Approximation of the Lerch zeta-function
|
|
- Χρύσηίς Μαλαξός
- 6 χρόνια πριν
- Προβολές:
Transcript
1 Approximaion of he Lerch zea-funcion Ramūna Garunkši Deparmen of Mahemaic and Informaic Vilniu Univeriy Naugarduko Vilniu Lihuania ramunagarunki@mafvul Abrac We conider uniform in parameer approximaion of he Lerch zeafuncion by Dirichle polynomial I allow u o obain uniform in parameer bound in he criical rip Le = σ + i be a complex variable For σ > he Lerch zea-funcion i given by he erie (m + α) wih parameer λ IR and 0 < α Thi funcion can be analyically coninued o he whole complex plane wih a poible excepion of a pole a he poin = Noe ha L(λ α ) i periodic in λ In [] Chaper 3 we ee ha for fixed 0 < λ < and for σ σ 0 > 0 πλx he following approximaion hold x (m + α) + O ( x σ) In hi paper we preen a uniform in λ and α approximaion of he above ype We alo calculae an explici conan in he error erm Le Θ(z) denoe ome complex number uch ha Θ(z) z Parially uppored by Gran from Lihuanian Foundaion of Sudie and Science
2 Theorem Suppoe ha / λ / λ 0 and le σ 0 x Then (( ) ) 4 (m + α) + Θ + 05 x σ We give he proof a he end of he paper By he eimae m (m + α) σ ( + α) σ + dx (x + α) σ ( + ( σ) α) σ if 0 σ e ( + α) if σ we obain he following: Corollary Suppoe ha / λ / λ 0 and le σ 0 Then ( + ( σ) α) σ L(λ α ) α σ + 7 λ σ + if 0 σ e ( + α) if σ To find an aympoic dependence on he parameer λ and α we need an approximae funcional equaion Theorem 3 Le 0 < λ 0 < α and 0 < σ Moreover le y = (/(π)) / q = [y] k = [y α] and β = q k () where k + ( π ( π + e(λm) (m + α) ( ) σ q +i πi i+ e 4 πiλα ) e( αm) e π+πiσ+πiα (m + λ) ( {λ}) ) σ e if(λασ) ψ(y q k {λ} α) + O( σ ) f(λ α ) = π πe (α {λ} ) αβ + y(β + {λ} α) (q + k) {λ}(β + α)
3 and ψ(a) = co(π(a / a /8)) co(πa) Formula () immediaely follow from formula () of Chaper 4 of [] Though no menioned in [] one can ee from he proof of () ha formula () hold uniformly in λ and α From Theorem 3 we derive he following: Corollary 4 Le 0 < λ α σ 0 and Then L(λ α ) α ( ( ) π ) σ +i πi i+ e 4 πiλα e π+πiσ+πiα λ ( {λ}) σ if 0 < σ ( σ) if σ uniformly in λ and α For negaive we can ue he formula L(λ α σ + i) = L( λ α σ i) To prove Theorem we need he following: Lemma 5 Le f(x) be a real-valued funcion on [a b] uch ha f (x) i coninuou and monoonic on [a b] and f (x) δ < Then b ( 4 δ e (f(n)) = e (f(x)) dx + Θ π( δ) + 6 ) δ + 3 π a<n b Here e(x) = e πix a Proof of hi lemma can be found for example in Ivić [3]; concerning he explici conan ee Lemma 9 of [] Proof of Theorem Le for u > 0 Then () S(λ u) = m u S(λ u) = S(λ [u]) = eπiλ([u]+) e πiλ = O ( λ ) Now ummaion by par how x (m + α) = S(λ x)(x + α) du S(λ u) (u + α) +
