before a proof of Theorem 2, three lemma are given which indicate that if (4) hold then Theorem 1 follow. Lemma 1. If (4) hold, M C 2 and F (M) i bounded, then M i bounded, i.e., F i proper. Proof. [Lemma 1] Suppoe M i a ubet of C 2 and F (M) i bounded. Since L(F (M)) i then bounded, (4) ield that L(M) i alo bounded. But then Q(L(M)) i bounded and o then i M. Lemma 2. Under (4), uppoev, w C 2. There i a unique function u :[0, ) C 2 uch that u(0) = w, u (t) = (F (u(t))) 1 (F (u(t)), t 0. (5) Moreover, q = lim u(t) exit and F (q) =v. (6) t Proof. [Lemma 2] Suppoe that each of w, v C 2 and the equation in (5) hold with olution u for ome maximal interval [0,c),c>0. Then (F (u) = (F (u) on[0,c)

3 THE DIVERGENCE-FREE JACOBIAN CONJECTURE IN DIMENSION TWO 3 and o F (u(t)) v = e t (F (w), t [0,c). (7) Aume that c i finite. Then F (u([0,c))) i bounded and therefore uing Lemma 1, u([0,c)) i alo bounded. Conequentl, due to (5), u ([0,c))) i bounded too. But thi lat concluion give that p = lim t c u(t) exit. Therefore u ma be extended b continuit to [0,c] and conequentl the olution u can be further extended beond [0,c], contradicting the maximalit of [0,c). Thu c =. It follow that there i a olution u to (5) exactl a tated there. Hence uing (5), u decreae to zero exponentiall and o q = lim u(t) t exit. That F (q) =v follow from (7). For v C 2, define G v : C 2 C 2 o that G v (w) = lim t u(t) whereu atifie (5). Given v C 2,oneathatw i in the domain of attraction of q relative to (5) i.e., (G v ) 1 (q) i thi domain of attraction. Lemma 3. Under (4), F ha an invere defined on all of C 2. Proof. [Lemma 3] Suppoe that v C 2. From Lemma 1,2 it follow that ever member of C 2 i in the domain of attraction of ome z o that of F (z) =v. Denote b S v the preimage of v under F. The collection S v ha no limit point ince uch a limit point would be a place at which F i ingular. Hence from general principle of ordinar differential equation, a domain of attraction of an element of S v i an open et. Now C 2 i not the union of mutuall eparated open et. Hence the domain of attraction of an element of S v i all of C 2 and in fact S v contain jut one point. Thu there can not be two element q, q o that F (q) =F (q) ince two uch element would be ditinct member of S v. Lemma 1,2,3 impl that under (3) F i a bijection and hence Theorem 1 follow from Theorem 2 ince thee lemma follow from Theorem 2. See alo [4] in connection with thi lemma. It remain to prove Theorem 2. Proof. [Theorem 2] Under the hpothee of Theorem 2, {r, } =0. Nowifr, are both zero, the concluion urel hold. Accordingl uppoe that one of r and i not zero, a r. Notethatr i not contant. Denote b (α, β) apointof C 2 at which at leat one of the partial derivative r 1,r 2 i not zero. A claical reult on functional dependence (cf [2] for matter of differentiabilit) and (cf [3], p 426 for functional dependence) give that there i ɛ>0 and an analtic function h with domain the open ball B ɛ (radiu ɛ, center (α, β)) o that not both of r 1,r 2 are zero at an point of B ɛ and Note that then (x, ) = h(r(x, )), (x, ) B ɛ. (8) 2 (x, ) = h (r(x, ))r 2 (x, ), (x, ) B ɛ. (9)

4 4 J.W.NEUBERGER (9) together with (3) ield that r 1 (x, )+h (r(x, ))r 2 (x, ) =0, (x, ) B ɛ. (10) For r atifing the above and (γ,δ) B ɛ denote b ( u function with maximal domain in C o that (u ) r2 u γ = (u,, (0) =. v r 1 v δ Note that r(u, =0 and conequentl, r(u, andh(r(u, ) are contant. Denote the common value of h (r(u, ) b c. Uing (10), u 1 = r 2 (u,. v c Thi implie that direction of member of the range of ( u are contant and hence the range of ( u lie on the (complex) line 1 γ W γ,δ = { + : C}, c δ the line of lope c through ( γ δ). Hence r i contant on the interection of thi line and B ɛ and o b analticit, r i contant on all of W γ,δ. It will be een that each member of the et of line {W γ,δ :(γ,δ) B ɛ } (11) ha lope c. If two of thee line had different lope, the would cro; then ever member of (11) would cro at leat one of thee two and hence r would be contant on all of B ɛ (and hence all of C 2 ), a contradiction. Thu the member of (11) are parallel, all with lope c. Put another wa, r atifie on B ɛ the partial differential equation r 1 + cr 2 =0. (12) Hence there i a function f from a ubet of C to C o that r(x, ) =f(cx ), (x, ) B ɛ. (13) The function f clearl i a polnomial. Hence relation (13) extend b analticit to all of C 2. Moreover, (8), with h now known to be linear and homogeneou (actuall the action of h i jut multiplication b c) mutextendtoallofc 2 and conequentl the relationhip (8) extend to all of C 2.Thetwoextenion noted above give that r(x, ) f(cx Q(x, ) = =, (x, ) C 2, (x, cf(cx where the firt equalit above i b definition. Defining L : C 2 C b x L = cx, (x, ) C 2,

