The Projective Quarter Symmetric Metric Connections and Their Curvature Tensors

Size: px
Start display at page:

Download "The Projective Quarter Symmetric Metric Connections and Their Curvature Tensors"

Transcription

1 Interntion Mtemtic Forum, 4, 009, no. 48, e Projective Qurter Symmetric Metric Connections nd eir Curvture ensors Hüy BAGDALI YILMAZ e University of Mrmr, Fcuty of Sciences nd Letters Deprtment of Mtemtics, Istnbu urkey bgdti@mrmr.edu.tr Aynur UYSAL e University of Dogus, Fcuty of Sciences nd Letters Deprtment of Mtemtics, Istnbu urkey uys@dogus.edu.tr Abstrct In tis pper, te existence of te projective qurter symmetric metric connection is proved in Riemnnin mnifods. In prticur two cses, tis connection reduces to semi-symmetric metric connection nd to projective semi-symmetric connection. Furtermore, we study scr curvture of Riemnnin mnifods wit keeping te covrint derivtive of tensor W j. Mtemtics Subject Cssifiction: 53A07, 53B5 Keywords:Projective qurter symmetric metric connection, e projective curvture tensor, -form Introduction In 970, Yno ], studied Riemnnin mnifods dmitting semi-symmetric metric connections wose curvture tensors vnis. In 980, Misr nd Prdey 6], studied qurter symmetric metric connections in Riemnnin, Keerin nd Sskin mnifods nd found some properties of curvture tensors of tem. In 98, Yno nd Imi 3], gve te most gener form of qurter symmetric metric connections nd studied its ppictions. In 008, Zo 5], investigted te properties of projective semi-symmetric metric connections of Riemnnin mnifod nd gve some interesting resuts wit respect to tis semi -symmetric connection.

2 370 H. BAGDALI YILMAZ nd A. UYSAL In te present pper, we define te projective qurter symmetric metric connections nd we so find formu for scr curvture of Riemnnin mnifods wit keeping te covrint derivtive of tensor W j. Projective Qurter Symmetric Metric Connection Let M be n-dimension Riemnnin mnifod of css C wit metric tensor g, nd be Levi- Cevit connection ssocited wit g. en, te condition Xk gx i, X j )= g ij x { } k gj { } jk gi = 0.) ods. A iner connection on M wose torsion tensor X, Y )= X Y Y X X, Y ] X, Y χm) wic is given by X, Y )=πy )tx) πx)ty ).) were π nd t re -form nd tensor of type, ), respectivey, is sid qurter symmetric connection, 6]. Aso, iner connection stisfying.) nd te condition X g ) Y,Z) = 0 were X, Y, Z χm), is ced qurter symmetric metric connection 6]. Here, χm) denote te set of differentibe vector fieds on M. If te geodesics wit respect to re wys consistent wit tose of, ten is sid projective equivent connection wit,5]. Definition If is bot te projective equivent connection wit nd te qurter symmetric metric connection, ten is ced te projective qurter symmetric metric connection. eorem Let be iner connection on M. is te projective qurter symmetric metric connection if nd ony if te coefficients Γ of te connection stisfy Γ = { } + + P.3) ) were = π k t i π i t k nd P = k δi + iδ k.

3 Projective qurter symmetric metric connections 37 Proof. Let be Xk gx i, X j )= g ij x k Γ g j Γ jk g i = 0.4) Subtrcting.4) from.), we ve Γ { }) gj + Γ jk { jk }) gi = 0.5) Now, we define tensor θ by θx, Y )= X Y X Y, X, Y χm). us, we cn write.5) in te foowing form θ g j + θ jk g i = 0.6) were te tensor θ is in te form θ =Γ { }.7) Hence, te torsion tensor ij wit te id of.6), we get cn be written s ij = θ ij θ ji.8) + θ ki) gj + jk + θ kj) gi =0 If te indices i, j, k) in.6) re cnged cycicy nd tis eqution for ec oter order is rewrote, te foowing equtions re obtined: θg j + θjkg i = 0 θji g k + θki g j = 0 θkj g i + θij g k = 0 Let us dd first two equtions nd subtrct te st eqution.us, we get ) θ + θki gj + θjk ) θ kj gi + θji ) θ ij gk =0.9) Using.8), we ve θ + θ ki ) gj + jkg i + jig k = 0.0) Since θ + θ ki =θ + ki.)

4 37 H. BAGDALI YILMAZ nd A. UYSAL e eqution.0) cn be written s θ + ki ) gj + jk g i + ji g k = 0.) If we mutipy te bove eqution by g j, we obtin θ = ki + jkg i g j + jig k g j).3) As sid before, is te projective equivent to if nd ony if te symmetric prt θ cn be written s θx, Y )+θy,x) =ΨY )X +ΨX)Y were Ψ is -form. erefore, we find X, Y χm) Contrcting for nd j in.3), we get θ + θ ki = jkg i g j + jig k g j) θ = ki + kδ i + iδk) Since te connection is projective qurter symmetric metric connection, by.), te torsion tensor is = π kt i π it k, were π is -form nd t is tensor of type, ). Hence, if we denote tensor k δi + ) i δ k by P, ten te projective qurter symmetric metric connection is given s foows wen.7) is used, Γ = { } + + P is competes te proof of eorem. Now, et us investigte some prticur cses for te connection.3).. In prticury, if P = 0 nd tensor of type, ) t i in = π kt i π it k is coiced t i = δi, ten te connection.3) is reduced to te semi -symmetric metric connection.t is to sy, Γ = { } + πk δi π iδk) tking φ k = π k nd using φ i = g im φ m. Hence,we ve, ], Γ = { } + φk δ i g φ.4)

5 Projective qurter symmetric metric connections 373. If P 0 nd we coice t i = δ i in te projective qurter symmetric metric connection, ten te connection.3) is reduced to projective semi -symmetric connection. = π kt i π it k = = π kδi π iδk.5) nd since P = k δi + i k) δ P n) = π i δk using ψ i = n) π i in.6), we get, 5] n) + π k δi.6) Γ = { } + πk δ i π i δ k + ψ i δ k + ψ k δ i.7) 3 e Riemnnin Mnifods wit Keeping te Covrint Derivtive of ensor W j We denote by R j R j = Γ x j Γ ij x k +Γ Γ j Γ ij Γ k te curvture tensor of te connection, 4]. We compute te curvture tensor using.3), we find R j = R j + k ij j + kp ij jp + 4 ] ij k j + P ij Pk PP j ] + ] ij Pk P j 3.) were Rj re te curvture tensor corresponding to. It is esiy sown tt 3.) stisfies te foowing properties: i) R mj = R mijk ii) R mk = 0 Contrcting 3.) wit respect to index nd j, we find : 3.)

