ON 3-DIMENSIONAL CONTACT METRIC MANIFOLDS
|
|
- Arthur Walsh
- 5 years ago
- Views:
Transcription
1 Mem. Fac. Inegaed As and Sci., Hioshima Univ., Se. IV, Vol , Dec. 00 ON 3-DIMENSIONAL CONTACT METRIC MANIFOLDS YOSHIO AGAOKA *, BYUNG HAK KIM ** AND JIN HYUK CHOI ** *Depamen of Mahemaics, Faculy of Inegaed As and Sciences, Hioshima Univesiy, Higashi-Hioshima , Japan **Depamen of Mahemaics and Insiue of Naual Sciences, Kyung Hee Univesiy, Suwon , Koea Absac Le M be a 3-dimensional almos conac meic manifold saisfying (*)-condiion. We denoe such a manifold by M *. We pove ha if M * is η-einsein, hen M * is eihe Sasaian o cosymplecic manifold, and is a space of consan cuvaue. Consequenly M * is eihe fla o isomeic o he 3-dimensional uni sphee if M * is complee and simply conneced. 1. Inoducion The confomal cuvaue enso C is invaian unde confomal ansfomaions and vanishes idenically fo 3-dimensional manifolds. Using his fac many auhos [1, 3, 4, 6] sudied 3-dimensional almos conac manifolds. In [5], hey inoduced a new class of almos conac manifold M * conaining quasi-sasaian and ans-sasaian sucue. Moeove hey consuced non-ivial examples. In his pape, we sudy a 3- dimensional η-einsein manifold M * by use of he fac ha C vanishes idenically and he special fom of Ricci cuvaue. Consequenly, we pove ha he 3-dimensional η-einsein manifold M * becomes eihe Sasaian o cosymplecic manifold, and is a space of consan cuvaue. In he cosymplecic case, M * is fla, and if M * is Sasaian, complee and simply conneced, hen M * is isomeic o he 3-dimensional uni sphee, ha is M * is eihe fla o isomeic o S 3 (1) unde his opological condiion.. Almos conac meic sucue Le M be an m-dimensional eal diffeeniable manifold of class C coveed by a sysem of coodinae neighbohoods { Ux ; h, in which hee ae given a enso field φ of ype (1,1), a veco field ξ and a 1-fom η saisfying (.1) φ X = X η( X) ξ, φ ξ = 0, η( φx)= 0, η( ξ)= 1 fo any veco field X on M. Such a se of φξη,, is called an almos conac sucue and we call a manifold wih an almos conac sucue an almos conac manifold. In an almos conac manifold, if hee is given a Riemannian meic g such ha Key wods: Confomal cuvaue enso, almos conac meic manifold, space of consan cuvaue. ** This wo was suppoed by ABRL Gan Poj. No. R fom KOSEF and Engineeing Foundaion. Received Ocobe 1 00; Acceped Novembe 1 00
2 30 YOSHIO AGAOKA, BYUNG HAK KIM AND JIN HYUK CHOI fo all veco fields X and Y on M, we say M has an almos conac meic sucue and g is called a compaible meic. Seing Y = ξ, we have immediaely η( X)= g( X, ξ). The fundamenal -fom Φ is defined by Φ( XY, )= g( φxy, ). I is nown ha he almos conac sucue φξη,, is nomal if and only if he Nijenhuis enso g ( φx, φy )= g ( X, Y ) η( X) η( Y) NXY, φφ, ( X,Y) dη( X, Y) ξ = [ ] vanishes, whee [, ] is a bace opeaion and d denoes he exeio deivaive. An almos conac meic sucue ( φξη,,,g) on M is said o be (a) Sasaian if Φ = dη and ( φξη,, ) is nomal, (b) cosymplecic if Φ and η ae closed and ( φξη,, ) is nomal. In [5], one of he pesen auho defined a new class of almos conac meic sucue on M which saisfies (*) d Φ = 0, ξ = λφx X and ( φξη,, ) is nomal fo a smooh funcion λ on M and denoes he Riemannian connecion fo g. Biefly, we denoe such a manifold by M *. I is easily seen ha M * is cosymplecic if λ = 0, and Sasaian if λ is a non-zeo consan. Theoem 1 [5]. On M *, we have (.) (.3) (.4) (.5) ( φ)( YZ, )= λ η( Y) g( XZ, ) η( g( XY, ), X { = { RX, ξ Y Xλ φy λ η YX g XY, ξ, ξλ = 0, = S ξ, X φx λ ( m 1) λ η( X), whee S is he Ricci cuvaue enso and R is he cuvaue enso defined by [ X Y] [ XY, ] RXYZ (, ) =, Z Z dimensional almos conac manifolds Le M * be a 3-dimensional manifold saisfying (*). I is well nown [] ha he confomal cuvaue enso of Weyl vanishes idenically fo 3-dimensional manifolds. Theefoe he cuvaue enso R of a 3- dimensional manifold M * is given by (3.1) RXYZ (, ) = SXZY (, ) SYZX (, ) g( XZQY, ) { g( YZQX, ) g( XZY, ) g ( YZX, ),
3 ON 3-DIMENSIONAL CONTACT METRIC MANIFOLDS 31 whee is he scala cuvaue and Q is defined by g( QX, Y)= S( X, Y). Using (.3), (.5) and (3.1), we have (3.) = SXY, η X φyλ η Y φxλ g XY, X Y. λ λ 3 η η( ) If we subsiue (3.) ino (3.1), hen we ge (3.3) RXYZW (,,, )= g RXYZW (, ), = η( X) (( φ λ) g( Y, W) η( (( φx) λ) g ( Y, W) η( Y) (( φ λ) g( XW, ) η( (( φy) λ) g( XW, ) η( Y) (( φw) λ) g( X, η( W) (( φy) λ) g( X, η( X) (( φw) λ) g ( Y, η( W) (( φx) λ) g ( Y, λ g( XZ, ) g( YW, ) g( YZ, ) g( XW, ) 3λ η( X) ( Y W) η( Y) ( X W) η Z { g, g, η( Y) g( X, η( X) g( Y, η( W). { If we pu Y = ξ in (3.3), hen by (.3) we obain ha is (3.4) (3.5) o in local componens (3.6) whee λ = λ and he indices i, j,, un ove he ange {1,,...,m. Fom (3.5) o (3.6), we can calculae (3.7) whee λ = g i λ i ( Xλ) Φ( Z, W) λ { η( g( X, W) η( W) g( X, = λ { η( g( X, W) η( W) g( X, (( φw) λ) { η( X) η( g( X, (( φ λ) { η( X) η( W) g ( X, W), ( Xλ) Φ( Z, W)= (( φw) λ) { η( X) η( g( X,. Moeove we can easily see ha ( ){ φz λ η X η W g X, W, λ φ λ ( ηη ) φ λ, Φih= h i gi i ηη h gh ij Φij =( λφij) λ Φ i = φλ λ. = 4 λ φ λ, = 0 Lemma. In a 3-dimensional manifold M *, he funcion λ is consan if and only if φx λ fo all X. i