5 THE DIVERGENCE-FREE JACOBIAN CONJECTURE IN DIMENSION TWO 5 one ha P (z) = z + Q(Lz), z C 2. Since LQ(Lz) = 0,z C 2, it i hown that (3) implie (4). Now it i to be hown that (4) implie (3). Chooe Q, L o that (4) hold. Chooe a, b C uch that x x L = ax + b, C 2. Denote b each of g, h a polnomial from C to C o that x g(ax + b) Q =, (x, ) C 2. h(ax + b) If a =0=b, thenr =0= and the concluion hold, o uppoe that at leat one of a, b i not zero. From (4) it follow that ag(ax + b)+bh(ax + b) = 0, (x, ) C 2, and o ag + bh = 0 ince with proper choice for x,, ax + b ma be an member of C. Thu ( )(x, ) = (ag + bh) (ax + b) = 0, (x, ) C 2. Thu (3) hold and the argument i finihed. It ha alread been noted that Theorem 1 follow from Theorem 2. Reference [1] H. Ba, E. Connell, D. Wright, The Jacobian Conjecture; Reduction of Degree and Formal Expanion of the Invere, Bull. Amer. Math. Soc. 7 (1982), [2] T.M. Flett, Differential Anali, Cambridge Univerit Pre, [3] J. Olmtead, Real Variable, Appleton-Centur Math. Ser., [4] W. Rudin Injective Polnomial Map are Automorphim, Amer. Math. Monthl 102 (1995), [5] A. van den Een, Polnomial Automorphim and the Jacobian Conjecture, Semin. Congr. 2, Soc. Math. France (1997), Department of Mathematic, Univerit of North Texa, Denton, TX addre: jwn@unt.edu

Bogoliubov Transformation in Classical Mechanics

Bogoliubov Transformation in Classical Mechanics Bogoliubov Tranformation in Claical Mechanic Canonical Tranformation Suppoe we have a et of complex canonical variable, {a j }, and would like to conider another et of variable, {b }, b b ({a j }). How

More information

Convex Hulls of Curves Sam Burton

Convex Hulls of Curves Sam Burton Convex Hull of Curve Sam Burton 1 Introduction Thi paper will primarily be concerned with determining the face of convex hull of curve of the form C = {(t, t a, t b ) t [ 1, 1]}, a < b N in R 3. We hall

More information

TRIPLE SOLUTIONS FOR THE ONE-DIMENSIONAL

TRIPLE SOLUTIONS FOR THE ONE-DIMENSIONAL GLASNIK MATEMATIČKI Vol. 38583, 73 84 TRIPLE SOLUTIONS FOR THE ONE-DIMENSIONAL p-laplacian Haihen Lü, Donal O Regan and Ravi P. Agarwal Academy of Mathematic and Sytem Science, Beijing, China, National

More information

Problem Set 8 Solutions

Problem Set 8 Solutions Deign and Analyi of Algorithm April 29, 2015 Maachuett Intitute of Technology 6.046J/18.410J Prof. Erik Demaine, Srini Devada, and Nancy Lynch Problem Set 8 Solution Problem Set 8 Solution Thi problem

More information

SOLUTIONS TO ALGEBRAIC GEOMETRY AND ARITHMETIC CURVES BY QING LIU. I will collect my solutions to some of the exercises in this book in this document.

SOLUTIONS TO ALGEBRAIC GEOMETRY AND ARITHMETIC CURVES BY QING LIU. I will collect my solutions to some of the exercises in this book in this document. SOLUTIONS TO ALGEBRAIC GEOMETRY AND ARITHMETIC CURVES BY QING LIU CİHAN BAHRAN I will collect my olution to ome of the exercie in thi book in thi document. Section 2.1 1. Let A = k[[t ]] be the ring of

More information

Some Sets of GCF ϵ Expansions Whose Parameter ϵ Fetch the Marginal Value

Some Sets of GCF ϵ Expansions Whose Parameter ϵ Fetch the Marginal Value Journal of Mathematical Reearch with Application May, 205, Vol 35, No 3, pp 256 262 DOI:03770/jin:2095-26520503002 Http://jmredluteducn Some Set of GCF ϵ Expanion Whoe Parameter ϵ Fetch the Marginal Value

More information

7.2 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 281

7.2 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 281 72 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 28 and i 2 Show how Euler formula (page 33) can then be ued to deduce the reult a ( a) 2 b 2 {e at co bt} {e at in bt} b ( a) 2 b 2 5 Under what condition

More information

Lecture 21. The Lovasz splitting-off lemma Topics in Combinatorial Optimization April 29th, 2004

Lecture 21. The Lovasz splitting-off lemma Topics in Combinatorial Optimization April 29th, 2004 18.997 Topic in Combinatorial Optimization April 29th, 2004 Lecture 21 Lecturer: Michel X. Goeman Scribe: Mohammad Mahdian 1 The Lovaz plitting-off lemma Lovaz plitting-off lemma tate the following. Theorem

More information

UNIQUE CONTINUATION FOR A QUASILINEAR ELLIPTIC EQUATION IN THE PLANE

UNIQUE CONTINUATION FOR A QUASILINEAR ELLIPTIC EQUATION IN THE PLANE UNIQUE CONTINUATION FOR A QUASILINEAR ELLIPTIC EQUATION IN THE PLANE SEPPO GRANLUND AND NIKO MAROLA Abtract. We conider planar olution to certain quailinear elliptic equation ubject to the Dirichlet boundary

More information

A SIMPLE NASH-MOSER IMPLICIT FUNCTION THEOREM IN WEIGHTED BANACH SPACES. Sanghyun Cho

A SIMPLE NASH-MOSER IMPLICIT FUNCTION THEOREM IN WEIGHTED BANACH SPACES. Sanghyun Cho A SIMPLE NASH-MOSER IMPLICIT FUNCTION THEOREM IN WEIGHTED BANACH SPACES Sanghyun Cho Abtract. We prove a implified verion of the Nah-Moer implicit function theorem in weighted Banach pace. We relax the

More information

c n b n 0. c k 0 x b n < 1 b k b n = 0. } of integers between 0 and b 1 such that x = b k. b k c k c k

c n b n 0. c k 0 x b n < 1 b k b n = 0. } of integers between 0 and b 1 such that x = b k. b k c k c k 1. Exitence Let x (0, 1). Define c k inductively. Suppoe c 1,..., c k 1 are already defined. We let c k be the leat integer uch that x k An eay proof by induction give that and for all k. Therefore c n

More information

arxiv: v4 [math.co] 21 Sep 2014

arxiv: v4 [math.co] 21 Sep 2014 ASYMPTOTIC IMPROVEMENT OF THE SUNFLOWER BOUND arxiv:408.367v4 [math.co] 2 Sep 204 JUNICHIRO FUKUYAMA Abtract. A unflower with a core Y i a family B of et uch that U U Y for each two different element U