6 374 H. BAGDALI YILMAZ nd A. UYSAL R = R + k j ij j j + kp j ij j P j + 4 ij j k j ] j + P ij P j k P P j j ] + ij P j k P j ] j 3.3) were R nd R re te Ricci tensor corresponding to nd, respectivey. Using 3.) nd 3.3) in te formu of te projective curvture tensor wit repect to wic is given by te formu ], we ve W j = R j R δj n R ijδk) 3.4) W j = Rj + kij j + kpij jp ij k ] j + P ij Pk P P ] j n n ) 4n ) n ) n ) ij Pk P ] j R δj R ijδk) k i n ) + ji ] ij k Pi P + jpi ] Pij i k ij + i ] j P i P k P P P ijp + P ip j ] i Pk P ijp + ip j ] 3.5) Furtermore, it cn be esiy obtined tt te projective curvture tensor 3.5) stisfies te foowing property W k = ) R R n ) Let us denote te covrint derivtive of nd by nd, respectivey. Using.3) one cn obtin:

7 Projective qurter symmetric metric connections 375 W j m = W j x m +Γ rm W r j Γr im W rkj Γr km W irj Γr jm W r ] ] = W j,m + W r j rm + P rm W rkj im r + P im r ] ] W irj km r + Pkm r W r jm r + Pjm r us, we ve were W j m = W j,m + W jm 3.6) ] ] ] ] W jm W r j rm + P rm W rkj im r + P im r W irj km r + P km r W r jm r + P jm r 3.7) us, we ve : eorem W j m = W j,m if nd ony if W jm =0. eorem 3 Let M be mnifod dmitting te connection.4). If W j m = W j,m, tere exists te foowing formu for -form π π i kj π i jk = ] R π j + n ) n +) nr n 4) kj R jk )π i + n +) R ijπ k Proof. From eorem 3 nd 3.7), we write W r j ] ] ] ] rm + Prm W rkj im r + Pim r W irj km r + Pkm r W r jm r + Pjm r =0 3.8) Moreover, substituting t i = δi in.), we obtin = π kδ i π iδ k 3.9) After contrcting 3.8) wit respect to index nd m, substituting 3.9) in 3.8), nd since P = 0, we obtin te foowing eqution n +)W m jπ m + W m mkjπ i + W m imjπ k + W m mπ j = 0 3.0)

8 376 H. BAGDALI YILMAZ nd A. UYSAL Wit te ep of 3.4), 3.0) cn be written in te form R m jπ m = n ) R ] π j + nrkj R jk )π i +n 4)R ij π k n + )n ) Since R m j π m = π i kj π i jk, we get π i kj π i jk = n ) R π j + 3.) { } ] nrkj R jk )π i +n 4)R ij π k 3.) n +) Concusion 3. Let M be mnifod dmitting te connection.4).ifw j m = W j,m nd π i kj = π i jk, ten scr curvture R of M is te foowing form R = nrkj R n +)π jk )π k π j +n 4)R ij π i π j] eorem 4 Let M be mnifod dmitting te connection.7). If W j m = W j,m, tere exists te foowing formu for -form π { } ] π i kj π i jk = R π j + nnrkj R n ) n jk )π i +n 4)R ij π k n + 4)n ) Proof. e proof is s bove te proof. Concusion 3. Let M be mnifod dmitting te connection.7).ifw j m = W j,m nd π i kj = π i jk, ten scr curvture R of M is te foowing form References R = nnrkj R n n +4)π jk )π k π j +n 4)R ij π i π j] ] K. Yno, On Semi-Symetric Metric Connection, Rev., Roum., Mt., Pureset App., 5 970), ] K. Yno, Some Remrks On ensor Fied nd Curvture, Anns of Mtemtics No:, Vo. 5595), ] K. Yno nd. Imi, Qurter Symmetric Metric Connections nd eir Curvture ensors, ensor N.S., Vo. 3898). 4] N. J. Hicks, Notes on Differenti Geometry,Princeton, H.J., Vn Nostrnd965). 5] P. Zo, Some Properties of Projective Semi-Symmetric Connections, Interntion Mtemtic Forum, 3, No: 7, 008), ] R.S. Misr nd S. N. Prdey, On Qurter Symmetric Metric F-Connection, ensor N.S., Vo ) Received: My, 009

Math 124B January 24, 2012

Math 124B January 24, 2012 Mth 24B Jnury 24, 22 Viktor Grigoryn 5 Convergence of Fourier series Strting from the method of seprtion of vribes for the homogeneous Dirichet nd Neumnn boundry vue probems, we studied the eigenvue probem

More information

Math 20C Multivariable Calculus Lecture 5 1. Lines and planes. Equations of lines (Vector, parametric, and symmetric eqs.). Equations of lines

Math 20C Multivariable Calculus Lecture 5 1. Lines and planes. Equations of lines (Vector, parametric, and symmetric eqs.). Equations of lines Mt 2C Multivrible Clculus Lecture 5 1 Lines nd plnes Slide 1 Equtions of lines (Vector, prmetric, nd symmetric eqs.). Equtions of plnes. Distnce from point to plne. Equtions of lines Slide 2 Definition

More information

Fundamental Theorem of Calculus

Fundamental Theorem of Calculus Funmentl Teorem of Clculus Liming Png 1 Sttement of te Teorem Te funmentl Teorem of Clculus is one of te most importnt teorems in te istory of mtemtics, wic ws first iscovere by Newton n Leibniz inepenently.

More information

University of Houston, Department of Mathematics Numerical Analysis II

University of Houston, Department of Mathematics Numerical Analysis II University of Houston, Deprtment of Mtemtics Numericl Anlysis II 6 Glerkin metod, finite differences nd colloction 6.1 Glerkin metod Consider sclr 2nd order ordinry differentil eqution in selfdjoint form

More information

Lecture Note 4: Numerical differentiation and integration. Xiaoqun Zhang Shanghai Jiao Tong University

Lecture Note 4: Numerical differentiation and integration. Xiaoqun Zhang Shanghai Jiao Tong University Lecture Note 4: Numericl differentition nd integrtion Xioqun Zng Sngi Jio Tong University Lst updted: November, 0 Numericl Anlysis. Numericl differentition.. Introduction Find n pproximtion of f (x 0 ),

More information

We name Functions f (x) or g(x) etc.