4 3 YOSHIO AGAOKA, BYUNG HAK KIM AND JIN HYUK CHOI If he Ricci cuvaue S on M is of he fom (3.8) SXY (, )= ag( XY, ) bη( X) η( Y), hen M is called an η-einsein space [1,6,7]. If M * is η-einsein, hen we have (3.9) 3a b = and (3.10) a b = 4λ by use of (.1), (3.) and (3.8). Hence we ge a = λ and b = 6λ. Theefoe he Ricci cuvaue S becomes (3.11) = ( ) SXY, λ g XY, 6λ η X η Y. If we pu Y = ξ in (3.11), hen we ge (3.1) = ( 6 ) φx λ λ η X fom (.5) and (3.11). If we se X = ξ in (3.1), hen i gives (3.13) =, 6λ ha is (3.14) ( φx) λ = 0 and ha (3.15) (, )= λ g( XY, ) SXY fom (3.11). We see ha λ is consan fom Lemma and (3.14). Since 3-dimensional Einsein space is a space of consan cuvaue, we obain he following heoem by using Lemma, (3.14) and (3.15). Theoem 3. Le M * be a 3-dimensional η-einsein manifold. Then M * is a space of consan cuvaue. Moeove M * is eihe Sasaian o cosymplecic manifold. In case λ = 0, since M * is a space of consan cuvaue, we have = 0 and hence RXYZ (, ) = 0, ha is M * is fla. On he ohe hand, E. M. Mosal obained he following esul (cf. [7]). Theoem 4. Le M be a complee and simply conneced Sasaian manifold. If M is Einsein and of posiive cuvaue, hen i is isomeic o he uni sphee. If λ is non-zeo consan, hen M * is Sasaian. Theefoe his fac and Theoems 3 and 4 educe
5 ON 3-DIMENSIONAL CONTACT METRIC MANIFOLDS 33 Theoem 5. Le M * be a 3-dimensional η-einsein manifold. Then M * is eihe fla o isomeic o S 3 (1) if M * is complee and simply conneced. Acnowledgemen. The auhos would lie o expess hei hans o he efeee fo his caeful eading and helpful suggesions. Refeences 1. D. E. Blai, Riemannian geomey of conac and symplecic manifolds, PM03, Bihäuse, Belin (00).. B. Y. Chen, Geomey of submanifolds, Macel Dee, New Yo (1973). 3. F. Gouli-Andeou and P. J. Xenos, On a class of 3-dimensional conac meic manifolds, J. Geom., 63 (1998), J. B. Jun, I. B. Kim and U. K. Kim, On 3-dimensional almos conac meic manifolds, Kyungpoo Mah. J., 34 (1994), J. H. Kwon and B. H. Kim, A new class of almos conac Riemannian manifolds, Comm. Koean Mah. Soc., 8 (1993), S. Sasai, Almos conac manifolds, Lecue noes, Mahemaical Insiue, Tohou Univ. 1 (1965). 7. S. Tanno, Pomenades on sphees, Toyo Ins. Tech., Toyo (1996).
On Control Problem Described by Infinite System of First-Order Differential Equations
Ausalian Jounal of Basic and Applied Sciences 5(): 736-74 ISS 99-878 On Conol Poblem Descibed by Infinie Sysem of Fis-Ode Diffeenial Equaions Gafujan Ibagimov and Abbas Badaaya J'afau Insiue fo Mahemaical
More informationBMOA estimates and radial growth of B φ functions
c Jounal of echnical Univesiy a Plovdiv Fundamenal Sciences and Applicaions, Vol., 995 Seies A-Pue and Applied Mahemaics Bulgaia, ISSN 3-827 axiv:87.53v [mah.cv] 3 Jul 28 BMOA esimaes and adial gowh of
More information336 ERIDANI kfk Lp = sup jf(y) ; f () jj j p p whee he supemum is aken ove all open balls = (a ) inr n, jj is he Lebesgue measue of in R n, () =(), f
TAMKANG JOURNAL OF MATHEMATIS Volume 33, Numbe 4, Wine 2002 ON THE OUNDEDNESS OF A GENERALIED FRATIONAL INTEGRAL ON GENERALIED MORREY SPAES ERIDANI Absac. In his pape we exend Nakai's esul on he boundedness
More informationMean Curvature and Shape Operator of Slant Immersions in a Sasakian Space Form
Mean Cuvatue and Shape Opeato of Slant Immesions in a Sasakian Space Fom Muck Main Tipathi, Jean-Sic Kim and Son-Be Kim Abstact Fo submanifolds, in a Sasakian space fom, which ae tangential to the stuctue
More information7 Wave Equation in Higher Dimensions
7 Wave Equaion in Highe Dimensions We now conside he iniial-value poblem fo he wave equaion in n dimensions, u c u x R n u(x, φ(x u (x, ψ(x whee u n i u x i x i. (7. 7. Mehod of Spheical Means Ref: Evans,
More informationThe shortest path between two truths in the real domain passes through the complex domain. J. Hadamard
Complex Analysis R.G. Halbud R.Halbud@ucl.ac.uk Depamen of Mahemaics Univesiy College London 202 The shoes pah beween wo uhs in he eal domain passes hough he complex domain. J. Hadamad Chape The fis fundamenal
More informationCombinatorial Approach to M/M/1 Queues. Using Hypergeometric Functions
Inenaional Mahemaical Foum, Vol 8, 03, no 0, 463-47 HIKARI Ld, wwwm-hikaicom Combinaoial Appoach o M/M/ Queues Using Hypegeomeic Funcions Jagdish Saan and Kamal Nain Depamen of Saisics, Univesiy of Delhi,
More information@FMI c Kyung Moon Sa Co.
