Sequences and Series of Functions, Convergence, Power Series
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Modes of Convergence in Probability Theory
Modes of Convergence in Probability Theory David Mandel November 5, 2015 Below, fix a probability space (Ω; F;P ) on which all random variables fXng and X are defined. All random variables are assumed to take values in R. Propositions marked with \F" denote results that rely on our finite measure space. That is, those marked results may not hold on a non-finite measure space. Since we already know uniform convergence =) pointwise convergence this proof is omitted, but we include a proof that shows pointwise convergence =) almost sure convergence, and hence uniform convergence =) almost sure convergence. The hierarchy we will show is diagrammed in Fig. 1, where some famous theorems that demonstrate the type of convergence are in parentheses: (SLLN) = strong long of large numbers, (WLLN) = weak law of large numbers, (CLT) ^ = central limit theorem. In parameter estimation, θn is said to be a consistent ^ estimator or θ if θn ! θ in probability. For example, by the SLLN, X¯n ! µ a.s., and hence X¯n ! µ in probability. Therefore the sample mean is a consistent estimator of the population mean. Figure 1: Hierarchy of modes of convergence in probability. 1 1 Definitions of Convergence 1.1 Modes from Calculus Definition Xn ! X pointwise if 8! 2 Ω, 8 > 0, 9N 2 N such that 8n ≥ N, jXn(!) − X(!)j < . Definition Xn ! X uniformly if 8 > 0, 9N 2 N such that 8! 2 Ω and 8n ≥ N, jXn(!) − X(!)j < . 1.2 Modes Unique to Measure Theory Definition Xn ! X in probability if 8 > 0, 8δ > 0, 9N 2 N such that 8n ≥ N, P (jXn − Xj ≥ ) < δ: Or, Xn ! X in probability if 8 > 0, lim P (jXn − Xj ≥ 0) = 0: n!1 The explicit epsilon-delta definition of convergence in probability is useful for proving a.s. -
Ch. 15 Power Series, Taylor Series
Ch. 15 Power Series, Taylor Series 서울대학교 조선해양공학과 서유택 2017.12 ※ 본 강의 자료는 이규열, 장범선, 노명일 교수님께서 만드신 자료를 바탕으로 일부 편집한 것입니다. Seoul National 1 Univ. 15.1 Sequences (수열), Series (급수), Convergence Tests (수렴판정) Sequences: Obtained by assigning to each positive integer n a number zn z . Term: zn z1, z 2, or z 1, z 2 , or briefly zn N . Real sequence (실수열): Sequence whose terms are real Convergence . Convergent sequence (수렴수열): Sequence that has a limit c limznn c or simply z c n . For every ε > 0, we can find N such that Convergent complex sequence |zn c | for all n N → all terms zn with n > N lie in the open disk of radius ε and center c. Divergent sequence (발산수열): Sequence that does not converge. Seoul National 2 Univ. 15.1 Sequences, Series, Convergence Tests Convergence . Convergent sequence: Sequence that has a limit c Ex. 1 Convergent and Divergent Sequences iin 11 Sequence i , , , , is convergent with limit 0. n 2 3 4 limznn c or simply z c n Sequence i n i , 1, i, 1, is divergent. n Sequence {zn} with zn = (1 + i ) is divergent. Seoul National 3 Univ. 15.1 Sequences, Series, Convergence Tests Theorem 1 Sequences of the Real and the Imaginary Parts . A sequence z1, z2, z3, … of complex numbers zn = xn + iyn converges to c = a + ib . if and only if the sequence of the real parts x1, x2, … converges to a . and the sequence of the imaginary parts y1, y2, … converges to b. Ex. -
Formal Power Series - Wikipedia, the Free Encyclopedia