We name Functions f (x) or g(x) etc. Section 2 1B: Function Notation Bot of te equations y 2x +1 and y 3x 2 are functions. It is common to ave two or more functions in terms of x in te same problem. If I ask you wat is te value for y if x

More information

1 Introduction. FILOMAT (Niš) 16 (2002), GEODESIC MAPPINGS BETWEEN KÄHLERIAN SPACES. Josef Mikeš, Olga Pokorná 1 and Galina Starko

1 Introduction. FILOMAT (Niš) 16 (2002), GEODESIC MAPPINGS BETWEEN KÄHLERIAN SPACES. Josef Mikeš, Olga Pokorná 1 and Galina Starko FILOMAT (Niš) 16 (2002), 43 50 GEODESIC MAPPINGS BETWEEN KÄHLERIAN SPACES Josef Mikeš, Olga Pokorná 1 and Galina Starko Abstract Geodesic mappings from a Kälerian space K n onto a Kälerian space K n will

More information

12 Basic Integration in R

12 Basic Integration in R 14.102, Mt for Economists Fll 2004 Lecture Notes, 10/14/2004 Tese notes re primrily bsed on tose written by Andrei Bremzen for 14.102 in 2002/3, nd by Mrek Pyci for te MIT Mt Cmp in 2003/4. I ve mde only

More information

Suggested Solution to Assignment 5

Suggested Solution to Assignment 5 MATH 4 (5-6) prti diferenti equtions Suggested Soution to Assignment 5 Exercise 5.. () (b) A m = A m = = ( )m+ mπ x sin mπx dx = x mπ cos mπx + + 4( )m 4 m π. 4x cos mπx dx mπ x cos mπxdx = x mπ sin mπx

More information

Symmetry Labeling of Molecular Energies

Symmetry Labeling of Molecular Energies Capter 7. Symmetry Labeling of Molecular Energies Notes: Most of te material presented in tis capter is taken from Bunker and Jensen 1998, Cap. 6, and Bunker and Jensen 2005, Cap. 7. 7.1 Hamiltonian Symmetry

More information

OSCILLATION OF SOLUTIONS TO NON-LINEAR DIFFERENCE EQUATIONS WITH SEVERAL ADVANCED ARGUMENTS. Sandra Pinelas and Julio G. Dix

OSCILLATION OF SOLUTIONS TO NON-LINEAR DIFFERENCE EQUATIONS WITH SEVERAL ADVANCED ARGUMENTS. Sandra Pinelas and Julio G. Dix Opuscula Mat. 37, no. 6 (2017), 887 898 ttp://dx.doi.org/10.7494/opmat.2017.37.6.887 Opuscula Matematica OSCILLATION OF SOLUTIONS TO NON-LINEAR DIFFERENCE EQUATIONS WITH SEVERAL ADVANCED ARGUMENTS Sandra

More information

1 + t5 dt with respect to x. du = 2. dg du = f(u). du dx. dg dx = dg. du du. dg du. dx = 4x3. - page 1 -

1 + t5 dt with respect to x. du = 2. dg du = f(u). du dx. dg dx = dg. du du. dg du. dx = 4x3. - page 1 - Eercise. Find te derivative of g( 3 + t5 dt wit respect to. Solution: Te integrand is f(t + t 5. By FTC, f( + 5. Eercise. Find te derivative of e t2 dt wit respect to. Solution: Te integrand is f(t e t2.

More information

Section 2.1 The Definition of the Derivative. We are interested in finding the slope of the tangent line at a specific point.

Section 2.1 The Definition of the Derivative. We are interested in finding the slope of the tangent line at a specific point. Popper 6: Review of skills: Find tis difference quotient. f ( x ) f ( x) if f ( x) x Answer coices given in audio on te video. Section.1 Te Definition of te Derivative We are interested in finding te slope

More information

1. The vibrating string problem revisited.

1. The vibrating string problem revisited. Weeks 7 8: S eprtion of Vribes In the pst few weeks we hve expored the possibiity of soving first nd second order PDEs by trnsforming them into simper forms ( method of chrcteristics. Unfortuntey, this

More information

Math 1241 Calculus Test 1

Math 1241 Calculus Test 1 February 4, 2004 Name Te first nine problems count 6 points eac and te final seven count as marked. Tere are 120 points available on tis test. Multiple coice section. Circle te correct coice(s). You do

More information

Math Week 5 concepts and homework, due Friday February 10

Math Week 5 concepts and homework, due Friday February 10 Mt 2280-00 Week 5 concepts nd omework, due Fridy Februry 0 Recll tt ll problems re good for seeing if you cn work wit te underlying concepts; tt te underlined problems re to be nded in; nd tt te Fridy

More information

RGMIA Research Report Collection, Vol. 1, No. 1, SOME OSTROWSKI TYPE INEQUALITIES FOR N-TIME DIFFERENTIA

RGMIA Research Report Collection, Vol. 1, No. 1, SOME OSTROWSKI TYPE INEQUALITIES FOR N-TIME DIFFERENTIA ttp//sci.vut.edu.u/rgmi/reports.tml SOME OSTROWSKI TYPE INEQUALITIES FOR N-TIME DIFFERENTIABLE MAPPINGS AND APPLICATIONS P. CERONE, S.S. DRAGOMIR AND J. ROUMELIOTIS Astrct. Some generliztions of te Ostrowski

More information

A note on proper curvature collineations in Bianchi types VI

A note on proper curvature collineations in Bianchi types VI note on roer curvture collinetions in inci tyes VI nd VII sce-times Gulm Sbbir nd mjd li Fculty o Engineering Sciences GIK Institute o Engineering Sciences nd Tecnology Toi Swbi NWFP Pkistn Emil: sbbir@gikieduk

More information

64 IX. The Exceptional Lie Algebras

64 IX. The Exceptional Lie Algebras 64 IX. Te Exceptional Lie Algebras IX. Te Exceptional Lie Algebras We ave displayed te four series of classical Lie algebras and teir Dynkin diagrams. How many more simple Lie algebras are tere? Surprisingly,

More information

Mathematics 5 Worksheet 11 Geometry, Tangency, and the Derivative

Mathematics 5 Worksheet 11 Geometry, Tangency, and the Derivative Matematics 5 Workseet 11 Geometry, Tangency, and te Derivative Problem 1. Find te equation of a line wit slope m tat intersects te point (3, 9). Solution. Te equation for a line passing troug a point (x