Annals of Fuzzy Mahemaics Infomaics Volume, No. 2, (Apil 20), pp. 9-3 ISSN 2093 930 hp://www.afmi.o.k @FMI c Kyung Moon Sa Co. hp://www.kyungmoon.com On lacunay saisical convegence in inuiionisic fuzzy
More informationLecture 18: Kinetics of Phase Growth in a Two-component System: general kinetics analysis based on the dilute-solution approximation
Lecue 8: Kineics of Phase Gowh in a Two-componen Sysem: geneal kineics analysis based on he dilue-soluion appoximaion Today s opics: In he las Lecues, we leaned hee diffeen ways o descibe he diffusion
More informationENGI 4430 Advanced Calculus for Engineering Faculty of Engineering and Applied Science Problem Set 9 Solutions [Theorems of Gauss and Stokes]
ENGI 44 Avance alculus fo Engineeing Faculy of Engineeing an Applie cience Poblem e 9 oluions [Theoems of Gauss an okes]. A fla aea A is boune by he iangle whose veices ae he poins P(,, ), Q(,, ) an R(,,
More informationDual Hierarchies of a Multi-Component Camassa Holm System
Commun. heo. Phys. 64 05 37 378 Vol. 64, No. 4, Ocobe, 05 Dual Hieachies of a Muli-Componen Camassa Holm Sysem LI Hong-Min, LI Yu-Qi, and CHEN Yong Shanghai Key Laboaoy of uswohy Compuing, Eas China Nomal
More informationExtremal problems for t-partite and t-colorable hypergraphs
Exemal poblems fo -paie and -coloable hypegaphs Dhuv Mubayi John Talbo June, 007 Absac Fix ineges and an -unifom hypegaph F. We pove ha he maximum numbe of edges in a -paie -unifom hypegaph on n veices
More informationMEEN 617 Handout #11 MODAL ANALYSIS OF MDOF Systems with VISCOUS DAMPING
MEEN 67 Handou # MODAL ANALYSIS OF MDOF Sysems wih VISCOS DAMPING ^ Symmeic Moion of a n-dof linea sysem is descibed by he second ode diffeenial equaions M+C+K=F whee () and F () ae n ows vecos of displacemens
More informationResearch Article A Note on Multiplication and Composition Operators in Lorentz Spaces
Hindawi Publishing Copoaion Jounal of Funcion Spaces and Applicaions Volume 22, Aicle ID 29363, pages doi:.55/22/29363 Reseach Aicle A Noe on Muliplicaion and Composiion Opeaos in Loenz Spaces Eddy Kwessi,
More informationDegree of Approximation of a Class of Function by (C, 1) (E, q) Means of Fourier Series
IAENG Inenaional Jounal of Applied Mahemaic, 4:, IJAM_4 7 Degee of Appoximaion of a Cla of Funcion by C, E, q Mean of Fouie Seie Hae Kihna Nigam and Kuum Shama Abac In hi pape, fo he fi ime, we inoduce
More informationLecture-V Stochastic Processes and the Basic Term-Structure Equation 1 Stochastic Processes Any variable whose value changes over time in an uncertain
Lecue-V Sochasic Pocesses and he Basic Tem-Sucue Equaion 1 Sochasic Pocesses Any vaiable whose value changes ove ime in an unceain way is called a Sochasic Pocess. Sochasic Pocesses can be classied as
More informationOrder statistics and concentration of l r norms for log-concave vectors
Jounal of Funcional Analysis 61 011 681 696 www.elsevie.com/locae/jfa Ode saisics and concenaion of l noms fo log-concave vecos Rafał Laała a,b, a Insiue of Mahemaics, Univesiy of Wasaw, Banacha, 0-097
More informationGeneral Non-Arbitrage Model. I. Partial Differential Equation for Pricing A. Traded Underlying Security
1 Geneal Non-Abiage Model I. Paial Diffeenial Equaion fo Picing A. aded Undelying Secuiy 1. Dynamics of he Asse Given by: a. ds = µ (S, )d + σ (S, )dz b. he asse can be eihe a sock, o a cuency, an index,
More informationOn the Semi-Discrete Davey-Stewartson System with Self-Consistent Sources
Jounal of Applied Mahemaics and Physics 25 3 478-487 Published Online May 25 in SciRes. hp://www.scip.og/jounal/jamp hp://dx.doi.og/.4236/jamp.25.356 On he Semi-Discee Davey-Sewason Sysem wih Self-Consisen
More informationPOSITIVE SOLUTIONS WITH SPECIFIC ASYMPTOTIC BEHAVIOR FOR A POLYHARMONIC PROBLEM ON R n. Abdelwaheb Dhifli
Opuscula Mah. 35, no. (205), 5 9 hp://dx.doi.og/0.7494/opmah.205.35..5 Opuscula Mahemaica POSITIVE SOLUTIONS WITH SPECIFIC ASYMPTOTIC BEHAVIOR FOR A POLYHARMONIC PROBLEM ON R n Abdelwaheb Dhifli Communicaed
More informationLecture 22 Electromagnetic Waves
Lecue Elecomagneic Waves Pogam: 1. Enegy caied by he wave (Poyning veco).. Maxwell s equaions and Bounday condiions a inefaces. 3. Maeials boundaies: eflecion and efacion. Snell s Law. Quesions you should