More information

Hybrid Control and Switched Systems. Lecture #6 Reachability

Hybrid Control and Switched Systems. Lecture #6 Reachability Hbrid Control and Switched Stem Lecture #6 Reachabilit João P. Hepanha Univerit of California at Santa Barbara Summar Review of previou lecture Reachabilit tranition tem reachabilit algorithm backward

More information

arxiv: v1 [math.mg] 25 Aug 2011

arxiv: v1 [math.mg] 25 Aug 2011 ABSORBING ANGLES, STEINER MINIMAL TREES, AND ANTIPODALITY HORST MARTINI, KONRAD J. SWANEPOEL, AND P. OLOFF DE WET arxiv:08.5046v [math.mg] 25 Aug 20 Abtract. We give a new proof that a tar {op i : i =,...,

More information

NULL HELIX AND k-type NULL SLANT HELICES IN E 4 1

NULL HELIX AND k-type NULL SLANT HELICES IN E 4 1 REVISTA DE LA UNIÓN MATEMÁTICA ARGENTINA Vol. 57, No. 1, 2016, Page 71 83 Publihed online: March 3, 2016 NULL HELIX AND k-type NULL SLANT HELICES IN E 4 1 JINHUA QIAN AND YOUNG HO KIM Abtract. We tudy

More information

Chapter 5 Consistency, Zero Stability, and the Dahlquist Equivalence Theorem

Chapter 5 Consistency, Zero Stability, and the Dahlquist Equivalence Theorem Chapter 5 Conitency, Zero Stability, and the Dahlquit Equivalence Theorem In Chapter 2 we dicued convergence of numerical method and gave an experimental method for finding the rate of convergence (aka,

More information

CHAPTER 8 OBSERVER BASED REDUCED ORDER CONTROLLER DESIGN FOR LARGE SCALE LINEAR DISCRETE-TIME CONTROL SYSTEMS

CHAPTER 8 OBSERVER BASED REDUCED ORDER CONTROLLER DESIGN FOR LARGE SCALE LINEAR DISCRETE-TIME CONTROL SYSTEMS CHAPTER 8 OBSERVER BASED REDUCED ORDER CONTROLLER DESIGN FOR LARGE SCALE LINEAR DISCRETE-TIME CONTROL SYSTEMS 8.1 INTRODUCTION 8.2 REDUCED ORDER MODEL DESIGN FOR LINEAR DISCRETE-TIME CONTROL SYSTEMS 8.3

More information

Feasible set in a discrete epidemic model

Feasible set in a discrete epidemic model Journal of Phic: Conference Serie Feaible et in a dicrete epidemic model To cite thi article: E-G Gu 008 J. Ph.: Conf. Ser. 96 05 View the article online for update and enhancement. Related content - Phic

More information

THE SPLITTING SUBSPACE CONJECTURE

THE SPLITTING SUBSPACE CONJECTURE THE SPLITTING SUBSPAE ONJETURE ERI HEN AND DENNIS TSENG Abtract We anwer a uetion by Niederreiter concerning the enumeration of a cla of ubpace of finite dimenional vector pace over finite field by proving

More information

OSCILLATIONS OF A CLASS OF EQUATIONS AND INEQUALITIES OF FOURTH ORDER * Zornitza A. Petrova

OSCILLATIONS OF A CLASS OF EQUATIONS AND INEQUALITIES OF FOURTH ORDER * Zornitza A. Petrova МАТЕМАТИКА И МАТЕМАТИЧЕСКО ОБРАЗОВАНИЕ, 2006 MATHEMATICS AND EDUCATION IN MATHEMATICS, 2006 Proceeding of the Thirty Fifth Spring Conference of the Union of Bulgarian Mathematician Borovet, April 5 8,

More information

List coloring hypergraphs

List coloring hypergraphs Lit coloring hypergraph Penny Haxell Jacque Vertraete Department of Combinatoric and Optimization Univerity of Waterloo Waterloo, Ontario, Canada pehaxell@uwaterloo.ca Department of Mathematic Univerity

More information

arxiv: v1 [math.ac] 30 Nov 2012

arxiv: v1 [math.ac] 30 Nov 2012 ON MODULAR INVARIANTS OF A VECTOR AND A COVECTOR YIN CHEN arxiv:73v [mathac 3 Nov Abtract Let S L (F q be the pecial linear group over a finite field F q, V be the -dimenional natural repreentation of

More information

MULTIPLE POSITIVE SOLUTIONS OF BOUNDARY VALUE PROBLEMS FOR P-LAPLACIAN IMPULSIVE DYNAMIC EQUATIONS ON TIME SCALES

MULTIPLE POSITIVE SOLUTIONS OF BOUNDARY VALUE PROBLEMS FOR P-LAPLACIAN IMPULSIVE DYNAMIC EQUATIONS ON TIME SCALES Fixed Point Theory, 5(24, No. 2, 475-486 http://www.math.ubbcluj.ro/ nodeacj/fptcj.html MULTIPLE POSITIVE SOLUTIONS OF BOUNDARY VALUE PROBLEMS FOR P-LAPLACIAN IMPULSIVE DYNAMIC EQUATIONS ON TIME SCALES

More information

ON A CERTAIN FAMILY OF QUARTIC THUE EQUATIONS WITH THREE PARAMETERS. Volker Ziegler Technische Universität Graz, Austria

ON A CERTAIN FAMILY OF QUARTIC THUE EQUATIONS WITH THREE PARAMETERS. Volker Ziegler Technische Universität Graz, Austria GLASNIK MATEMATIČKI Vol. 1(61)(006), 9 30 ON A CERTAIN FAMILY OF QUARTIC THUE EQUATIONS WITH THREE PARAMETERS Volker Ziegler Techniche Univerität Graz, Autria Abtract. We conider the parameterized Thue

More information

Preemptive scheduling on a small number of hierarchical machines

Preemptive scheduling on a small number of hierarchical machines Available online at www.ciencedirect.com Information and Computation 06 (008) 60 619 www.elevier.com/locate/ic Preemptive cheduling on a mall number of hierarchical machine György Dóa a, Leah Eptein b,