4 Thu we have ha for σ > and any poiive ineger N N S(λ N)(N + α) (m + α) du + S(λ u) N (u + α) + Since he laer inegral converge uniformly on compac ube of he half-plane σ > 0 he above expreion alo remain valid for σ > 0 In view of () N du S(λ u) (u + α) = O ( N σ σ λ ) + and herefore we obain he following approximaion of he funcion L(λ α ) for σ > 0: N S(λ N)(N + α) (m + α) (3) Now le u conider he um (m + α) = + O ( N σ σ λ ) πi(λm ( (m+α))/π) e (m + α) σ Le f(u) = λu ( (u + α))/π Then f (u) = λ /π(u + α) and f (u) λ < for u [x N] Conequenly by Lemma 5 and inegraion by par A(N) := (m + α) i = Hence by parial ummaion we find N x = Θ (m + α) = A(N) N N + α + σ x e πi(λu ( (u+α))/π) du + Θ(05) ( ) A(u) du (u + α) σ+ Now in view of (3) ending N o infiniy we obain (( ) 4 (m + α) + Θ + 05 The la formula i proved for σ > 0 By he coninuiy of he Lerch zea-funcion i alo remain valid for σ 0 x σ ) 4
5 Reference [] R Garunkši The effecive univeraliy heorem for he Riemann zea funcion in: Proceeding of he eion in analyic number heory and Diophanine equaion MPI-Bonn January - June 00 Ed by D R Heah-Brown B Z Moroz Bonner mahemaiche Schrifen 360 (003) pp [] A Laurinčika and R Garunkši The Lerch Zea-funcion Dordrech Kluwer Academic Publiher (00) [3] A Ivić The Riemann Zea-funcion New York John Wiley (985) Reziumė Sraipnyje nagrinėjame olygia paramer u ažvilgiu Lerch o dzea funkcijo aprokimacija Dirichle polinomai Tai leidžia gaui olygiu paramer u ažvilgiu i verčiu kriinėje juooje 5
( ) ( t) ( 0) ( ) dw w. = = β. Then the solution of (1.1) is easily found to. wt = t+ t. We generalize this to the following nonlinear differential
Periodic oluion of van der Pol differenial equaion. by A. Arimoo Deparmen of Mahemaic Muahi Iniue of Technology Tokyo Japan in Seminar a Kiami Iniue of Technology January 8 9. Inroducion Le u conider a
= e 6t. = t 1 = t. 5 t 8L 1[ 1 = 3L 1 [ 1. L 1 [ π. = 3 π. = L 1 3s = L. = 3L 1 s t. = 3 cos(5t) sin(5t).
Worked Soluion 95 Chaper 25: The Invere Laplace Tranform 25 a From he able: L ] e 6 6 25 c L 2 ] ] L! + 25 e L 5 2 + 25] ] L 5 2 + 5 2 in(5) 252 a L 6 + 2] L 6 ( 2)] 6L ( 2)] 6e 2 252 c L 3 8 4] 3L ] 8L
Ordinal Arithmetic: Addition, Multiplication, Exponentiation and Limit
Ordinal Arithmetic: Addition, Multiplication, Exponentiation and Limit Ting Zhang Stanford May 11, 2001 Stanford, 5/11/2001 1 Outline Ordinal Classification Ordinal Addition Ordinal Multiplication Ordinal
Uniform Convergence of Fourier Series Michael Taylor
Uniform Convergence of Fourier Series Michael Taylor Given f L 1 T 1 ), we consider the partial sums of the Fourier series of f: N 1) S N fθ) = ˆfk)e ikθ. k= N A calculation gives the Dirichlet formula
16. 17. r t te 2t i t 1. 18 19 Find the derivative of the vector function. 19. r t e t cos t i e t sin t j ln t k. 31 33 Evaluate the integral.