More informationReichenbach and f-generated implications in fuzzy database relations
INTERNATIONAL JOURNAL O CIRCUITS SYSTEMS AND SIGNAL PROCESSING Volume 08 Reichenbach and f-geneaed implicaions in fuzzy daabase elaions Nedžad Dukić Dženan Gušić and Nemana Kajmoić Absac Applying a definiion
More informationComputer Propagation Analysis Tools
Compue Popagaion Analysis Tools. Compue Popagaion Analysis Tools Inoducion By now you ae pobably geing he idea ha pedicing eceived signal sengh is a eally impoan as in he design of a wieless communicaion
More informationFuzzy Hv-submodules in Γ-Hv-modules Arvind Kumar Sinha 1, Manoj Kumar Dewangan 2 Department of Mathematics NIT Raipur, Chhattisgarh, India
Inenaional Jounal of Engineeing Reseach (IJOER) [Vol-1, Issue-1, Apil.- 2015] Fuzz v-submodules in Γ-v-modules Avind Kuma Sinha 1, Manoj Kuma Dewangan 2 Depamen of Mahemaics NIT Raipu, Chhaisgah, India
More informationMonochromatic Wave over One and Two Bars
Applied Mahemaical Sciences, Vol. 8, 204, no. 6, 307-3025 HIKARI Ld, www.m-hikai.com hp://dx.doi.og/0.2988/ams.204.44245 Monochomaic Wave ove One and Two Bas L.H. Wiyano Faculy of Mahemaics and Naual Sciences,
More informationThe sudden release of a large amount of energy E into a background fluid of density
10 Poin explosion The sudden elease of a lage amoun of enegy E ino a backgound fluid of densiy ceaes a song explosion, chaaceized by a song shock wave (a blas wave ) emanaing fom he poin whee he enegy
More informationONTHEPATHWISEUNIQUENESSOF STOCHASTIC PARTIAL DIFFERENTIAL EQUATIONS WITH NON-LIPSCHITZ COEFFICIENTS
OCKY MOUNTAIN JOUNAL OF MATHEMATICS Volume 43, Numbe 5, 213 ONTHEPATHWISEUNIQUENESSOF STOCHASTIC PATIAL DIFFEENTIAL EQUATIONS WITH NON-LIPSCHITZ COEFFICIENTS DEFEI ZHANG AND PING HE ABSTACT. In hi pape,
More informationA note on characterization related to distributional properties of random translation, contraction and dilation of generalized order statistics
PobSa Foum, Volume 6, July 213, Pages 35 41 ISSN 974-3235 PobSa Foum is an e-jounal. Fo eails please visi www.pobsa.og.in A noe on chaaceizaion elae o isibuional popeies of anom anslaion, conacion an ilaion
More informationOrthotropic Materials
Kapiel 2 Ohoopic Maeials 2. Elasic Sain maix Elasic sains ae elaed o sesses by Hooke's law, as saed below. The sesssain elaionship is in each maeial poin fomulaed in he local caesian coodinae sysem. ε
More informationTHE MODULAR INEQUALITIES FOR A CLASS OF CONVOLUTION OPERATORS ON MONOTONE FUNCTIONS
PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 5, Numbe 8, Augus 997, Pages 93 35 S -9939(973867-7 THE MODULAR INEQUALITIES FOR A CLASS OF CONVOLUTION OPERATORS ON MONOTONE FUNCTIONS JIM QILE
More informationA STOCHASTIC MODELING FOR THE UNSTABLE FINANCIAL MARKETS
A STOCHASTIC MODELING FOR THE UNSTABLE FINANCIAL MARKETS Assoc. Pof. Romeo Negea Ph. D Poliehnica Univesiy of Timisoaa Depamen of Mahemaics Timisoaa, Romania Assoc. Pof. Cipian Peda Ph. D Wes Univesiy
More informationSecure Frameproof Codes Through Biclique Covers
Discee Mahemaics and Theoeical Compue Science DMTCS vol. 4:2, 202, 26 270 Secue Famepoof Codes Though Biclique Coves Hossein Hajiabolhassan,2 and Faokhlagha Moazami 3 Depamen of Mahemaical Sciences, Shahid
More informationK. G. Malyutin, T. I. Malyutina, I. I. Kozlova ON SUBHARMONIC FUNCTIONS IN THE HALF-PLANE OF INFINITE ORDER WITH RADIALLY DISTRIBUTED MEASURE
Математичнi Студiї. Т.4, 2 Maemaychni Sudii. V.4, No.2 УДК 57.5 K. G. Malyuin, T. I. Malyuina, I. I. Kozlova ON SUBHARMONIC FUNCTIONS IN THE HALF-PLANE OF INFINITE ORDER WITH RADIALLY DISTRIBUTED MEASURE
More informationLecture 17: Kinetics of Phase Growth in a Two-component System:
Lecue 17: Kineics of Phase Gowh in a Two-componen Sysem: descipion of diffusion flux acoss he α/ ineface Today s opics Majo asks of oday s Lecue: how o deive he diffusion flux of aoms. Once an incipien
More informationMATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH
Fundamenal Jounal of Mahemaical Phsics Vol 3 Issue 013 Pages 55-6 Published online a hp://wwwfdincom/ MATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH Univesias