Formal power series - Wikipedia, the free encyclopedia http://en.wikipedia.org/wiki/Formal_power_series Formal power series From Wikipedia, the free encyclopedia In mathematics, formal power series are a generalization of polynomials as formal objects, where the number of terms is allowed to be infinite; this implies giving up the possibility to substitute arbitrary values for indeterminates. This perspective contrasts with that of power series, whose variables designate numerical values, and which series therefore only have a definite value if convergence can be established. Formal power series are often used merely to represent the whole collection of their coefficients. In combinatorics, they provide representations of numerical sequences and of multisets, and for instance allow giving concise expressions for recursively defined sequences regardless of whether the recursion can be explicitly solved; this is known as the method of generating functions. Contents 1 Introduction 2 The ring of formal power series 2.1 Definition of the formal power series ring 2.1.1 Ring structure 2.1.2 Topological structure 2.1.3 Alternative topologies 2.2 Universal property 3 Operations on formal power series 3.1 Multiplying series 3.2 Power series raised to powers 3.3 Inverting series 3.4 Dividing series 3.5 Extracting coefficients 3.6 Composition of series 3.6.1 Example 3.7 Composition inverse 3.8 Formal differentiation of series 4 Properties 4.1 Algebraic properties of the formal power series ring 4.2 Topological properties of the formal power series -
7. Properties of Uniformly Convergent Sequences
46 1. THE THEORY OF CONVERGENCE 7. Properties of uniformly convergent sequences Here a relation between continuity, differentiability, and Riemann integrability of the sum of a functional series or the limit of a functional sequence and uniform convergence is studied. 7.1. Uniform convergence and continuity. Theorem 7.1. (Continuity of the sum of a series) N The sum of the series un(x) of terms continuous on D R is continuous if the series converges uniformly on D. ⊂ P Let Sn(x)= u1(x)+u2(x)+ +un(x) be a sequence of partial sum. It converges to some function S···(x) because every uniformly convergent series converges pointwise. Continuity of S at a point x means (by definition) lim S(y)= S(x) y→x Fix a number ε> 0. Then one can find a number δ such that S(x) S(y) <ε whenever 0 < x y <δ | − | | − | In other words, the values S(y) can get arbitrary close to S(x) and stay arbitrary close to it for all points y = x that are sufficiently close to x. Let us show that this condition follows6 from the hypotheses. Owing to the uniform convergence of the series, given ε > 0, one can find an integer m such that ε S(x) Sn(x) sup S Sn , x D, n m | − |≤ D | − |≤ 3 ∀ ∈ ∀ ≥ Note that m is independent of x. By continuity of Sn (as a finite sum of continuous functions), for n m, one can also find a number δ > 0 such that ≥ ε Sn(x) Sn(y) < whenever 0 < x y <δ | − | 3 | − | So, given ε> 0, the integer m is found. -
Arxiv:2102.05840V2 [Math.PR]
SEQUENTIAL CONVERGENCE ON THE SPACE OF BOREL MEASURES LIANGANG MA Abstract We study equivalent descriptions of the vague, weak, setwise and total- variation (TV) convergence of sequences of Borel measures on metrizable and non-metrizable topological spaces in this work. On metrizable spaces, we give some equivalent conditions on the vague convergence of sequences of measures following Kallenberg, and some equivalent conditions on the TV convergence of sequences of measures following Feinberg-Kasyanov-Zgurovsky. There is usually some hierarchy structure on the equivalent descriptions of convergence in different modes, but not always. On non-metrizable spaces, we give examples to show that these conditions are seldom enough to guarantee any convergence of sequences of measures. There are some remarks on the attainability of the TV distance and more modes of sequential convergence at the end of the work. 1. Introduction Let X be a topological space with its Borel σ-algebra B. Consider the collection M˜ (X) of all the Borel measures on (X, B). When we consider the regularity of some mapping f : M˜ (X) → Y with Y being a topological space, some topology or even metric is necessary on the space M˜ (X) of Borel measures. Various notions of topology and metric grow out of arXiv:2102.05840v2 [math.PR] 28 Apr 2021 different situations on the space M˜ (X) in due course to deal with the corresponding concerns of regularity. In those topology and metric endowed on M˜ (X), it has been recognized that the vague, weak, setwise topology as well as the total-variation (TV) metric are highlighted notions on the topological and metric description of M˜ (X) in various circumstances, refer to [Kal, GR, Wul]. -