More information

Unbounded solutions of second order discrete BVPs on infinite intervals

Unbounded solutions of second order discrete BVPs on infinite intervals Available online at www.tjna.com J. Nonlinear Sci. Appl. 9 206), 357 369 Reearch Article Unbounded olution of econd order dicrete BVP on infinite interval Hairong Lian a,, Jingwu Li a, Ravi P Agarwal b

More information

Multicolor Sunflowers

Multicolor Sunflowers Multicolor Sunflower Dhruv Mubayi Lujia Wang October 19, 2017 Abtract A unflower i a collection of ditinct et uch that the interection of any two of them i the ame a the common interection C of all of

More information

Chapter 4. The Laplace Transform Method

Chapter 4. The Laplace Transform Method Chapter 4. The Laplace Tranform Method The Laplace Tranform i a tranformation, meaning that it change a function into a new function. Actually, it i a linear tranformation, becaue it convert a linear combination

More information

ON THE DETERMINATION OF NUMBERS BY THEIR SUMS OF A FIXED ORDER J. L. SELFRIDGE AND E. G. STRAUS

ON THE DETERMINATION OF NUMBERS BY THEIR SUMS OF A FIXED ORDER J. L. SELFRIDGE AND E. G. STRAUS ON THE DETERMINATION OF NUMBERS BY THEIR SUMS OF A FIXED ORDER J. L. SELFRIDGE AND E. G. STRAUS 1. Introduction. We wih to treat the following problem (uggeted by a problem of L. Moer [2]): Let {x} = {x

More information

March 18, 2014 Academic Year 2013/14

March 18, 2014 Academic Year 2013/14 POLITONG - SHANGHAI BASIC AUTOMATIC CONTROL Exam grade March 8, 4 Academic Year 3/4 NAME (Pinyin/Italian)... STUDENT ID Ue only thee page (including the back) for anwer. Do not ue additional heet. Ue of

More information

Lecture 17: Analytic Functions and Integrals (See Chapter 14 in Boas)

Lecture 17: Analytic Functions and Integrals (See Chapter 14 in Boas) Lecture 7: Analytic Function and Integral (See Chapter 4 in Boa) Thi i a good point to take a brief detour and expand on our previou dicuion of complex variable and complex function of complex variable.

More information

Correction for Simple System Example and Notes on Laplace Transforms / Deviation Variables ECHE 550 Fall 2002

Correction for Simple System Example and Notes on Laplace Transforms / Deviation Variables ECHE 550 Fall 2002 Correction for Simple Sytem Example and Note on Laplace Tranform / Deviation Variable ECHE 55 Fall 22 Conider a tank draining from an initial height of h o at time t =. With no flow into the tank (F in

More information

Lecture 3. January 9, 2018

Lecture 3. January 9, 2018 Lecture 3 January 9, 208 Some complex analyi Although you might have never taken a complex analyi coure, you perhap till know what a complex number i. It i a number of the form z = x + iy, where x and

More information

TAYLOR POLYNOMIALS FOR NABLA DYNAMIC EQUATIONS ON TIME SCALES

TAYLOR POLYNOMIALS FOR NABLA DYNAMIC EQUATIONS ON TIME SCALES TAYLOR POLYNOMIALS FOR NABLA DYNAMIC EQUATIONS ON TIME SCALES DOUGLAS R. ANDERSON Abtract. We are concerned with the repreentation of polynomial for nabla dynamic equation on time cale. Once etablihed,

More information

Control Systems Analysis and Design by the Root-Locus Method

Control Systems Analysis and Design by the Root-Locus Method 6 Control Sytem Analyi and Deign by the Root-Locu Method 6 1 INTRODUCTION The baic characteritic of the tranient repone of a cloed-loop ytem i cloely related to the location of the cloed-loop pole. If

More information

ON A CERTAIN FAMILY OF QUARTIC THUE EQUATIONS WITH THREE PARAMETERS

ON A CERTAIN FAMILY OF QUARTIC THUE EQUATIONS WITH THREE PARAMETERS ON A CERTAIN FAMILY OF QUARTIC THUE EQUATIONS WITH THREE PARAMETERS VOLKER ZIEGLER Abtract We conider the parameterized Thue equation X X 3 Y (ab + (a + bx Y abxy 3 + a b Y = ±1, where a, b 1 Z uch that

More information

LTV System Modelling

LTV System Modelling Helinki Univerit of Technolog S-72.333 Potgraduate Coure in Radiocommunication Fall 2000 LTV Stem Modelling Heikki Lorentz Sonera Entrum O heikki.lorentz@onera.fi Januar 23 rd 200 Content. Introduction

More information

The Hassenpflug Matrix Tensor Notation

The Hassenpflug Matrix Tensor Notation The Haenpflug Matrix Tenor Notation D.N.J. El Dept of Mech Mechatron Eng Univ of Stellenboch, South Africa e-mail: dnjel@un.ac.za 2009/09/01 Abtract Thi i a ample document to illutrate the typeetting of

More information

MATEMATIK Datum: Tid: eftermiddag. A.Heintz Telefonvakt: Anders Martinsson Tel.:

MATEMATIK Datum: Tid: eftermiddag. A.Heintz Telefonvakt: Anders Martinsson Tel.: MATEMATIK Datum: 20-08-25 Tid: eftermiddag GU, Chalmer Hjälpmedel: inga A.Heintz Telefonvakt: Ander Martinon Tel.: 073-07926. Löningar till tenta i ODE och matematik modellering, MMG5, MVE6. Define what

More information

Practice Problems - Week #7 Laplace - Step Functions, DE Solutions Solutions

Practice Problems - Week #7 Laplace - Step Functions, DE Solutions Solutions For Quetion -6, rewrite the piecewie function uing tep function, ketch their graph, and find F () = Lf(t). 0 0 < t < 2. f(t) = (t 2 4) 2 < t In tep-function form, f(t) = u 2 (t 2 4) The graph i the olid

More information

An Inequality for Nonnegative Matrices and the Inverse Eigenvalue Problem

An Inequality for Nonnegative Matrices and the Inverse Eigenvalue Problem An Inequality for Nonnegative Matrice and the Invere Eigenvalue Problem Robert Ream Program in Mathematical Science The Univerity of Texa at Dalla Box 83688, Richardon, Texa 7583-688 Abtract We preent

More information

Riemann s Functional Equation is Not Valid and its Implication on the Riemann Hypothesis. Armando M. Evangelista Jr.