More informationSTUDY OF THE STRESS-STRENGTH RELIABILITY AMONG THE PARAMETERS OF GENERALIZED INVERSE WEIBULL DISTRIBUTION
Inenaional Jounal of Science, Technology & Managemen Volume No 04, Special Issue No. 0, Mach 205 ISSN (online): 2394-537 STUDY OF THE STRESS-STRENGTH RELIABILITY AMONG THE PARAMETERS OF GENERALIZED INVERSE
More informationAVERAGING OF ENTIRE FUNCTIONS OF IMPROVED REGULAR GROWTH WITH ZEROS ON A FINITE SYSTEM OF RAYS R.V. Khats
ÂIÑÍÈÊ ÍÀÖIÎÍÀËÜÍÎÃÎ ÓÍIÂÅÐÑÈÒÅÒÓ ËÜÂIÂÑÜÊÀ ÏÎËIÒÅÕÍIÊÀ Ôiçèêî-ìàòåìàòè íi íàóêè Âèï.718 718, (211) c. 114 JOURNAL OF NATIONAL UNIVERSITY LVIVSKA POLITECHNIKA Physical & mahemaical sciences Vol.718 No
More informationFINITE DIFFERENCE APPROACH TO WAVE GUIDE MODES COMPUTATION
FINITE DIFFERENCE ROCH TO WVE GUIDE MODES COMUTTION Ing.lessando Fani Elecomagneic Gou Deamen of Elecical and Eleconic Engineeing Univesiy of Cagliai iazza d mi, 93 Cagliai, Ialy SUMMRY Inoducion Finie
More informationarxiv: v1 [math.co] 4 Apr 2019
Dieced dominaion in oiened hypegaphs axiv:1904.02351v1 [mah.co] 4 Ap 2019 Yai Cao Dep. of Mahemaics Univesiy of Haifa-Oanim Tivon 36006, Isael yacao@kvgeva.og.il This pape is dedicaed o Luz Volkmann on
More informationAngular momentum in general relativity: The definition at null infinity includes the spatial definition as a special case
PHYSICL REVIEW D, VOLUME 63, 04002 ngula momenum in geneal elaiviy: The definiion a null infiniy includes he spaial definiion as a special case nhony Rizzi Califonia Insiue of Technology, LIGO, Livingson,
More informationGRADIENT ESTIMATES FOR A SIMPLE PARABOLIC LICHNEROWICZ EQUATION. Osaka Journal of Mathematics. 51(1) P.245-P.256
Tile Auhor(s) GRADIENT ESTIMATES FOR A SIMPLE PARABOLIC LICHNEROWICZ EQUATION Zhao, Liang Ciaion Osaka Journal of Mahemaics. 51(1) P.45-P.56 Issue Dae 014-01 Tex Version publisher URL hps://doi.org/10.18910/9195
More informationRelations on the Apostol Type (p, q)-frobenius-euler Polynomials and Generalizations of the Srivastava-Pintér Addition Theorems
Tish Joal of Aalysis ad Nmbe Theoy 27 Vol 5 No 4 26-3 Available olie a hp://pbssciepbcom/ja/5/4/2 Sciece ad Edcaio Pblishig DOI:269/ja-5-4-2 Relaios o he Aposol Type (p -Fobeis-Ele Polyomials ad Geealizaios
More informationConvergence of the Neumann series in higher norms
Convergence of he Neumann series in higher norms Charles L. Epsein Deparmen of Mahemaics, Universiy of Pennsylvania Version 1.0 Augus 1, 003 Absrac Naural condiions on an operaor A are given so ha he Neumann
More informationVariance and Covariance Processes
Vaiance and Covaiance Pocesses Pakash Balachandan Depamen of Mahemaics Duke Univesiy May 26, 2008 These noes ae based on Due s Sochasic Calculus, Revuz and Yo s Coninuous Maingales and Bownian Moion, Kaazas
More informationKINEMATICS OF RIGID BODIES
KINEMTICS OF RIGID ODIES In igid body kinemaics, we use he elaionships govening he displacemen, velociy and acceleaion, bu mus also accoun fo he oaional moion of he body. Descipion of he moion of igid
More informationODEs II, Lecture 1: Homogeneous Linear Systems - I. Mike Raugh 1. March 8, 2004
ODEs II, Lecure : Homogeneous Linear Sysems - I Mike Raugh March 8, 4 Inroducion. In he firs lecure we discussed a sysem of linear ODEs for modeling he excreion of lead from he human body, saw how o ransform
More informationSharif University of Technology - CEDRA By: Professor Ali Meghdari
Shaif Univesiy of echnology - CEDRA By: Pofesso Ali Meghai Pupose: o exen he Enegy appoach in eiving euaions of oion i.e. Lagange s Meho fo Mechanical Syses. opics: Genealize Cooinaes Lagangian Euaion
More informationON THE EXISTENCE OF NEARLY QUASI-EINSTEIN MANIFOLDS. 1. Introduction. Novi Sad J. Math. Vol. 39, No. 2, 2009,
Novi Sad J. Math. Vol. 39, No. 2, 2009, 111-117 ON THE EXISTENCE OF NEARLY QUASI-EINSTEIN MANIFOLDS Abul Kalam Gazi 1, Uday Chand De 2 Abstact. The objective of the pesent pape is to establish the existence
More informationOn the 5-dimensional Sasaki-Einstein manifold
Proceedings of The Fourteenth International Workshop on Diff. Geom. 14(2010) 171-175 On the 5-dimensional Sasaki-Einstein manifold Byung Hak Kim Department of Applied Mathematics, Kyung Hee University,
More informationThe Miki-type identity for the Apostol-Bernoulli numbers