Uniform Convergence and Differentiation Theorem 6.3.1
Math 341 Lecture #29 x6.3: Uniform Convergence and Differentiation We have seen that a pointwise converging sequence of continuous functions need not have a continuous limit function; we needed uniform convergence to get continuity of the limit function. What can we say about the differentiability of the limit function of a pointwise converging sequence of differentiable functions? 1+1=(2n−1) The sequence of differentiable hn(x) = x , x 2 [−1; 1], converges pointwise to the nondifferentiable h(x) = x; we will need to assume more about the pointwise converging sequence of differentiable functions to ensure that the limit function is differentiable. Theorem 6.3.1 (Differentiable Limit Theorem). Let fn ! f pointwise on the 0 closed interval [a; b], and assume that each fn is differentiable. If (fn) converges uniformly on [a; b] to a function g, then f is differentiable and f 0 = g. Proof. Let > 0 and fix c 2 [a; b]. Our goal is to show that f 0(c) exists and equals g(c). To this end, we will show the existence of δ > 0 such that for all 0 < jx − cj < δ, with x 2 [a; b], we have f(x) − f(c) − g(c) < x − c which implies that f(x) − f(c) f 0(c) = lim x!c x − c exists and is equal to g(c). The way forward is to replace (f(x) − f(c))=(x − c) − g(c) with expressions we can hopefully control: f(x) − f(c) f(x) − f(c) fn(x) − fn(c) fn(x) − fn(c) − g(c) = − + x − c x − c x − c x − c 0 0 − f (c) + f (c) − g(c) n n f(x) − f(c) fn(x) − fn(c) ≤ − x − c x − c fn(x) − fn(c) 0 0 + − f (c) + jf (c) − g(c)j: x − c n n The second and third expressions we can control respectively by the differentiability of 0 fn and the uniformly convergence of fn to g. -
G: Uniform Convergence of Fourier Series
G: Uniform Convergence of Fourier Series From previous work on the prototypical problem (and other problems) 8 < ut = Duxx 0 < x < l ; t > 0 u(0; t) = 0 = u(l; t) t > 0 (1) : u(x; 0) = f(x) 0 < x < l we developed a (formal) series solution 1 1 X X 2 2 2 nπx u(x; t) = u (x; t) = b e−n π Dt=l sin( ) ; (2) n n l n=1 n=1 2 R l nπy with bn = l 0 f(y) sin( l )dy. These are the Fourier sine coefficients for the initial data function f(x) on [0; l]. We have no real way to check that the series representation (2) is a solution to (1) because we do not know we can interchange differentiation and infinite summation. We have only assumed that up to now. In actuality, (2) makes sense as a solution to (1) if the series is uniformly convergent on [0; l] (and its derivatives also converges uniformly1). So we first discuss conditions for an infinite series to be differentiated (and integrated) term-by-term. This can be done if the infinite series and its derivatives converge uniformly. We list some results here that will establish this, but you should consult Appendix B on calculus facts, and review definitions of convergence of a series of numbers, absolute convergence of such a series, and uniform convergence of sequences and series of functions. Proofs of the following results can be found in any reasonable real analysis or advanced calculus textbook. 0.1 Differentiation and integration of infinite series Let I = [a; b] be any real interval. -
Noncommutative Ergodic Theorems for Connected Amenable Groups 3