More information

More on generalized inverses of partitioned matrices with Banachiewicz-Schur forms

More on generalized inverses of partitioned matrices with Banachiewicz-Schur forms More on generalized inverses of partitioned matrices wit anaciewicz-scur forms Yongge Tian a,, Yosio Takane b a Cina Economics and Management cademy, Central University of Finance and Economics, eijing,

More information

Solutions of Klein - Gordan equations, using Finite Fourier Sine Transform

Solutions of Klein - Gordan equations, using Finite Fourier Sine Transform IOSR Journl of Mthemtics (IOSR-JM) e-issn: 2278-5728, p-issn: 2319-765X. Volume 13, Issue 6 Ver. IV (Nov. - Dec. 2017), PP 19-24 www.iosrjournls.org Solutions of Klein - Gordn equtions, using Finite Fourier

More information

Math 212-Lecture 9. For a single-variable function z = f(x), the derivative is f (x) = lim h 0

Math 212-Lecture 9. For a single-variable function z = f(x), the derivative is f (x) = lim h 0 3.4: Partial Derivatives Definition Mat 22-Lecture 9 For a single-variable function z = f(x), te derivative is f (x) = lim 0 f(x+) f(x). For a function z = f(x, y) of two variables, to define te derivatives,

More information

5.1 We will begin this section with the definition of a rational expression. We

5.1 We will begin this section with the definition of a rational expression. We Basic Properties and Reducing to Lowest Terms 5.1 We will begin tis section wit te definition of a rational epression. We will ten state te two basic properties associated wit rational epressions and go

More information

Chapter 2. Numerical Integration also called quadrature. 2.2 Trapezoidal Rule. 2.1 A basic principle Extending the Trapezoidal Rule DRAWINGS

Chapter 2. Numerical Integration also called quadrature. 2.2 Trapezoidal Rule. 2.1 A basic principle Extending the Trapezoidal Rule DRAWINGS S Cpter Numericl Integrtion lso clled qudrture Te gol of numericl integrtion is to pproximte numericlly. f(x)dx Tis is useful for difficult integrls like sin(x) ; sin(x ); x + x 4 Or worse still for multiple-dimensionl

More information

Jet geometrical extension of the KCC-invariants arxiv: v3 [math.dg] 1 Dec 2009

Jet geometrical extension of the KCC-invariants arxiv: v3 [math.dg] 1 Dec 2009 Jet geometrical extension of te KCC-invariants arxiv:0906.2903v3 [mat.dg] 1 Dec 2009 Vladimir Balan and Mircea Neagu June 2009; Last revised December 2009 (an added bibliograpical item) Abstract In tis

More information

Key words. Numerical quadrature, piecewise polynomial, convergence rate, trapezoidal rule, midpoint rule, Simpson s rule, spectral accuracy.

Key words. Numerical quadrature, piecewise polynomial, convergence rate, trapezoidal rule, midpoint rule, Simpson s rule, spectral accuracy. O SPECTRA ACCURACY OF QUADRATURE FORMUAE BASED O PIECEWISE POYOMIA ITERPOATIO A KURGAOV AD S TSYKOV Abstrct It is well-known tt te trpezoidl rule, wile being only second-order ccurte in generl, improves

More information

Online Appendix for Lerner Symmetry: A Modern Treatment

Online Appendix for Lerner Symmetry: A Modern Treatment Online Appendix or Lerner Symmetry: A Modern Treatment Arnaud Costinot MIT Iván Werning MIT May 2018 Abstract Tis Appendix provides te proos o Teorem 1, Teorem 2, and Proposition 1. 1 Perect Competition

More information

Parabolic PDEs: time approximation Implicit Euler

Parabolic PDEs: time approximation Implicit Euler Part IX, Capter 53 Parabolic PDEs: time approximation We are concerned in tis capter wit bot te time and te space approximation of te model problem (52.4). We adopt te metod of line introduced in 52.2.

More information

ON THE GEOMETRY OF TANGENT BUNDLE OF A (PSEUDO-) RIEMANNIAN MANIFOLD

ON THE GEOMETRY OF TANGENT BUNDLE OF A (PSEUDO-) RIEMANNIAN MANIFOLD ANALELE ŞTIINŢIFICE ALE UNIVERSITĂŢII AL.I.CUZA IAŞI Tomul XLIV, s.i.a, Matematică, 1998, f1 ON THE GEOMETRY OF TANGENT BUNDLE OF A (PSEUDO-) RIEMANNIAN MANIFOLD BY V. OPROIU and N. PAPAGHIUC 0. Introduction.

More information

1. Which one of the following expressions is not equal to all the others? 1 C. 1 D. 25x. 2. Simplify this expression as much as possible.

1. Which one of the following expressions is not equal to all the others? 1 C. 1 D. 25x. 2. Simplify this expression as much as possible. 004 Algebra Pretest answers and scoring Part A. Multiple coice questions. Directions: Circle te letter ( A, B, C, D, or E ) net to te correct answer. points eac, no partial credit. Wic one of te following

More information

GAUGE THEORY ON A SPACE-TIME WITH TORSION

GAUGE THEORY ON A SPACE-TIME WITH TORSION GAUGE THEORY ON A SPACE-TIME WITH TORSION C. D. OPRISAN, G. ZET Fculty of Physics, Al. I. Cuz University, Isi, Romni Deprtment of Physics, Gh. Aschi Technicl University, Isi 700050, Romni Received September

More information

Section 3.1: Derivatives of Polynomials and Exponential Functions

Section 3.1: Derivatives of Polynomials and Exponential Functions Section 3.1: Derivatives of Polynomials and Exponential Functions In previous sections we developed te concept of te derivative and derivative function. Te only issue wit our definition owever is tat it

More information

f a h f a h h lim lim

f a h f a h h lim lim Te Derivative Te derivative of a function f at a (denoted f a) is f a if tis it exists. An alternative way of defining f a is f a x a fa fa fx fa x a Note tat te tangent line to te grap of f at te point

More information

PHYS 4390: GENERAL RELATIVITY LECTURE 6: TENSOR CALCULUS

PHYS 4390: GENERAL RELATIVITY LECTURE 6: TENSOR CALCULUS PHYS 4390: GENERAL RELATIVITY LECTURE 6: TENSOR CALCULUS To strt on tensor clculus, we need to define differentition on mnifold.a good question to sk is if the prtil derivtive of tensor tensor on mnifold?