Annales Mahemaicae e Informaicae 46 6 pp. 97 4 hp://ami.ef.hu The Mii-ype ideniy for he Aposol-Bernoulli numbers Orli Herscovici, Toufi Mansour Deparmen of Mahemaics, Universiy of Haifa, 3498838 Haifa,
More informationDeviation probability bounds for fractional martingales and related remarks
Deviaion pobabiliy bounds fo facional maingales and elaed emaks Buno Sausseeau Laboaoie de Mahémaiques de Besançon CNRS, UMR 6623 16 Roue de Gay 253 Besançon cedex, Fance Absac In his pape we pove exponenial
More informationSobolev-type Inequality for Spaces L p(x) (R N )
In. J. Conemp. Mah. Sciences, Vol. 2, 27, no. 9, 423-429 Sobolev-ype Inequaliy for Spaces L p(x ( R. Mashiyev and B. Çekiç Universiy of Dicle, Faculy of Sciences and Ars Deparmen of Mahemaics, 228-Diyarbakir,
More informationVariational Iteration Method for Solving System of Fractional Order Ordinary Differential Equations
IOSR Journal of Mahemaics (IOSR-JM) e-issn: 2278-5728, p-issn: 2319-765X. Volume 1, Issue 6 Ver. II (Nov - Dec. 214), PP 48-54 Variaional Ieraion Mehod for Solving Sysem of Fracional Order Ordinary Differenial
More informationAsymptotic instability of nonlinear differential equations
Elecronic Journal of Differenial Equaions, Vol. 1997(1997), No. 16, pp. 1 7. ISSN: 172-6691. URL: hp://ejde.mah.sw.edu or hp://ejde.mah.un.edu fp (login: fp) 147.26.13.11 or 129.12.3.113 Asympoic insabiliy
More informationfunctions on localized Morrey-Campanato spaces over doubling metric measure spaces
JOURNAL OF FUNCTION SPACES AND APPLICATIONS Volume 9, Numbe 3 2), 245 282 c 2, Scienific Hoizon hp://www.jfsa.ne oundedness of Lusin-aea and gλ funcions on localized Moey-Campanao spaces ove doubling meic
More informationMapping Properties Of The General Integral Operator On The Classes R k (ρ, b) And V k (ρ, b)
Applied Mahemaics E-Noes, 15(215), 14-21 c ISSN 167-251 Available free a mirror sies of hp://www.mah.nhu.edu.w/ amen/ Mapping Properies Of The General Inegral Operaor On The Classes R k (ρ, b) And V k
More informationBOUNDEDNESS OF MAXIMAL FUNCTIONS ON NON-DOUBLING MANIFOLDS WITH ENDS
BOUNDEDNESS OF MAXIMAL FUNCTIONS ON NON-DOUBLING MANIFOLDS WITH ENDS XUAN THINH DUONG, JI LI, AND ADAM SIKORA Absrac Le M be a manifold wih ends consruced in [2] and be he Laplace-Belrami operaor on M
More informationON A CLASS OF N(k)-CONTACT METRIC MANIFOLDS
ON A CLASS OF N(k)-CONTACT METRIC MANIFOLDS UDAY CHAND DE, AHMET YILDIZ and SUJIT GHOSH Communicated by the fome editoial boad The object of the pesent pape is to study ξ-conciculaly flat and φ-conciculaly
More informationProperties Of Solutions To A Generalized Liénard Equation With Forcing Term
Applied Mahemaics E-Noes, 8(28), 4-44 c ISSN 67-25 Available free a mirror sies of hp://www.mah.nhu.edu.w/ amen/ Properies Of Soluions To A Generalized Liénard Equaion Wih Forcing Term Allan Kroopnick
More informationAn Automatic Door Sensor Using Image Processing
An Auomaic Doo Senso Using Image Pocessing Depamen o Elecical and Eleconic Engineeing Faculy o Engineeing Tooi Univesiy MENDEL 2004 -Insiue o Auomaion and Compue Science- in BRNO CZECH REPUBLIC 1. Inoducion
More informationGeneralized Chebyshev polynomials
Generalized Chebyshev polynomials Clemene Cesarano Faculy of Engineering, Inernaional Telemaic Universiy UNINETTUNO Corso Viorio Emanuele II, 39 86 Roma, Ialy email: c.cesarano@unineunouniversiy.ne ABSTRACT
More informationCERTAIN CLASSES OF SOLUTIONS OF LAGERSTROM EQUATIONS
SARAJEVO JOURNAL OF MATHEMATICS Vol.10 (22 (2014, 67 76 DOI: 10.5644/SJM.10.1.09 CERTAIN CLASSES OF SOLUTIONS OF LAGERSTROM EQUATIONS ALMA OMERSPAHIĆ AND VAHIDIN HADŽIABDIĆ Absrac. This paper presens sufficien
More informationSystem of Linear Differential Equations
Sysem of Linear Differenial Equaions In "Ordinary Differenial Equaions" we've learned how o solve a differenial equaion for a variable, such as: y'k5$e K2$x =0 solve DE yx = K 5 2 ek2 x C_C1 2$y''C7$y
More informationOn The Estimation of Two Missing Values in Randomized Complete Block Designs
Mahemaical Theoy and Modeling ISSN 45804 (Pape ISSN 505 (Online Vol.6, No.7, 06 www.iise.og On The Esimaion of Two Missing Values in Randomized Complee Bloc Designs EFFANGA, EFFANGA OKON AND BASSE, E.