NONCOMMUTATIVE ERGODIC THEOREMS FOR CONNECTED AMENABLE GROUPS MU SUN Abstract. This paper is devoted to the study of noncommutative ergodic theorems for con- nected amenable locally compact groups. For a dynamical system (M,τ,G,σ), where (M, τ) is a von Neumann algebra with a normal faithful finite trace and (G, σ) is a connected amenable locally compact group with a well defined representation on M, we try to find the largest non- commutative function spaces constructed from M on which the individual ergodic theorems hold. By using the Emerson-Greenleaf’s structure theorem, we transfer the key question to proving the ergodic theorems for Rd group actions. Splitting the Rd actions problem in two cases accord- ing to different multi-parameter convergence types—cube convergence and unrestricted conver- gence, we can give maximal ergodic inequalities on L1(M) and on noncommutative Orlicz space 2(d−1) L1 log L(M), each of which is deduced from the result already known in discrete case. Fi- 2(d−1) nally we give the individual ergodic theorems for G acting on L1(M) and on L1 log L(M), where the ergodic averages are taken along certain sequences of measurable subsets of G. 1. Introduction The study of ergodic theorems is an old branch of dynamical system theory which was started in 1931 by von Neumann and Birkhoff, having its origins in statistical mechanics. While new applications to mathematical physics continued to come in, the theory soon earned its own rights as an important chapter in functional analysis and probability. In the classical situation the sta- tionarity is described by a measure preserving transformation T , and one considers averages taken along a sequence f, f ◦ T, f ◦ T 2,.. -
Series of Functions Theorem 6.4.2
Math 341 Lecture #30 x6.4: Series of Functions Recall that we constructed the continuous nowhere differentiable function from Section 5.4 by using a series. We will develop the tools necessary to showing that this pointwise convergent series is indeed a continuous function. Definition 6.4.1. Let fn, n 2 N, and f be functions on A ⊆ R. The infinite series 1 X fn(x) = f1(x) + f2(x) + f3(x) + ··· n=1 converges pointwise on A to f(x) if the sequence of partial sums, sk(x) = f1(x) + f2(x) + ··· + fk(x) converges pointwise to f(x). The series converges uniformly on A to f if the sequence sk(x) converges uniformly on A to f(x). Uniform convergence of a series on A implies pointwise convergence of the series on A. For a pointwise or uniformly convergent series we write 1 1 X X f = fn or f(x) = fn(x): n=1 n=1 When the functions fn are continuous on A, each partial sum sk(x) is continuous on A by the Algebraic Continuity Theorem (Theorem 4.3.4). We can therefore apply the theory for uniformly convergent sequences to series. Theorem 6.4.2 (Term-by-term Continuity Theorem). Let fn be continuous functions on A ⊆ . If R 1 X fn n=1 converges uniformly to f on A, then f is continuous on A. Proof. We apply Theorem 6.2.6 to the partial sums sk = f1 + f2 + ··· + fk. When the functions fn are differentiable on a closed interval [a; b], we have that each partial sum sk is differentiable on [a; b] as well. -
Classical Analysis
Classical Analysis Edmund Y. M. Chiang December 3, 2009 Abstract This course assumes students to have mastered the knowledge of complex function theory in which the classical analysis is based. Either the reference book by Brown and Churchill [6] or Bak and Newman [4] can provide such a background knowledge. In the all-time classic \A Course of Modern Analysis" written by Whittaker and Watson [23] in 1902, the authors divded the content of their book into part I \The processes of analysis" and part II \The transcendental functions". The main theme of this course is to study some fundamentals of these classical transcendental functions which are used extensively in number theory, physics, engineering and other pure and applied areas. Contents 1 Separation of Variables of Helmholtz Equations 3 1.1 What is not known? . .8 2 Infinite Products 9 2.1 Definitions . .9 2.2 Cauchy criterion for infinite products . 