More information

ODE: Existence and Uniqueness of a Solution

ODE: Existence and Uniqueness of a Solution Mth 22 Fll 213 Jerry Kzdn ODE: Existence nd Uniqueness of Solution The Fundmentl Theorem of Clculus tells us how to solve the ordinry differentil eqution (ODE) du = f(t) dt with initil condition u() =

More information

Research Article A Note on Pseudo-Umbilical Submanifolds of Hessian Manifolds with Constant Hessian Sectional Curvature

Research Article A Note on Pseudo-Umbilical Submanifolds of Hessian Manifolds with Constant Hessian Sectional Curvature International Scolarly Researc Network ISRN Geometry Volume 011, Article ID 374584, 1 pages doi:10.540/011/374584 Researc Article A Note on Pseudo-Umbilical Submanifolds of Hessian Manifolds wit Constant

More information

Numerical Differentiation

Numerical Differentiation Numerical Differentiation Finite Difference Formulas for te first derivative (Using Taylor Expansion tecnique) (section 8.3.) Suppose tat f() = g() is a function of te variable, and tat as 0 te function

More information

A Computational Method for Solving Linear Volterra Integral Equations

A Computational Method for Solving Linear Volterra Integral Equations Applied Mthemticl Sciences, Vol. 6, 01, no. 17, 807-814 A Computtionl Method for Solving Liner Volterr Integrl Equtions Frshid Mirzee Deprtment of Mthemtics, Fculty of Science Mlyer University, Mlyer,

More information

2.11 That s So Derivative

2.11 That s So Derivative 2.11 Tat s So Derivative Introduction to Differential Calculus Just as one defines instantaneous velocity in terms of average velocity, we now define te instantaneous rate of cange of a function at a point

More information

1. Consider the trigonometric function f(t) whose graph is shown below. Write down a possible formula for f(t).

1. Consider the trigonometric function f(t) whose graph is shown below. Write down a possible formula for f(t). . Consider te trigonometric function f(t) wose grap is sown below. Write down a possible formula for f(t). Tis function appears to be an odd, periodic function tat as been sifted upwards, so we will use

More information

4 The dynamical FRW universe

4 The dynamical FRW universe 4 The dynmicl FRW universe 4.1 The Einstein equtions Einstein s equtions G µν = T µν (7) relte the expnsion rte (t) to energy distribution in the universe. On the left hnd side is the Einstein tensor which

More information

Patrice Cassagnard Université Montesquieu Bordeaux IV LAREefi. Abstract

Patrice Cassagnard Université Montesquieu Bordeaux IV LAREefi. Abstract A useful grpicl metod under Cournot competition Ptrice Cssgnrd Université Montesquieu Bordeux IV LAEefi Astrct Tis note proposes grpicl pproc useful in gme teor. Tis metod consists in representing incentives

More information

WHEN IS A FUNCTION NOT FLAT? 1. Introduction. {e 1 0, x = 0. f(x) =

WHEN IS A FUNCTION NOT FLAT? 1. Introduction. {e 1 0, x = 0. f(x) = WHEN IS A FUNCTION NOT FLAT? YIFEI PAN AND MEI WANG Abstrct. In this pper we prove unique continution property for vector vlued functions of one vrible stisfying certin differentil inequlity. Key words:

More information

NEW INTEGRAL INEQUALITIES OF THE TYPE OF SIMPSON S AND HERMITE-HADAMARD S FOR TWICE DIFFERENTIABLE QUASI-GEOMETRICALLY CONVEX MAPPINGS

NEW INTEGRAL INEQUALITIES OF THE TYPE OF SIMPSON S AND HERMITE-HADAMARD S FOR TWICE DIFFERENTIABLE QUASI-GEOMETRICALLY CONVEX MAPPINGS TJMM 8 6, No., 37-45 NEW INTEGRAL INEQUALITIES OF THE TYPE OF SIMPSON S AND HERMITE-HADAMARD S FOR TWICE DIFFERENTIABLE QUASI-GEOMETRICALLY CONVEX MAPPINGS MUHAMMAD MUDDASSAR AND ZAFFER ELAHI Astrct. In

More information

Derivatives. if such a limit exists. In this case when such a limit exists, we say that the function f is differentiable.

Derivatives. if such a limit exists. In this case when such a limit exists, we say that the function f is differentiable. Derivatives 3. Derivatives Definition 3. Let f be a function an a < b be numbers. Te average rate of cange of f from a to b is f(b) f(a). b a Remark 3. Te average rate of cange of a function f from a to

More information

1. On some properties of definite integrals. We prove

1. On some properties of definite integrals. We prove This short collection of notes is intended to complement the textbook Anlisi Mtemtic 2 by Crl Mdern, published by Città Studi Editore, [M]. We refer to [M] for nottion nd the logicl stremline of the rguments.

More information

Finite Difference Method

Finite Difference Method Capter 8 Finite Difference Metod 81 2nd order linear pde in two variables General 2nd order linear pde in two variables is given in te following form: L[u] = Au xx +2Bu xy +Cu yy +Du x +Eu y +Fu = G According

More information

Differentiation in higher dimensions

Differentiation in higher dimensions Capter 2 Differentiation in iger dimensions 2.1 Te Total Derivative Recall tat if f : R R is a 1-variable function, and a R, we say tat f is differentiable at x = a if and only if te ratio f(a+) f(a) tends

More information

Lecture XVII. Abstract We introduce the concept of directional derivative of a scalar function and discuss its relation with the gradient operator.