More informationOn Two Integrability Methods of Improper Integrals
Inernaional Journal of Mahemaics and Compuer Science, 13(218), no. 1, 45 5 M CS On Two Inegrabiliy Mehods of Improper Inegrals H. N. ÖZGEN Mahemaics Deparmen Faculy of Educaion Mersin Universiy, TR-33169
More informationHomotopy Perturbation Method for Solving Some Initial Boundary Value Problems with Non Local Conditions
Proceedings of he World Congress on Engineering and Compuer Science 23 Vol I WCECS 23, 23-25 Ocober, 23, San Francisco, USA Homoopy Perurbaion Mehod for Solving Some Iniial Boundary Value Problems wih
More informationON AN EXTENDED CONTACT BOCHNER CURVATURE TENSOR ON CONTACT METRIC MANIFOLDS
C O L L O Q U I U M M A T H E M A T I C U M VOL. LXV 1993 FASC. 1 ON AN EXTENDED CONTACT BOCHNER CURVATURE TENSOR ON CONTACT METRIC MANIFOLDS BY HIROSHI E N D O (ICHIKAWA) 1. Introduction. On Sasakian
More informationAverage Number of Lattice Points in a Disk
Average Number of Laice Poins in a Disk Sujay Jayakar Rober S. Sricharz Absrac The difference beween he number of laice poins in a disk of radius /π and he area of he disk /4π is equal o he error in he
More informationTHE GENERALIZED PASCAL MATRIX VIA THE GENERALIZED FIBONACCI MATRIX AND THE GENERALIZED PELL MATRIX
J Korean Mah Soc 45 008, No, pp 479 49 THE GENERALIZED PASCAL MATRIX VIA THE GENERALIZED FIBONACCI MATRIX AND THE GENERALIZED PELL MATRIX Gwang-yeon Lee and Seong-Hoon Cho Reprined from he Journal of he
More informationThe Asymptotic Behavior of Nonoscillatory Solutions of Some Nonlinear Dynamic Equations on Time Scales
Advances in Dynamical Sysems and Applicaions. ISSN 0973-5321 Volume 1 Number 1 (2006, pp. 103 112 c Research India Publicaions hp://www.ripublicaion.com/adsa.hm The Asympoic Behavior of Nonoscillaory Soluions
More informationSolution of Integro-Differential Equations by Using ELzaki Transform
Global Journal of Mahemaical Sciences: Theory and Pracical. Volume, Number (), pp. - Inernaional Research Publicaion House hp://www.irphouse.com Soluion of Inegro-Differenial Equaions by Using ELzaki Transform
More informationReading from Young & Freedman: For this topic, read sections 25.4 & 25.5, the introduction to chapter 26 and sections 26.1 to 26.2 & 26.4.
PHY1 Elecriciy Topic 7 (Lecures 1 & 11) Elecric Circuis n his opic, we will cover: 1) Elecromoive Force (EMF) ) Series and parallel resisor combinaions 3) Kirchhoff s rules for circuis 4) Time dependence
More informationEssential Maps and Coincidence Principles for General Classes of Maps
Filoma 31:11 (2017), 3553 3558 hps://doi.org/10.2298/fil1711553o Published by Faculy of Sciences Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma Essenial Maps Coincidence
More informationBoundedness and Stability of Solutions of Some Nonlinear Differential Equations of the Third-Order.
Boundedness Sabili of Soluions of Some Nonlinear Differenial Equaions of he Third-Order. A.T. Ademola, M.Sc. * P.O. Arawomo, Ph.D. Deparmen of Mahemaics Saisics, Bowen Universi, Iwo, Nigeria. Deparmen
More informationAN EVOLUTIONARY APPROACH FOR SOLVING DIFFERENTIAL EQUATIONS
AN EVOLUTIONARY APPROACH FOR SOLVING DIFFERENTIAL EQUATIONS M. KAMESWAR RAO AND K.P. RAVINDRAN Depamen of Mechanical Engineeing, Calicu Regional Engineeing College, Keala-67 6, INDIA. Absac:- We eploe
More informationLOGARITHMIC ORDER AND TYPE OF INDETERMINATE MOMENT PROBLEMS
LOGARITHMIC ORDER AND TYPE OF INDETERMINATE MOMENT PROBLEMS CHRISTIAN BERG AND HENRIK L. PEDERSEN WITH AN APPENDIX BY WALTER HAYMAN We invesigae a efined gowh scale, logaihmic gowh, fo indeeminae momen
More informationStability and Bifurcation in a Neural Network Model with Two Delays
Inernaional Mahemaical Forum, Vol. 6, 11, no. 35, 175-1731 Sabiliy and Bifurcaion in a Neural Nework Model wih Two Delays GuangPing Hu and XiaoLing Li School of Mahemaics and Physics, Nanjing Universiy
More informationThe Production of Polarization
Physics 36: Waves Lecue 13 3/31/211 The Poducion of Polaizaion Today we will alk abou he poducion of polaized ligh. We aleady inoduced he concep of he polaizaion of ligh, a ansvese EM wave. To biefly eview
More informationarxiv: v2 [math.pr] 19 Feb 2016
Global Diichle Hea Kenel Esimaes fo Symmeic Lévy Pocesses in Half-space Zhen-Qing Chen and Panki Kim axiv:54.4673v2 [mah.pr] 9 Feb 26 Mach 5, 28 Absac In his pape, we deive explici shap wo-sided esimaes
More informationNew sufficient conditions of robust recovery for low-rank matrices
New sufficien condiions of ous ecovey fo low-an maices Jianwen Huang a, Jianjun Wang a,, Feng Zhang a, Wendong Wang a a School of Mahemaics and Saisics, Souhwes Univesiy, Chongqing, 400715, China Reseach
More informationOn Carlsson type orthogonality and characterization of inner product spaces
Filoma 26:4 (212), 859 87 DOI 1.2298/FIL124859K Published by Faculy of Sciences and Mahemaics, Universiy of Niš, Serbia Available a: hp://www.pmf.ni.ac.rs/filoma On Carlsson ype orhogonaliy and characerizaion
More informationKOEBE DOMAINS FOR THE CLASSES OF FUNCTIONS WITH RANGES INCLUDED IN GIVEN SETS
Jounal of Applied Analysis Vol. 14, No. 1 2008), pp. 43 52 KOEBE DOMAINS FOR THE CLASSES OF FUNCTIONS WITH RANGES INCLUDED IN GIVEN SETS L. KOCZAN and P. ZAPRAWA Received Mach 12, 2007 and, in evised fom,
More informationA Necessary and Sufficient Condition for the Solutions of a Functional Differential Equation to Be Oscillatory or Tend to Zero