SECTION.7 VECTOR FUNCTIONS AND SPACE CURVES.7 VECTOR FUNCTIONS AND SPACE CURVES A Click here for answers. S Click here for soluions. Copyrigh Cengage Learning. All righs reserved.. Find he domain of he
Nowhere-zero flows Let be a digraph, Abelian group. A Γ-circulation in is a mapping : such that, where, and : tail in X, head in
Nowhere-zero flows Let be a digraph, Abelian group. A Γ-circulation in is a mapping : such that, where, and : tail in X, head in : tail in X, head in A nowhere-zero Γ-flow is a Γ-circulation such that
α ]0,1[ of Trigonometric Fourier Series and its Conjugate
aqartvelo mecierebata erovuli aademii moambe 3 # 9 BULLETIN OF THE GEORGIN NTIONL CDEMY OF SCIENCES vol 3 o 9 Mahemaic Some pproimae Properie o he Cezàro Mea o Order ][ o Trigoomeric Fourier Serie ad i
Fourier Series. MATH 211, Calculus II. J. Robert Buchanan. Spring Department of Mathematics
Fourier Series MATH 211, Calculus II J. Robert Buchanan Department of Mathematics Spring 2018 Introduction Not all functions can be represented by Taylor series. f (k) (c) A Taylor series f (x) = (x c)
Nonlinear Analysis: Modelling and Control, 2013, Vol. 18, No. 4,
Nonlinear Analysis: Modelling and Conrol, 23, Vol. 8, No. 4, 493 58 493 Exisence and uniqueness of soluions for a singular sysem of higher-order nonlinear fracional differenial equaions wih inegral boundary
Necessary and sufficient conditions for oscillation of first order nonlinear neutral differential equations
J. Mah. Anal. Appl. 321 (2006) 553 568 www.elsevier.com/locae/jmaa Necessary sufficien condiions for oscillaion of firs order nonlinear neural differenial equaions X.H. ang a,, Xiaoyan Lin b a School of
Section 8.3 Trigonometric Equations
99 Section 8. Trigonometric Equations Objective 1: Solve Equations Involving One Trigonometric Function. In this section and the next, we will exple how to solving equations involving trigonometric functions.
Trigonometric Formula Sheet
Trigonometric Formula Sheet Definition of the Trig Functions Right Triangle Definition Assume that: 0 < θ < or 0 < θ < 90 Unit Circle Definition Assume θ can be any angle. y x, y hypotenuse opposite θ
Global Attractor for a Class of Nonlinear Generalized Kirchhoff-Boussinesq Model
Inernaional Journal of Modern Nonlinear Theory and Applicaion, 6, 5, 8-9 Publihed Online March 6 in SciRe hp://wwwcirporg/journal/ijmna hp://dxdoiorg/36/ijmna659 Global Aracor for a la of Nonlinear Generalized
The one-dimensional periodic Schrödinger equation
The one-dmensonal perodc Schrödnger equaon Jordan Bell jordan.bell@gmal.com Deparmen of Mahemacs, Unversy of Torono Aprl 23, 26 Translaons and convoluon For y, le τ y f(x f(x y. To say ha f : C s unformly
Fractional Colorings and Zykov Products of graphs
Fractional Colorings and Zykov Products of graphs Who? Nichole Schimanski When? July 27, 2011 Graphs A graph, G, consists of a vertex set, V (G), and an edge set, E(G). V (G) is any finite set E(G) is
Math221: HW# 1 solutions
Math: HW# solutions Andy Royston October, 5 7.5.7, 3 rd Ed. We have a n = b n = a = fxdx = xdx =, x cos nxdx = x sin nx n sin nxdx n = cos nx n = n n, x sin nxdx = x cos nx n + cos nxdx n cos n = + sin
EE512: Error Control Coding
EE512: Error Control Coding Solution for Assignment on Finite Fields February 16, 2007 1. (a) Addition and Multiplication tables for GF (5) and GF (7) are shown in Tables 1 and 2. + 0 1 2 3 4 0 0 1 2 3
Fractional Calculus. Student: Manal AL-Ali Dr. Abdalla Obeidat
Fracional Calculu Suen: Manal AL-Ali Dr. Aballa Obeia Deignaion Deignaion mean inegraion an iffereniaion of arbirary orer, In oher ereion i mean ealing wih oeraor like,, i arbirary real or Comle value.