Lecture XVII. Abstract We introduce the concept of directional derivative of a scalar function and discuss its relation with the gradient operator. Lecture XVII Abstract We introduce te concept of directional derivative of a scalar function and discuss its relation wit te gradient operator. Directional derivative and gradient Te directional derivative

More information

DECOMPOSITION OF RECURRENT CURVATURE TENSOR FIELDS IN A KAEHLERIAN MANIFOLD OF FIRST ORDER. Manoj Singh Bisht 1 and U.S.Negi 2

DECOMPOSITION OF RECURRENT CURVATURE TENSOR FIELDS IN A KAEHLERIAN MANIFOLD OF FIRST ORDER. Manoj Singh Bisht 1 and U.S.Negi 2 DECOMPOSITION OF RECURRENT CURVATURE TENSOR FIELDS IN A KAEHLERIAN MANIFOLD OF FIRST ORDER Manoj Sing Bist 1 and U.S.Negi 2 1, 2 Department of Matematics, H.N.B. Garwal (A Central) University, SRT Campus

More information

GENERALIZED ANALYTICAL FUNCTIONS OF POLY NUMBER VARIABLE. G. I. Garas ko

GENERALIZED ANALYTICAL FUNCTIONS OF POLY NUMBER VARIABLE. G. I. Garas ko 7 Garas ko G. I. Generalized analytical functions of poly number variable GENERALIZED ANALYTICAL FUNCTIONS OF POLY NUMBER VARIABLE G. I. Garas ko Electrotechnical institute of Russia gri9z@mail.ru We introduce

More information

Joint Distribution of any Record Value and an Order Statistics

Joint Distribution of any Record Value and an Order Statistics Interntionl Mthemticl Forum, 4, 2009, no. 22, 09-03 Joint Distribution of ny Record Vlue nd n Order Sttistics Cihn Aksop Gzi University, Deprtment of Sttistics 06500 Teknikokullr, Ankr, Turkey entelpi@yhoo.com

More information

Polynomial Interpolation

Polynomial Interpolation Capter 4 Polynomial Interpolation In tis capter, we consider te important problem of approximatinga function fx, wose values at a set of distinct points x, x, x,, x n are known, by a polynomial P x suc

More information

Logarithms and Exponential Functions. Gerda de Vries & John S. Macnab. match as necessary, or to work these results into other lessons.

Logarithms and Exponential Functions. Gerda de Vries & John S. Macnab. match as necessary, or to work these results into other lessons. Logritms nd Eponentil Functions Gerd de Vries & Jon S. Mcn It is epected tt students re lred fmilir wit tis mteril. We include it ere for completeness. Te tree lessons given ere re ver sort. Te tecer is

More information

3.1 Extreme Values of a Function

3.1 Extreme Values of a Function .1 Etreme Values of a Function Section.1 Notes Page 1 One application of te derivative is finding minimum and maimum values off a grap. In precalculus we were only able to do tis wit quadratics by find

More information

Doubly Warped Products in Locally Conformal Almost Cosymplectic Manifolds

Doubly Warped Products in Locally Conformal Almost Cosymplectic Manifolds INTERNATIONAL ELECTRONIC JOURNAL OF GEOMETRY VOLUME 0 NO. 2 PAGE 73 8 207) Doubly Warped Products in Locally Conformal Almost Cosymplectic Manifolds Andreea Olteanu Communicated by Ion Miai) ABSTRACT Recently,

More information

Super-energy in general relativity ( ).

Super-energy in general relativity ( ). L super-énergie en retivité génére, Bu. Soc. Mth. Beg. 10 (1958), 11-147. Super-energy in gener retivity ( ). By ROBERT DEBEVER INTRODUCTION. If the probems of the definition of the energy of grvittion

More information

A Combinatorial Interpretation of the Generalized Fibonacci Numbers

A Combinatorial Interpretation of the Generalized Fibonacci Numbers ADVANCES IN APPLIED MATHEMATICS 19, 306318 1997 ARTICLE NO. AM970531 A Combinatorial Interpretation of te Generalized Fibonacci Numbers Emanuele Munarini Dipartimento di Matematica, Politecnico di Milano,

More information

Section 2. Basic formulas and identities in Riemannian geometry

Section 2. Basic formulas and identities in Riemannian geometry Section 2. Basic formulas and identities in Riemannian geometry Weimin Sheng and 1. Bianchi identities The first and second Bianchi identities are R ijkl + R iklj + R iljk = 0 R ijkl,m + R ijlm,k + R ijmk,l

More information

4.2 - Richardson Extrapolation

4.2 - Richardson Extrapolation . - Ricardson Extrapolation. Small-O Notation: Recall tat te big-o notation used to define te rate of convergence in Section.: Definition Let x n n converge to a number x. Suppose tat n n is a sequence

More information

Topic 6b Finite Difference Approximations

Topic 6b Finite Difference Approximations /8/8 Course Instructor Dr. Rymond C. Rump Oice: A 7 Pone: (95) 747 6958 E Mil: rcrump@utep.edu Topic 6b Finite Dierence Approximtions EE 486/5 Computtionl Metods in EE Outline Wt re inite dierence pproximtions?

More information

Some estimates on the Hermite-Hadamard inequality through quasi-convex functions

Some estimates on the Hermite-Hadamard inequality through quasi-convex functions Annls of University of Criov, Mth. Comp. Sci. Ser. Volume 3, 7, Pges 8 87 ISSN: 13-693 Some estimtes on the Hermite-Hdmrd inequlity through qusi-convex functions Dniel Alexndru Ion Abstrct. In this pper

More information

Effect of the Dependent Paths in Linear Hull

Effect of the Dependent Paths in Linear Hull 1 Effect of te Dependent Pats in Linear Hull Zenli Dai, Meiqin Wang, Yue Sun Scool of Matematics, Sandong University, Jinan, 250100, Cina Key Laboratory of Cryptologic Tecnology and Information Security,

More information

Sample Problems for Third Midterm March 18, 2013

Sample Problems for Third Midterm March 18, 2013 Mat 30. Treibergs Sampe Probems for Tird Midterm Name: Marc 8, 03 Questions 4 appeared in my Fa 000 and Fa 00 Mat 30 exams (.)Let f : R n R n be differentiabe at a R n. (a.) Let g : R n R be defined by

More information

University Mathematics 2

University Mathematics 2 University Matematics 2 1 Differentiability In tis section, we discuss te differentiability of functions. Definition 1.1 Differentiable function). Let f) be a function. We say tat f is differentiable at

More information

MATH 1A Midterm Practice September 29, 2014

MATH 1A Midterm Practice September 29, 2014 MATH A Midterm Practice September 9, 04 Name: Problem. (True/False) If a function f : R R is injective, ten f as an inverse. Solution: True. If f is injective, ten it as an inverse since tere does not

More information

The Recurrent Reimannian Spaces Having a Semi-symmetric Metric Connection and a Decomposable Curvature Tensor

The Recurrent Reimannian Spaces Having a Semi-symmetric Metric Connection and a Decomposable Curvature Tensor Int. J. Contemp. Math. Sciences, Vol. 2, 2007, no. 21, 1025-1029 The Recurrent Reimannian Spaces Having a Semi-symmetric Metric Connection and a Decomposable Curvature Tensor Hakan Demirbüker and Fatma