10 2.3 Absolute and uniform convergence . 11 2.4 Associated series of logarithms . 14 2.5 Uniform convergence . 15 3 Gamma Function 20 3.1 Infinite product definition . 20 3.2 The Euler (Mascheroni) constant γ ............... 21 3.3 Weierstrass's definition . 22 3.4 A first order difference equation . 25 3.5 Integral representation definition . 25 3.6 Uniform convergence . 27 3.7 Analytic properties of Γ(z)................... 30 3.8 Tannery's theorem . 32 3.9 Integral representation . 33 3.10 The Eulerian integral of the first kind . 35 3.11 The Euler reflection formula . 37 3.12 Stirling's asymptotic formula . 40 3.13 Gauss's Multiplication Formula . -
Uniform Convergence and Polynomial Approximation
PROBLEMS AND NOTES: UNIFORM CONVERGENCE AND POLYNOMIAL APPROXIMATION SAMEER CHAVAN Abstract. These are the lecture notes prepared for the participants of IST to be conducted at BP, Pune from 3rd to 15th November, 2014. Contents 1. Pointwise and Uniform Convergence 1 2. Lebesgue's Proof of Weierstrass' Theorem 2 3. Bernstein's Theorem 3 4. Applications of Weierstrass' Theorem 4 5. Stone's Theorem and its Consequences 5 6. A Proof of Stone's Theorem 7 7. M¨untz-Sz´aszTheorem 8 8. Nowhere Differentiable Continuous Function 9 References 10 1. Pointwise and Uniform Convergence n Exercise 1.1 : Consider the function fn(x) = x for x 2 [0; 1]: Check that ffng converges pointwise to f; where f(x) = 0 for x 2 [0; 1) and f(1) = 1: n Exercise 1.2 : Consider the function fm(x) = limn!1(cos(m!πx)) for x 2 R: Verify the following: (1) ffmg converges pointwise to f; where f(x) = 0 if x 2 R n Q; and f(x) = 1 for x 2 Q: (2) f is discontinuous everywhere, and hence non-integrable. Remark 1.3 : If f is pointwise limit of a sequence of continuous functions then the set of continuties of f is everywhere dense [1, Pg 115]. Consider the vector space B[a; b] of bounded function from [a; b] into C: Let fn; f be such that fn − f 2 B[a; b]. A sequence ffng converges uniformly to f if kfn − fk1 := sup jfn(x) − f(x)j ! 0 as n ! 1: x2[a;b] 1 2 SAMEER CHAVAN Theorem 1.4. -
Basic Functional Analysis Master 1 UPMC MM005
Basic Functional Analysis Master 1 UPMC MM005 Jean-Fran¸coisBabadjian, Didier Smets and Franck Sueur October 18, 2011 2 Contents 1 Topology 5 1.1 Basic definitions . 5 1.1.1 General topology . 5 1.1.2 Metric spaces . 6 1.2 Completeness . 7 1.2.1 Definition . 7 1.2.2 Banach fixed point theorem for contraction mapping . 7 1.2.3 Baire's theorem . 7 1.2.4 Extension of uniformly continuous functions . 8 1.2.5 Banach spaces and algebra . 8 1.3 Compactness . 11 1.4 Separability . 12 2 Spaces of continuous functions 13 2.1 Basic definitions . 13 2.2 Completeness . 13 2.3 Compactness . 14 2.4 Separability . 15 3 Measure theory and Lebesgue integration 19 3.1 Measurable spaces and measurable functions . 19 3.2 Positive measures . 20 3.3 Definition and properties of the Lebesgue integral . 21 3.3.1 Lebesgue integral of non negative measurable functions . 21 3.3.2 Lebesgue integral of real valued measurable functions . 23 3.4 Modes of convergence . 25 3.4.1 Definitions and relationships . 25 3.4.2 Equi-integrability . 27 3.5 Positive Radon measures . 29 3.6 Construction of the Lebesgue measure . 34 4 Lebesgue spaces 39 4.1 First definitions and properties . 39 4.2 Completeness . 41 4.3 Density and separability . 42 4.4 Convolution . 42 4.4.1 Definition and Young's inequality . 43 4.4.2 Mollifier . 44 4.5 A compactness result . 45 5 Continuous linear maps 47 5.1 Space of continuous linear maps . 47 5.2 Uniform boundedness principle{Banach-Steinhaus theorem .