Vidyalankar. Vidyalankar S.E. Sem. III [BIOM] Applied Mathematics - III Prelim Question Paper Solution. 1 e = 1 1. f(t) =
. (a). (b). (c) f() L L e i e Vidyalakar S.E. Sem. III [BIOM] Applied Mahemaic - III Prelim Queio Paper Soluio L el e () i ( ) H( ) u e co y + 3 3y u e co y + 6 uy e i y 6y uyy e co y 6 u + u yy e co y
Areas and Lengths in Polar Coordinates
Kiryl Tsishchanka Areas and Lengths in Polar Coordinates In this section we develop the formula for the area of a region whose boundary is given by a polar equation. We need to use the formula for the
2 Composition. Invertible Mappings
Arkansas Tech University MATH 4033: Elementary Modern Algebra Dr. Marcel B. Finan Composition. Invertible Mappings In this section we discuss two procedures for creating new mappings from old ones, namely,
Areas and Lengths in Polar Coordinates
Kiryl Tsishchanka Areas and Lengths in Polar Coordinates In this section we develop the formula for the area of a region whose boundary is given by a polar equation. We need to use the formula for the
Main source: "Discrete-time systems and computer control" by Α. ΣΚΟΔΡΑΣ ΨΗΦΙΑΚΟΣ ΕΛΕΓΧΟΣ ΔΙΑΛΕΞΗ 4 ΔΙΑΦΑΝΕΙΑ 1
Main source: "Discrete-time systems and computer control" by Α. ΣΚΟΔΡΑΣ ΨΗΦΙΑΚΟΣ ΕΛΕΓΧΟΣ ΔΙΑΛΕΞΗ 4 ΔΙΑΦΑΝΕΙΑ 1 A Brief History of Sampling Research 1915 - Edmund Taylor Whittaker (1873-1956) devised a
Xiaoquan (Michael) Zhang
RESEARCH ARTICLE HO DOES THE INTERNET AFFECT THE FINANCIAL MARKET? AN EQUILIBRIUM MODEL OF INTERNET-FACILITATED FEEDBACK TRADING Xiaoquan (Michael) Zhang School of Buine and Managemen, Hong Kong Unieriy
Other Test Constructions: Likelihood Ratio & Bayes Tests
Other Test Constructions: Likelihood Ratio & Bayes Tests Side-Note: So far we have seen a few approaches for creating tests such as Neyman-Pearson Lemma ( most powerful tests of H 0 : θ = θ 0 vs H 1 :
Research Article Existence of Positive Solutions for Fourth-Order Three-Point Boundary Value Problems
Hindawi Publihing Corporation Boundary Value Problem Volume 27, Article ID 68758, 1 page doi:1.1155/27/68758 Reearch Article Exitence of Poitive Solution for Fourth-Order Three-Point Boundary Value Problem
Matrices and Determinants
Matrices and Determinants SUBJECTIVE PROBLEMS: Q 1. For what value of k do the following system of equations possess a non-trivial (i.e., not all zero) solution over the set of rationals Q? x + ky + 3z
Phys460.nb Solution for the t-dependent Schrodinger s equation How did we find the solution? (not required)
Phys460.nb 81 ψ n (t) is still the (same) eigenstate of H But for tdependent H. The answer is NO. 5.5.5. Solution for the tdependent Schrodinger s equation If we assume that at time t 0, the electron starts
Coefficient Inequalities for a New Subclass of K-uniformly Convex Functions
International Journal of Computational Science and Mathematics. ISSN 0974-89 Volume, Number (00), pp. 67--75 International Research Publication House http://www.irphouse.com Coefficient Inequalities for
Reminders: linear functions
Reminders: linear functions Let U and V be vector spaces over the same field F. Definition A function f : U V is linear if for every u 1, u 2 U, f (u 1 + u 2 ) = f (u 1 ) + f (u 2 ), and for every u U
I.I. Guseinov. Department of Physics, Faculty of Arts and Sciences, Onsekiz Mart University, Çanakkale, Turkey
Epanion and one-range addiion heore for coplee orhonoral e of pinor wave funcion and Slaer pinor orbial of arbirary half-inegral pin in poiion oenu and four-dienional pace I.I. Gueinov Deparen of Phyic
( ) ( ) ( ) Fourier series. ; m is an integer. r(t) is periodic (T>0), r(t+t) = r(t), t Fundamental period T 0 = smallest T. Fundamental frequency ω