JOURNAL OF MAEMAICAL ANALYSIS AND APPLICAIONS 24, 7887 1997 ARICLE NO. AY965143 A Necessary and Sufficien Condiion for he Soluions of a Funcional Differenial Equaion o Be Oscillaory or end o Zero Piambar
More informationInternational Journal of Pure and Applied Sciences and Technology
In. J. Pue Appl. Sci. Technol., 4 (211, pp. 23-29 Inenaional Jounal of Pue and Applied Sciences and Technology ISS 2229-617 Available online a www.ijopaasa.in eseach Pape Opizaion of he Uiliy of a Sucual
More informationElastic-Plastic Deformation of a Rotating Solid Disk of Exponentially Varying Thickness and Exponentially Varying Density
Poceedings of he Inenaional MuliConfeence of Enginees Compue Scieniss 6 Vol II, IMECS 6, Mach 6-8, 6, Hong Kong Elasic-Plasic Defomaion of a Roaing Solid Dis of Exponenially Vaying hicness Exponenially
More informationÖRNEK 1: THE LINEAR IMPULSE-MOMENTUM RELATION Calculate the linear momentum of a particle of mass m=10 kg which has a. kg m s
MÜHENDİSLİK MEKANİĞİ. HAFTA İMPULS- MMENTUM-ÇARPIŞMA Linea oenu of a paicle: The sybol L denoes he linea oenu and is defined as he ass ies he elociy of a paicle. L ÖRNEK : THE LINEAR IMPULSE-MMENTUM RELATIN
More informationSolutions from Chapter 9.1 and 9.2
Soluions from Chaper 9 and 92 Secion 9 Problem # This basically boils down o an exercise in he chain rule from calculus We are looking for soluions of he form: u( x) = f( k x c) where k x R 3 and k is
More informationEXISTENCE OF NON-OSCILLATORY SOLUTIONS TO FIRST-ORDER NEUTRAL DIFFERENTIAL EQUATIONS
Elecronic Journal of Differenial Equaions, Vol. 206 (206, No. 39, pp.. ISSN: 072-669. URL: hp://ejde.mah.xsae.edu or hp://ejde.mah.un.edu fp ejde.mah.xsae.edu EXISTENCE OF NON-OSCILLATORY SOLUTIONS TO
More informationCourse Notes for EE227C (Spring 2018): Convex Optimization and Approximation
Course Noes for EE7C Spring 018: Convex Opimizaion and Approximaion Insrucor: Moriz Hard Email: hard+ee7c@berkeley.edu Graduae Insrucor: Max Simchowiz Email: msimchow+ee7c@berkeley.edu Ocober 15, 018 3
More informationOmega-limit sets and bounded solutions
arxiv:3.369v [mah.gm] 3 May 6 Omega-limi ses and bounded soluions Dang Vu Giang Hanoi Insiue of Mahemaics Vienam Academy of Science and Technology 8 Hoang Quoc Vie, 37 Hanoi, Vienam e-mail: dangvugiang@yahoo.com
More informationSections 3.1 and 3.4 Exponential Functions (Growth and Decay)
Secions 3.1 and 3.4 Eponenial Funcions (Gowh and Decay) Chape 3. Secions 1 and 4 Page 1 of 5 Wha Would You Rahe Have... $1million, o double you money evey day fo 31 days saing wih 1cen? Day Cens Day Cens
More informationPositive continuous solution of a quadratic integral equation of fractional orders
Mah. Sci. Le., No., 9-7 (3) 9 Mahemaical Sciences Leers An Inernaional Journal @ 3 NSP Naural Sciences Publishing Cor. Posiive coninuous soluion of a quadraic inegral equaion of fracional orders A. M.
More informationEN221 - Fall HW # 7 Solutions
EN221 - Fall2008 - HW # 7 Soluions Pof. Vivek Shenoy 1.) Show ha he fomulae φ v ( φ + φ L)v (1) u v ( u + u L)v (2) can be pu ino he alenaive foms φ φ v v + φv na (3) u u v v + u(v n)a (4) (a) Using v
More informationAn Introduction to Malliavin calculus and its applications
An Inroducion o Malliavin calculus and is applicaions Lecure 5: Smoohness of he densiy and Hörmander s heorem David Nualar Deparmen of Mahemaics Kansas Universiy Universiy of Wyoming Summer School 214
More informationMonotonic Solutions of a Class of Quadratic Singular Integral Equations of Volterra type
In. J. Conemp. Mah. Sci., Vol. 2, 27, no. 2, 89-2 Monoonic Soluions of a Class of Quadraic Singular Inegral Equaions of Volerra ype Mahmoud M. El Borai Deparmen of Mahemaics, Faculy of Science, Alexandria
More informationTwo Coupled Oscillators / Normal Modes
Lecure 3 Phys 3750 Two Coupled Oscillaors / Normal Modes Overview and Moivaion: Today we ake a small, bu significan, sep owards wave moion. We will no ye observe waves, bu his sep is imporan in is own
More informationStress Analysis of Infinite Plate with Elliptical Hole
Sess Analysis of Infinie Plae ih Ellipical Hole Mohansing R Padeshi*, D. P. K. Shaa* * ( P.G.Suden, Depaen of Mechanical Engg, NRI s Insiue of Infoaion Science & Technology, Bhopal, India) * ( Head of,
More information338 Jin Suk Pak and Yang Jae Shin 2. Preliminaries Let M be a( + )-dimensional almost contact metric manifold with an almost contact metric structure
Comm. Korean Math. Soc. 3(998), No. 2, pp. 337-343 A NOTE ON CONTACT CONFORMAL CURVATURE TENSOR Jin Suk Pak* and Yang Jae Shin Abstract. In this paper we show that every contact metric manifold with vanishing
More informationOn the probabilistic stability of the monomial functional equation
Available online a www.jnsa.com J. Nonlinear Sci. Appl. 6 (013), 51 59 Research Aricle On he probabilisic sabiliy of he monomial funcional equaion Claudia Zaharia Wes Universiy of Timişoara, Deparmen of
More informationVanishing Viscosity Method. There are another instructive and perhaps more natural discontinuous solutions of the conservation law
Vanishing Viscosiy Mehod. There are anoher insrucive and perhaps more naural disconinuous soluions of he conservaion law (1 u +(q(u x 0, he so called vanishing viscosiy mehod. This mehod consiss in viewing
More information