Riemann s Functional Equation is Not Valid and its Implication on the Riemann Hypothesis. Armando M. Evangelista Jr. Riemann Functional Equation i Not Valid and it Implication on the Riemann Hypothei By Armando M. Evangelita Jr. On November 4, 28 ABSTRACT Riemann functional equation wa formulated by Riemann that uppoedly

More information

THE HAUSDORFF MEASURE OF SIERPINSKI CARPETS BASING ON REGULAR PENTAGON

THE HAUSDORFF MEASURE OF SIERPINSKI CARPETS BASING ON REGULAR PENTAGON Anal. Theory Appl. Vol. 28, No. (202), 27 37 THE HAUSDORFF MEASURE OF SIERPINSKI CARPETS BASING ON REGULAR PENTAGON Chaoyi Zeng, Dehui Yuan (Hanhan Normal Univerity, China) Shaoyuan Xu (Gannan Normal Univerity,

More information

Given the following circuit with unknown initial capacitor voltage v(0): X(s) Immediately, we know that the transfer function H(s) is

Given the following circuit with unknown initial capacitor voltage v(0): X(s) Immediately, we know that the transfer function H(s) is EE 4G Note: Chapter 6 Intructor: Cheung More about ZSR and ZIR. Finding unknown initial condition: Given the following circuit with unknown initial capacitor voltage v0: F v0/ / Input xt 0Ω Output yt -

More information

An Interesting Property of Hyperbolic Paraboloids

An Interesting Property of Hyperbolic Paraboloids Page v w Conider the generic hyperbolic paraboloid defined by the equation. u = where a and b are aumed a b poitive. For our purpoe u, v and w are a permutation of x, y, and z. A typical graph of uch a

More information

New bounds for Morse clusters

New bounds for Morse clusters New bound for More cluter Tamá Vinkó Advanced Concept Team, European Space Agency, ESTEC Keplerlaan 1, 2201 AZ Noordwijk, The Netherland Tama.Vinko@ea.int and Arnold Neumaier Fakultät für Mathematik, Univerität

More information

Linear System Fundamentals

Linear System Fundamentals Linear Sytem Fundamental MEM 355 Performance Enhancement of Dynamical Sytem Harry G. Kwatny Department of Mechanical Engineering & Mechanic Drexel Univerity Content Sytem Repreentation Stability Concept

More information

SECTION x2 x > 0, t > 0, (8.19a)

SECTION x2 x > 0, t > 0, (8.19a) SECTION 8.5 433 8.5 Application of aplace Tranform to Partial Differential Equation In Section 8.2 and 8.3 we illutrated the effective ue of aplace tranform in olving ordinary differential equation. The

More information

Geometric Measure Theory

Geometric Measure Theory Geometric Meaure Theory Lin, Fall 010 Scribe: Evan Chou Reference: H. Federer, Geometric meaure theory L. Simon, Lecture on geometric meaure theory P. Mittila, Geometry of et and meaure in Euclidean pace

More information

SOME RESULTS ON INFINITE POWER TOWERS

SOME RESULTS ON INFINITE POWER TOWERS NNTDM 16 2010) 3, 18-24 SOME RESULTS ON INFINITE POWER TOWERS Mladen Vailev - Miana 5, V. Hugo Str., Sofia 1124, Bulgaria E-mail:miana@abv.bg Abtract To my friend Kratyu Gumnerov In the paper the infinite

More information

POINCARE INEQUALITY AND CAMPANATO ESTIMATES FOR WEAK SOLUTIONS OF PARABOLIC EQUATIONS

POINCARE INEQUALITY AND CAMPANATO ESTIMATES FOR WEAK SOLUTIONS OF PARABOLIC EQUATIONS Electronic Journal of Differential Equation, Vol. 206 (206), No. 204, pp. 8. ISSN: 072-669. URL: http://ejde.math.txtate.edu or http://ejde.math.unt.edu POINCARE INEQUALITY AND CAMPANATO ESTIMATES FOR

More information

arxiv:math/ v4 [math.ag] 1 Aug 2007

arxiv:math/ v4 [math.ag] 1 Aug 2007 arxiv:math/0603259v4 [math.ag] 1 Aug 2007 CONNECTIONS ON MODULES OVER QUASI-HOMOGENEOUS PLANE CURVES EIVIND ERIKSEN Abtract. Let k be an algebraically cloed field of characteritic 0, and let A = k[x,y]/(f)

More information

Introduction to Laplace Transform Techniques in Circuit Analysis

Introduction to Laplace Transform Techniques in Circuit Analysis Unit 6 Introduction to Laplace Tranform Technique in Circuit Analyi In thi unit we conider the application of Laplace Tranform to circuit analyi. A relevant dicuion of the one-ided Laplace tranform i found

More information

ON MULTIPLE AND INFINITE LOG-CONCAVITY

ON MULTIPLE AND INFINITE LOG-CONCAVITY ON MULTIPLE AND INFINITE LOG-CONCAVITY LUIS A. MEDINA AND ARMIN STRAUB Abtract. Following Boro Moll, a equence (a n) i m-log-concave if L j (a n) 0 for all j = 0,,..., m. Here, L i the operator defined

More information

Pacific Journal of Mathematics

Pacific Journal of Mathematics Pacific Journal of Mathematic OSCILLAION AND NONOSCILLAION OF FORCED SECOND ORDER DYNAMIC EQUAIONS MARIN BOHNER AND CHRISOPHER C. ISDELL Volume 230 No. March 2007 PACIFIC JOURNAL OF MAHEMAICS Vol. 230,