Fourier series e jm when m d when m ; m is an ineger. jm jm jm jm e d e e e jm jm jm jm r( is periodi (>, r(+ r(, Fundamenal period smalles Fundamenal frequeny r ( + r ( is periodi hen M M e j M, e j,
The Laplace transform of Dirichlet L-functions
Nonlinear Analysis: Modelling and Control, 1, Vol. 17, No., 17 138 17 The Lalace transform of Dirichlet L-functions Aidas Balčiūnas a, Antanas Laurinčikas b a Institute of Mathematics and Informatics,
The Student s t and F Distributions Page 1
The Suden s and F Disribuions Page The Fundamenal Transformaion formula for wo random variables: Consider wo random variables wih join probabiliy disribuion funcion f (, ) simulaneously ake on values in
ST5224: Advanced Statistical Theory II
ST5224: Advanced Statistical Theory II 2014/2015: Semester II Tutorial 7 1. Let X be a sample from a population P and consider testing hypotheses H 0 : P = P 0 versus H 1 : P = P 1, where P j is a known
Example Sheet 3 Solutions
Example Sheet 3 Solutions. i Regular Sturm-Liouville. ii Singular Sturm-Liouville mixed boundary conditions. iii Not Sturm-Liouville ODE is not in Sturm-Liouville form. iv Regular Sturm-Liouville note
Practice Exam 2. Conceptual Questions. 1. State a Basic identity and then verify it. (a) Identity: Solution: One identity is csc(θ) = 1
Conceptual Questions. State a Basic identity and then verify it. a) Identity: Solution: One identity is cscθ) = sinθ) Practice Exam b) Verification: Solution: Given the point of intersection x, y) of the
Managing Production-Inventory Systems with Scarce Resources
Managing Producion-Invenory Sysems wih Scarce Resources Online Supplemen Proof of Lemma 1: Consider he following dynamic program: where ḡ (x, z) = max { cy + E f (y, z, D)}, (7) x y min(x+u,z) f (y, z,
Every set of first-order formulas is equivalent to an independent set
Every set of first-order formulas is equivalent to an independent set May 6, 2008 Abstract A set of first-order formulas, whatever the cardinality of the set of symbols, is equivalent to an independent
Arithmetical applications of lagrangian interpolation. Tanguy Rivoal. Institut Fourier CNRS and Université de Grenoble 1
Arithmetical applications of lagrangian interpolation Tanguy Rivoal Institut Fourier CNRS and Université de Grenoble Conference Diophantine and Analytic Problems in Number Theory, The 00th anniversary
F19MC2 Solutions 9 Complex Analysis
F9MC Solutions 9 Complex Analysis. (i) Let f(z) = eaz +z. Then f is ifferentiable except at z = ±i an so by Cauchy s Resiue Theorem e az z = πi[res(f,i)+res(f, i)]. +z C(,) Since + has zeros of orer at
6. MAXIMUM LIKELIHOOD ESTIMATION
6 MAXIMUM LIKELIHOOD ESIMAION [1] Maximum Likelihood Estimator (1) Cases in which θ (unknown parameter) is scalar Notational Clarification: From now on, we denote the true value of θ as θ o hen, view θ
Homework 3 Solutions
Homework 3 Solutions Igor Yanovsky (Math 151A TA) Problem 1: Compute the absolute error and relative error in approximations of p by p. (Use calculator!) a) p π, p 22/7; b) p π, p 3.141. Solution: For
Solutions to Exercise Sheet 5
Solutions to Eercise Sheet 5 jacques@ucsd.edu. Let X and Y be random variables with joint pdf f(, y) = 3y( + y) where and y. Determine each of the following probabilities. Solutions. a. P (X ). b. P (X
University of Washington Department of Chemistry Chemistry 553 Spring Quarter 2010 Homework Assignment 3 Due 04/26/10
Universiy of Washingon Deparmen of Chemisry Chemisry 553 Spring Quarer 1 Homework Assignmen 3 Due 4/6/1 v e v e A s ds: a) Show ha for large 1 and, (i.e. 1 >> and >>) he velociy auocorrelaion funcion 1)
Math 248 Homework 1. Edward Burkard. Exercise 1. Prove the following Fourier Transforms where a > 0 and c R: f (x) = b. f(x c) = e.