More information

Chapter 2 Differentiation

Chapter 2 Differentiation Cpter Differentition. Introduction In its initil stges differentition is lrgely mtter of finding limiting vlues, wen te vribles ( δ ) pproces zero, nd to begin tis cpter few emples will be tken. Emple..:

More information

1 The concept of limits (p.217 p.229, p.242 p.249, p.255 p.256) 1.1 Limits Consider the function determined by the formula 3. x since at this point

1 The concept of limits (p.217 p.229, p.242 p.249, p.255 p.256) 1.1 Limits Consider the function determined by the formula 3. x since at this point MA00 Capter 6 Calculus and Basic Linear Algebra I Limits, Continuity and Differentiability Te concept of its (p.7 p.9, p.4 p.49, p.55 p.56). Limits Consider te function determined by te formula f Note

More information

New Integral Inequalities through Generalized Convex Functions

New Integral Inequalities through Generalized Convex Functions Punjb University Journ of Mthetics ISSN 116-2526) Vo. 462)214) pp. 47-51 New Integr Inequities through Generized Convex Functions Muhd Muddssr, Deprtent of Mthetics, University of Engineering nd Technoogy,

More information

Definite integral. Mathematics FRDIS MENDELU

Definite integral. Mathematics FRDIS MENDELU Definite integrl Mthemtics FRDIS MENDELU Simon Fišnrová Brno 1 Motivtion - re under curve Suppose, for simplicity, tht y = f(x) is nonnegtive nd continuous function defined on [, b]. Wht is the re of the

More information

MTH-112 Quiz 1 Name: # :

MTH-112 Quiz 1 Name: # : MTH- Quiz Name: # : Please write our name in te provided space. Simplif our answers. Sow our work.. Determine weter te given relation is a function. Give te domain and range of te relation.. Does te equation

More information

Math 31A Discussion Notes Week 4 October 20 and October 22, 2015

Math 31A Discussion Notes Week 4 October 20 and October 22, 2015 Mat 3A Discussion Notes Week 4 October 20 and October 22, 205 To prepare for te first midterm, we ll spend tis week working eamples resembling te various problems you ve seen so far tis term. In tese notes

More information

Definite integral. Mathematics FRDIS MENDELU. Simona Fišnarová (Mendel University) Definite integral MENDELU 1 / 30

Definite integral. Mathematics FRDIS MENDELU. Simona Fišnarová (Mendel University) Definite integral MENDELU 1 / 30 Definite integrl Mthemtics FRDIS MENDELU Simon Fišnrová (Mendel University) Definite integrl MENDELU / Motivtion - re under curve Suppose, for simplicity, tht y = f(x) is nonnegtive nd continuous function

More information

Pre-lab Quiz/PHYS 224 Earth s Magnetic Field. Your name Lab section

Pre-lab Quiz/PHYS 224 Earth s Magnetic Field. Your name Lab section Pre-lab Quiz/PHYS 4 Eart s Magnetic Field Your name Lab section 1. Wat do you investigate in tis lab?. For a pair of Helmoltz coils described in tis manual and sown in Figure, r=.15 m, N=13, I =.4 A, wat

More information

Set Integral Equations in Metric Spaces

Set Integral Equations in Metric Spaces Mthemtic Morvic Vol. 13-1 2009, 95 102 Set Integrl Equtions in Metric Spces Ion Tişe Abstrct. Let P cp,cvr n be the fmily of ll nonempty compct, convex subsets of R n. We consider the following set integrl

More information

Dynamics and Relativity

Dynamics and Relativity Dynamics and Relativity Stepen Siklos Lent term 2011 Hand-outs and examples seets, wic I will give out in lectures, are available from my web site www.damtp.cam.ac.uk/user/stcs/dynamics.tml Lecture notes,

More information

4. The slope of the line 2x 7y = 8 is (a) 2/7 (b) 7/2 (c) 2 (d) 2/7 (e) None of these.

4. The slope of the line 2x 7y = 8 is (a) 2/7 (b) 7/2 (c) 2 (d) 2/7 (e) None of these. Mat 11. Test Form N Fall 016 Name. Instructions. Te first eleven problems are wort points eac. Te last six problems are wort 5 points eac. For te last six problems, you must use relevant metods of algebra

More information

INTRODUCTION TO LINEAR ALGEBRA

INTRODUCTION TO LINEAR ALGEBRA ME Applied Mthemtics for Mechnicl Engineers INTRODUCTION TO INEAR AGEBRA Mtrices nd Vectors Prof. Dr. Bülent E. Pltin Spring Sections & / ME Applied Mthemtics for Mechnicl Engineers INTRODUCTION TO INEAR

More information

MAT 145. Type of Calculator Used TI-89 Titanium 100 points Score 100 possible points

MAT 145. Type of Calculator Used TI-89 Titanium 100 points Score 100 possible points MAT 15 Test #2 Name Solution Guide Type of Calculator Used TI-89 Titanium 100 points Score 100 possible points Use te grap of a function sown ere as you respond to questions 1 to 8. 1. lim f (x) 0 2. lim

More information

Theory and implementation behind: Universal surface creation - smallest unitcell

Theory and implementation behind: Universal surface creation - smallest unitcell Teory and impementation beind: Universa surface creation - smaest unitce Bjare Brin Buus, Jaob Howat & Tomas Bigaard September 15, 218 1 Construction of surface sabs Te aim for tis part of te project is

More information

A SHORT INTRODUCTION TO BANACH LATTICES AND

A SHORT INTRODUCTION TO BANACH LATTICES AND CHAPTER A SHORT INTRODUCTION TO BANACH LATTICES AND POSITIVE OPERATORS In tis capter we give a brief introduction to Banac lattices and positive operators. Most results of tis capter can be found, e.g.,

More information

232 Calculus and Structures

232 Calculus and Structures 3 Calculus and Structures CHAPTER 17 JUSTIFICATION OF THE AREA AND SLOPE METHODS FOR EVALUATING BEAMS Calculus and Structures 33 Copyrigt Capter 17 JUSTIFICATION OF THE AREA AND SLOPE METHODS 17.1 THE

More information

MAGIC058 & MATH64062: Partial Differential Equations 1

MAGIC058 & MATH64062: Partial Differential Equations 1 MAGIC58 & MATH646: Prti Differenti Equtions 1 Section 4 Fourier series 4.1 Preiminry definitions Definition: Periodic function A function f( is sid to be periodic, with period p if, for, f( + p = f( where

More information

THE SECTIONAL CURVATURE OF THE TANGENT BUNDLES WITH GENERAL NATURAL LIFTED METRICS

THE SECTIONAL CURVATURE OF THE TANGENT BUNDLES WITH GENERAL NATURAL LIFTED METRICS Ninth International Conference on Geometry, Integrability and Quantization June 8 13, 2007, Varna, Bulgaria Ivaïlo M. Mladenov, Editor SOFTEX, Sofia 2008, pp 198 209 Geometry, Integrability and Quantization

More information

Quantum Mechanics Chapter 1.5: An illustration using measurements of particle spin.