More information

A PROOF OF TWO CONJECTURES RELATED TO THE ERDÖS-DEBRUNNER INEQUALITY

A PROOF OF TWO CONJECTURES RELATED TO THE ERDÖS-DEBRUNNER INEQUALITY Volume 8 2007, Iue 3, Article 68, 3 pp. A PROOF OF TWO CONJECTURES RELATED TO THE ERDÖS-DEBRUNNER INEQUALITY C. L. FRENZEN, E. J. IONASCU, AND P. STĂNICĂ DEPARTMENT OF APPLIED MATHEMATICS NAVAL POSTGRADUATE

More information

Singular perturbation theory

Singular perturbation theory Singular perturbation theory Marc R. Rouel June 21, 2004 1 Introduction When we apply the teady-tate approximation (SSA) in chemical kinetic, we typically argue that ome of the intermediate are highly

More information

On the convexity of the function C f(det C) on positive-definite matrices

On the convexity of the function C f(det C) on positive-definite matrices Article On the convexit of the function C fdet C) on poitive-definite matrice Mathematic and Mechanic of Solid 2014, Vol 194) 369 375 The Author) 2013 Reprint and permiion: agepubcouk/journalpermiionnav

More information

Flag-transitive non-symmetric 2-designs with (r, λ) = 1 and alternating socle

Flag-transitive non-symmetric 2-designs with (r, λ) = 1 and alternating socle Flag-tranitive non-ymmetric -deign with (r, λ = 1 and alternating ocle Shenglin Zhou, Yajie Wang School of Mathematic South China Univerity of Technology Guangzhou, Guangdong 510640, P. R. China lzhou@cut.edu.cn

More information

REVERSE HÖLDER INEQUALITIES AND INTERPOLATION

REVERSE HÖLDER INEQUALITIES AND INTERPOLATION REVERSE HÖLDER INEQUALITIES AND INTERPOLATION J. BASTERO, M. MILMAN, AND F. J. RUIZ Abtract. We preent new method to derive end point verion of Gehring Lemma uing interpolation theory. We connect revere

More information

Riemann s Functional Equation is Not a Valid Function and Its Implication on the Riemann Hypothesis. Armando M. Evangelista Jr.

Riemann s Functional Equation is Not a Valid Function and Its Implication on the Riemann Hypothesis. Armando M. Evangelista Jr. Riemann Functional Equation i Not a Valid Function and It Implication on the Riemann Hypothei By Armando M. Evangelita Jr. armando78973@gmail.com On Augut 28, 28 ABSTRACT Riemann functional equation wa

More information

Pythagorean Triple Updated 08--5 Drlnoordzij@leennoordzijnl wwwleennoordzijme Content A Roadmap for generating Pythagorean Triple Pythagorean Triple 3 Dicuion Concluion 5 A Roadmap for generating Pythagorean

More information

Assignment for Mathematics for Economists Fall 2016

Assignment for Mathematics for Economists Fall 2016 Due date: Mon. Nov. 1. Reading: CSZ, Ch. 5, Ch. 8.1 Aignment for Mathematic for Economit Fall 016 We now turn to finihing our coverage of concavity/convexity. There are two part: Jenen inequality for concave/convex

More information

Linear Motion, Speed & Velocity

Linear Motion, Speed & Velocity Add Important Linear Motion, Speed & Velocity Page: 136 Linear Motion, Speed & Velocity NGSS Standard: N/A MA Curriculum Framework (006): 1.1, 1. AP Phyic 1 Learning Objective: 3.A.1.1, 3.A.1.3 Knowledge/Undertanding

More information

Lecture 9: Shor s Algorithm

Lecture 9: Shor s Algorithm Quantum Computation (CMU 8-859BB, Fall 05) Lecture 9: Shor Algorithm October 7, 05 Lecturer: Ryan O Donnell Scribe: Sidhanth Mohanty Overview Let u recall the period finding problem that wa et up a a function

More information

Manprit Kaur and Arun Kumar

Manprit Kaur and Arun Kumar CUBIC X-SPLINE INTERPOLATORY FUNCTIONS Manprit Kaur and Arun Kumar manpreet2410@gmail.com, arun04@rediffmail.com Department of Mathematic and Computer Science, R. D. Univerity, Jabalpur, INDIA. Abtract:

More information

On the Function ω(n)

On the Function ω(n) International Mathematical Forum, Vol. 3, 08, no. 3, 07 - HIKARI Ltd, www.m-hikari.com http://doi.org/0.988/imf.08.708 On the Function ω(n Rafael Jakimczuk Diviión Matemática, Univeridad Nacional de Luján

More information

Lecture 8: Period Finding: Simon s Problem over Z N

Lecture 8: Period Finding: Simon s Problem over Z N Quantum Computation (CMU 8-859BB, Fall 205) Lecture 8: Period Finding: Simon Problem over Z October 5, 205 Lecturer: John Wright Scribe: icola Rech Problem A mentioned previouly, period finding i a rephraing

More information

NUMBERS. := p n 1 + p n 2 q + p n 3 q pq n 2 + q n 1 = pn q n p q. We can write easily that [n] p,q. , where [n] q/p

NUMBERS. := p n 1 + p n 2 q + p n 3 q pq n 2 + q n 1 = pn q n p q. We can write easily that [n] p,q. , where [n] q/p Kragujevac Journal of Mathematic Volume 424) 2018), Page 555 567 APOSTOL TYPE p, q)-frobenius-euler POLYNOMIALS AND NUMBERS UGUR DURAN 1 AND MEHMET ACIKGOZ 2 Abtract In the preent paper, we introduce p,

More information

ON THE APPROXIMATION ERROR IN HIGH DIMENSIONAL MODEL REPRESENTATION. Xiaoqun Wang

ON THE APPROXIMATION ERROR IN HIGH DIMENSIONAL MODEL REPRESENTATION. Xiaoqun Wang Proceeding of the 2008 Winter Simulation Conference S. J. Maon, R. R. Hill, L. Mönch, O. Roe, T. Jefferon, J. W. Fowler ed. ON THE APPROXIMATION ERROR IN HIGH DIMENSIONAL MODEL REPRESENTATION Xiaoqun Wang

More information

COHOMOLOGY AS A LOCAL-TO-GLOBAL BRIDGE

COHOMOLOGY AS A LOCAL-TO-GLOBAL BRIDGE COHOMOLOGY AS A LOCAL-TO-GLOBAL BRIDGE LIVIU I. NICOLAESCU ABSTRACT. I dicu low dimenional incarnation of cohomology and illutrate how baic cohomological principle lead to a proof of Sperner lemma. CONTENTS.