Math 48 Homework Ewar Burkar Exercise. Prove the following Fourier Transforms where a > an c : a. f(x) f(ξ) b. f(x c) e πicξ f(ξ) c. eπixc f(x) f(ξ c). f(ax) f(ξ) a e. f (x) πiξ f(ξ) f. xf(x) f(ξ) πi ξ
C.S. 430 Assignment 6, Sample Solutions
C.S. 430 Assignment 6, Sample Solutions Paul Liu November 15, 2007 Note that these are sample solutions only; in many cases there were many acceptable answers. 1 Reynolds Problem 10.1 1.1 Normal-order
2. Let H 1 and H 2 be Hilbert spaces and let T : H 1 H 2 be a bounded linear operator. Prove that [T (H 1 )] = N (T ). (6p)
Uppsala Universitet Matematiska Institutionen Andreas Strömbergsson Prov i matematik Funktionalanalys Kurs: F3B, F4Sy, NVP 2005-03-08 Skrivtid: 9 14 Tillåtna hjälpmedel: Manuella skrivdon, Kreyszigs bok
ECE145a / 218a Tuned Amplifier Design -basic gain relationships
ca note, M. Rodwe, copyrighted 009 ECE45a / 8a uned Ampifier Deign -aic ga reationhip -deign the (impe) uniatera imit it Mark Rodwe Univerity of Caifornia, anta Barara rodwe@ece.uc.edu 805-893-344, 805-893-36
Almost all short intervals containing prime numbers
ACTA ARITHMETICA LXXVI (6 Almos all shor inervals conaining prime nmbers by Chaoha Jia (Beijing Inrocion In 37, Cramér [] conjecred ha every inerval (n, n f(n log 2 n conains a prime for some f(n as n
Solution Series 9. i=1 x i and i=1 x i.
Lecturer: Prof. Dr. Mete SONER Coordinator: Yilin WANG Solution Series 9 Q1. Let α, β >, the p.d.f. of a beta distribution with parameters α and β is { Γ(α+β) Γ(α)Γ(β) f(x α, β) xα 1 (1 x) β 1 for < x
CHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS
CHAPTER 5 SOLVING EQUATIONS BY ITERATIVE METHODS EXERCISE 104 Page 8 1. Find the positive root of the equation x + 3x 5 = 0, correct to 3 significant figures, using the method of bisection. Let f(x) =
On Strong Product of Two Fuzzy Graphs
Inernaional Journal of Scienific and Research Publicaions, Volume 4, Issue 10, Ocober 014 1 ISSN 50-3153 On Srong Produc of Two Fuzzy Graphs Dr. K. Radha* Mr.S. Arumugam** * P.G & Research Deparmen of
2. THEORY OF EQUATIONS. PREVIOUS EAMCET Bits.
EAMCET-. THEORY OF EQUATIONS PREVIOUS EAMCET Bits. Each of the roots of the equation x 6x + 6x 5= are increased by k so that the new transformed equation does not contain term. Then k =... - 4. - Sol.