Quantum Mechanics Chapter 1.5: An illustration using measurements of particle spin. I Introduction. Quantum Mecanics Capter.5: An illustration using measurements of particle spin. Quantum mecanics is a teory of pysics tat as been very successful in explaining and predicting many pysical

More information

Online Appendix. to Add-on Policies under Vertical Differentiation: Why Do Luxury Hotels Charge for Internet While Economy Hotels Do Not?

Online Appendix. to Add-on Policies under Vertical Differentiation: Why Do Luxury Hotels Charge for Internet While Economy Hotels Do Not? Onine Appendix to Add-on Poicies under Vertica Differentiation: Wy Do Luxury Hotes Carge for Internet Wie Economy Hotes Do Not? Song Lin Department of Marketing, Hong Kong University of Science and Tecnoogy

More information

The Form of Hanging Slinky

The Form of Hanging Slinky Bulletin of Aichi Univ. of Eduction, 66Nturl Sciences, pp. - 6, Mrch, 07 The Form of Hnging Slinky Kenzi ODANI Deprtment of Mthemtics Eduction, Aichi University of Eduction, Kriy 448-854, Jpn Introduction

More information

Superconvergence of energy-conserving discontinuous Galerkin methods for. linear hyperbolic equations. Abstract

Superconvergence of energy-conserving discontinuous Galerkin methods for. linear hyperbolic equations. Abstract Superconvergence of energy-conserving discontinuous Galerkin metods for linear yperbolic equations Yong Liu, Ci-Wang Su and Mengping Zang 3 Abstract In tis paper, we study superconvergence properties of

More information

PLANAR NORMAL SECTIONS OF FOCAL MANIFOLDS OF ISOPARAMETRIC HYPERSURFACES IN SPHERES

PLANAR NORMAL SECTIONS OF FOCAL MANIFOLDS OF ISOPARAMETRIC HYPERSURFACES IN SPHERES REVISTA DE LA UNIÓN MATEMÁTICA ARGENTINA Vol. 56, No. 2, 2015, Pges 119 133 Published online: September 30, 2015 PLANAR NORMAL SECTIONS OF FOCAL MANIFOLDS OF ISOPARAMETRIC HYPERSURFACES IN SPHERES Abstrct.

More information

INTRODUCTION AND MATHEMATICAL CONCEPTS

INTRODUCTION AND MATHEMATICAL CONCEPTS Capter 1 INTRODUCTION ND MTHEMTICL CONCEPTS PREVIEW Tis capter introduces you to te basic matematical tools for doing pysics. You will study units and converting between units, te trigonometric relationsips

More information

Solutions to Problems Integration in IR 2 and IR 3

Solutions to Problems Integration in IR 2 and IR 3 Solutions to Problems Integrtion in I nd I. For ec of te following, evlute te given double integrl witout using itertion. Insted, interpret te integrl s, for emple, n re or n verge vlue. ) dd were is te

More information

Zygmunt Wronicz ON SOME APPLICATION OF BIORTHOGONAL SPLINE SYSTEMS TO INTEGRAL EQUATIONS

Zygmunt Wronicz ON SOME APPLICATION OF BIORTHOGONAL SPLINE SYSTEMS TO INTEGRAL EQUATIONS Opuscul Mtemtic Vol. 5 o. 1 005 Zygmunt Wronicz O SOME APPLICATIO OF BIORTHOGOAL SPLIE SYSTEMS TO ITEGRAL EQUATIOS Abstrct. We consider n opertor P : L p(i S n(, suc tt P f = f for f S n(, were S n( is

More information

Calculus I Practice Exam 1A

Calculus I Practice Exam 1A Calculus I Practice Exam A Calculus I Practice Exam A Tis practice exam empasizes conceptual connections and understanding to a greater degree tan te exams tat are usually administered in introductory

More information

Well Centered Spherical Quadrangles

Well Centered Spherical Quadrangles Beiträge zur Algebr und Geometrie Contributions to Algebr nd Geometry Volume 44 (003), No, 539-549 Well Centered Sphericl Qudrngles An M d Azevedo Bred 1 Altino F Sntos Deprtment of Mthemtics, University

More information

1 (10) 2 (10) 3 (10) 4 (10) 5 (10) 6 (10) Total (60)

1 (10) 2 (10) 3 (10) 4 (10) 5 (10) 6 (10) Total (60) First Name: OSU Number: Last Name: Signature: OKLAHOMA STATE UNIVERSITY Department of Matematics MATH 2144 (Calculus I) Instructor: Dr. Matias Sculze MIDTERM 1 September 17, 2008 Duration: 50 minutes No

More information

AVL trees. AVL trees

AVL trees. AVL trees Dnamic set DT dnamic set DT is a structure tat stores a set of elements. Eac element as a (unique) ke and satellite data. Te structure supports te following operations. Searc(S, k) Return te element wose

More information

Chapter 3 Basic Crystallography and Electron Diffraction from Crystals. Lecture 9. CHEM 793, 2008 Fall

Chapter 3 Basic Crystallography and Electron Diffraction from Crystals. Lecture 9. CHEM 793, 2008 Fall Cpte 3 Bsic Cystopy nd Eecton Diffction fom Cysts Lectue 9 Top of tin foi Cyst pne () Bottom of tin foi B Lw d sinθ n Equtions connectin te Cyst metes (,, ) nd d-spcin wit bem pmetes () ( ) ne B Lw d (nm)

More information

called the homomorphism induced by the inductive limit. One verifies that the diagram

called the homomorphism induced by the inductive limit. One verifies that the diagram Inductive limits of C -algebras 51 sequences {a n } suc tat a n, and a n 0. If A = A i for all i I, ten A i = C b (I,A) and i I A i = C 0 (I,A). i I 1.10 Inductive limits of C -algebras Definition 1.10.1

More information