More information

On the Unit Groups of a Class of Total Quotient Rings of Characteristic p k with k 3

On the Unit Groups of a Class of Total Quotient Rings of Characteristic p k with k 3 International Journal of Algebra, Vol, 207, no 3, 27-35 HIKARI Ltd, wwwm-hikaricom http://doiorg/02988/ija2076750 On the Unit Group of a Cla of Total Quotient Ring of Characteritic p k with k 3 Wanambii

More information

2 where. x 1 θ = 1 θ = 0.6 x 2 θ = 0 θ = 0.2

2 where. x 1 θ = 1 θ = 0.6 x 2 θ = 0 θ = 0.2 Convex et I a ne and convex et I ome important example I operation that preerve convexity I eparating and upporting hyperplane I generalized inequalitie I dual cone and generalized inequalitie IOE 6: Nonlinear

More information

Convergence criteria and optimization techniques for beam moments

Convergence criteria and optimization techniques for beam moments Pure Appl. Opt. 7 (1998) 1221 1230. Printed in the UK PII: S0963-9659(98)90684-5 Convergence criteria and optimization technique for beam moment G Gbur and P S Carney Department of Phyic and Atronomy and

More information

Advanced methods for ODEs and DAEs

Advanced methods for ODEs and DAEs Lecture : Implicit Runge Kutta method Bojana Roić, 9. April 7 What you need to know before thi lecture numerical integration: Lecture from ODE iterative olver: Lecture 5-8 from ODE 9. April 7 Bojana Roić

More information

A relationship between generalized Davenport-Schinzel sequences and interval chains

A relationship between generalized Davenport-Schinzel sequences and interval chains A relationhip between generalized Davenport-Schinzel equence and interval chain The MIT Faculty ha made thi article openly available. Pleae hare how thi acce benefit you. Your tory matter. Citation A Publihed

More information

AN INTEGRAL FORMULA FOR COMPACT HYPERSURFACES IN SPACE FORMS AND ITS APPLICATIONS

AN INTEGRAL FORMULA FOR COMPACT HYPERSURFACES IN SPACE FORMS AND ITS APPLICATIONS J. Aut. ath. Soc. 74 (2003), 239 248 AN INTEGRAL FORULA FOR COPACT HYPERSURFACES IN SPACE FORS AND ITS APPLICATIONS LUIS J. ALÍAS (Received 5 December 2000; revied 8 arch 2002) Communicated by K. Wyocki

More information

Electronic Theses and Dissertations

Electronic Theses and Dissertations Eat Tenneee State Univerity Digital Common @ Eat Tenneee State Univerity Electronic Thee and Diertation Student Work 5-208 Vector Partition Jennifer French Eat Tenneee State Univerity Follow thi and additional

More information

3. In an interaction between two objects, each object exerts a force on the other. These forces are equal in magnitude and opposite in direction.

3. In an interaction between two objects, each object exerts a force on the other. These forces are equal in magnitude and opposite in direction. Lecture quiz toda. Small change to webite. Problem 4.30 the peed o the elevator i poitive even though it i decending. The WebAign anwer i wrong. ewton Law o Motion (page 9-99) 1. An object velocit vector

More information

arxiv: v2 [math.co] 11 Sep 2017

arxiv: v2 [math.co] 11 Sep 2017 The maximum number of clique in graph without long cycle Ruth Luo September 13, 017 arxiv:1701.0747v [math.co] 11 Sep 017 Abtract The Erdő Gallai Theorem tate that for k 3 every graph on n vertice with

More information

Nonlinear Single-Particle Dynamics in High Energy Accelerators

Nonlinear Single-Particle Dynamics in High Energy Accelerators Nonlinear Single-Particle Dynamic in High Energy Accelerator Part 6: Canonical Perturbation Theory Nonlinear Single-Particle Dynamic in High Energy Accelerator Thi coure conit of eight lecture: 1. Introduction

More information

Solving Differential Equations by the Laplace Transform and by Numerical Methods

Solving Differential Equations by the Laplace Transform and by Numerical Methods 36CH_PHCalter_TechMath_95099 3//007 :8 PM Page Solving Differential Equation by the Laplace Tranform and by Numerical Method OBJECTIVES When you have completed thi chapter, you hould be able to: Find the

More information

CDMA Signature Sequences with Low Peak-to-Average-Power Ratio via Alternating Projection

CDMA Signature Sequences with Low Peak-to-Average-Power Ratio via Alternating Projection CDMA Signature Sequence with Low Peak-to-Average-Power Ratio via Alternating Projection Joel A Tropp Int for Comp Engr and Sci (ICES) The Univerity of Texa at Autin 1 Univerity Station C0200 Autin, TX

More information

Simple Observer Based Synchronization of Lorenz System with Parametric Uncertainty

Simple Observer Based Synchronization of Lorenz System with Parametric Uncertainty IOSR Journal of Electrical and Electronic Engineering (IOSR-JEEE) ISSN: 78-676Volume, Iue 6 (Nov. - Dec. 0), PP 4-0 Simple Oberver Baed Synchronization of Lorenz Sytem with Parametric Uncertainty Manih

More information

Codes Correcting Two Deletions

Codes Correcting Two Deletions 1 Code Correcting Two Deletion Ryan Gabry and Frederic Sala Spawar Sytem Center Univerity of California, Lo Angele ryan.gabry@navy.mil fredala@ucla.edu Abtract In thi work, we invetigate the problem of

More information

Adelic Modular Forms

Adelic Modular Forms Aelic Moular Form October 3, 20 Motivation Hecke theory i concerne with a family of finite-imenional vector pace S k (N, χ), inexe by weight, level, an character. The Hecke operator on uch pace alreay

More information

EE 508 Lecture 16. Filter Transformations. Lowpass to Bandpass Lowpass to Highpass Lowpass to Band-reject

EE 508 Lecture 16. Filter Transformations. Lowpass to Bandpass Lowpass to Highpass Lowpass to Band-reject EE 508 Lecture 6 Filter Tranformation Lowpa to Bandpa Lowpa to Highpa Lowpa to Band-reject Review from Lat Time Theorem: If the perimeter variation and contact reitance are neglected, the tandard deviation

More information

ON THE UNIQUENESS OF MEROMORPHIC FUNCTIONS SHARING THREE WEIGHTED VALUES. Indrajit Lahiri and Gautam Kumar Ghosh

ON THE UNIQUENESS OF MEROMORPHIC FUNCTIONS SHARING THREE WEIGHTED VALUES. Indrajit Lahiri and Gautam Kumar Ghosh MATEMATIQKI VESNIK 60 (008), 5 3 UDK 517.546 originalni nauqni rad reearch aer ON THE UNIQUENESS OF MEROMORPHIC FUNCTIONS SHARING THREE WEIGHTED VALUES Indrajit Lahiri and Gautam Kumar Ghoh Abtract. We

More information

AN EXAMPLE FOR THE GENERALIZATION OF THE INTEGRATION OF SPECIAL FUNCTIONS BY USING THE LAPLACE TRANSFORM

AN EXAMPLE FOR THE GENERALIZATION OF THE INTEGRATION OF SPECIAL FUNCTIONS BY USING THE LAPLACE TRANSFORM Journal of Inequalitie Special Function ISSN: 7-433, URL: http://www.iliria.com Volume 6 Iue 5, Page 5-3. AN EXAMPLE FOR THE GENERALIZATION OF THE INTEGRATION OF SPECIAL FUNCTIONS BY USING THE LAPLACE

More information

The Laplace Transform

The Laplace Transform Chapter 7 The Laplace Tranform 85 In thi chapter we will explore a method for olving linear differential equation with contant coefficient that i widely ued in electrical engineering. It involve the tranformation

More information

IEOR 3106: Fall 2013, Professor Whitt Topics for Discussion: Tuesday, November 19 Alternating Renewal Processes and The Renewal Equation

IEOR 3106: Fall 2013, Professor Whitt Topics for Discussion: Tuesday, November 19 Alternating Renewal Processes and The Renewal Equation IEOR 316: Fall 213, Profeor Whitt Topic for Dicuion: Tueday, November 19 Alternating Renewal Procee and The Renewal Equation 1 Alternating Renewal Procee An alternating renewal proce alternate between

More information

Extension of Inagaki General Weighted Operators. and. A New Fusion Rule Class of Proportional Redistribution of Intersection Masses

Extension of Inagaki General Weighted Operators. and. A New Fusion Rule Class of Proportional Redistribution of Intersection Masses Extenion of nagaki General Weighted Operator and A New Fuion Rule Cla of Proportional Reditribution of nterection Mae Florentin Smarandache Chair of Math & Science Depart. Univerity of New Mexico, Gallup,

More information

Robustness analysis for the boundary control of the string equation

Robustness analysis for the boundary control of the string equation Routne analyi for the oundary control of the tring equation Martin GUGAT Mario SIGALOTTI and Mariu TUCSNAK I INTRODUCTION AND MAIN RESULTS In thi paper we conider the infinite dimenional ytem determined

More information

Position. If the particle is at point (x, y, z) on the curved path s shown in Fig a,then its location is defined by the position vector

Position. If the particle is at point (x, y, z) on the curved path s shown in Fig a,then its location is defined by the position vector 34 C HAPTER 1 KINEMATICS OF A PARTICLE 1 1.5 Curvilinear Motion: Rectangular Component Occaionall the motion of a particle can bet be decribed along a path that can be epreed in term of it,, coordinate.

More information

arxiv: v2 [math.nt] 30 Apr 2015

arxiv: v2 [math.nt] 30 Apr 2015 A THEOREM FOR DISTINCT ZEROS OF L-FUNCTIONS École Normale Supérieure arxiv:54.6556v [math.nt] 3 Apr 5 943 Cachan November 9, 7 Abtract In thi paper, we etablih a imple criterion for two L-function L and

More information

NAME (pinyin/italian)... MATRICULATION NUMBER... SIGNATURE

NAME (pinyin/italian)... MATRICULATION NUMBER... SIGNATURE POLITONG SHANGHAI BASIC AUTOMATIC CONTROL June Academic Year / Exam grade NAME (pinyin/italian)... MATRICULATION NUMBER... SIGNATURE Ue only thee page (including the bac) for anwer. Do not ue additional

More information

EC381/MN308 Probability and Some Statistics. Lecture 7 - Outline. Chapter Cumulative Distribution Function (CDF) Continuous Random Variables

EC381/MN308 Probability and Some Statistics. Lecture 7 - Outline. Chapter Cumulative Distribution Function (CDF) Continuous Random Variables EC38/MN38 Probability and Some Statitic Yanni Pachalidi yannip@bu.edu, http://ionia.bu.edu/ Lecture 7 - Outline. Continuou Random Variable Dept. of Manufacturing Engineering Dept. of Electrical and Computer

More information

Weber Schafheitlin-type integrals with exponent 1

Weber Schafheitlin-type integrals with exponent 1 Integral Tranform and Special Function Vol., No., February 9, 47 53 Weber Schafheitlin-type integral with exponent Johanne Kellendonk* and Serge Richard Univerité de Lyon, Univerité Lyon, Intitut Camille

More information

Approximate Analytical Solution for Quadratic Riccati Differential Equation

Approximate Analytical Solution for Quadratic Riccati Differential Equation Iranian J. of Numerical Analyi and Optimization Vol 3, No. 2, 2013), pp 21-31 Approximate Analytical Solution for Quadratic Riccati Differential Equation H. Aminikhah Abtract In thi paper, we introduce

More information

Representation Formulas of Curves in a Two- and Three-Dimensional Lightlike Cone

Representation Formulas of Curves in a Two- and Three-Dimensional Lightlike Cone Reult. Math. 59 (011), 437 451 c 011 Springer Bael AG 14-6383/11/030437-15 publihed online April, 011 DOI 10.1007/0005-011-0108-y Reult in Mathematic Repreentation Formula of Curve in a Two- and Three-Dimenional

More information