Reservoir modeling. Reservoir modelling Linear reservoirs. The linear reservoir, no input. Starting up reservoir modeling
Reservoir modeling Reservoir modelling Linear reservoirs Paul Torfs Basic equaion for one reservoir:) change in sorage = sum of inflows minus ouflows = Q in,n Q ou,n n n jus an ordinary differenial equaion
Approximation of distance between locations on earth given by latitude and longitude
Approximation of distance between locations on earth given by latitude and longitude Jan Behrens 2012-12-31 In this paper we shall provide a method to approximate distances between two points on earth
ω = radians per sec, t = 3 sec
Secion. Linear and Angular Speed 7. From exercise, =. A= r A = ( 00 ) (. ) = 7,00 in 7. Since 7 is in quadran IV, he reference 7 8 7 angle is = =. In quadran IV, he cosine is posiive. Thus, 7 cos = cos
Parametrized Surfaces
Parametrized Surfaces Recall from our unit on vector-valued functions at the beginning of the semester that an R 3 -valued function c(t) in one parameter is a mapping of the form c : I R 3 where I is some
Roman Witu la 1. Let ξ = exp(i2π/5). Then, the following formulas hold true [6]:
Novi Sad J. Math. Vol. 43 No. 1 013 9- δ-fibonacci NUMBERS PART II Roman Witu la 1 Abstract. This is a continuation of paper [6]. We study fundamental properties applications of the so called δ-fibonacci
Congruence Classes of Invertible Matrices of Order 3 over F 2
International Journal of Algebra, Vol. 8, 24, no. 5, 239-246 HIKARI Ltd, www.m-hikari.com http://dx.doi.org/.2988/ija.24.422 Congruence Classes of Invertible Matrices of Order 3 over F 2 Ligong An and
SCITECH Volume 13, Issue 2 RESEARCH ORGANISATION Published online: March 29, 2018
Journal of rogressive Research in Mathematics(JRM) ISSN: 2395-028 SCITECH Volume 3, Issue 2 RESEARCH ORGANISATION ublished online: March 29, 208 Journal of rogressive Research in Mathematics www.scitecresearch.com/journals
Evaluation of some non-elementary integrals of sine, cosine and exponential integrals type
Noname manuscript No. will be inserted by the editor Evaluation of some non-elementary integrals of sine, cosine and exponential integrals type Victor Nijimbere Received: date / Accepted: date Abstract
Problem Set 3: Solutions
CMPSCI 69GG Applied Information Theory Fall 006 Problem Set 3: Solutions. [Cover and Thomas 7.] a Define the following notation, C I p xx; Y max X; Y C I p xx; Ỹ max I X; Ỹ We would like to show that C
Asymptotic behavior of solutions of mixed type impulsive neutral differential equations
Tariboon e al. Advance in Difference Equaion 2014, 2014:327 hp://www.advanceindifferenceequaion.com/conen/2014/1/327 R E S E A R C H Open Acce Aympoic behavior of oluion of mixed ype impulive neural differenial
Finite Field Problems: Solutions
Finite Field Problems: Solutions 1. Let f = x 2 +1 Z 11 [x] and let F = Z 11 [x]/(f), a field. Let Solution: F =11 2 = 121, so F = 121 1 = 120. The possible orders are the divisors of 120. Solution: The
( P) det. constitute the cofactor matrix, or the matrix of the cofactors: com P = c. ( 1) det
Aendix C Tranfer Matrix Inverion To invert one matrix P, the variou te are a follow: calculate it erminant ( P calculate the cofactor ij of each element, tarting from the erminant of the correonding minor
HOMEWORK 4 = G. In order to plot the stress versus the stretch we define a normalized stretch:
HOMEWORK 4 Problem a For the fast loading case, we want to derive the relationship between P zz and λ z. We know that the nominal stress is expressed as: P zz = ψ λ z where λ z = λ λ z. Therefore, applying
Mellin transforms and asymptotics: Harmonic sums
Mellin tranform and aymptotic: Harmonic um Phillipe Flajolet, Xavier Gourdon, Philippe Duma Die Theorie der reziproen Funtionen und Integrale it ein centrale Gebiet, welche manche anderen Gebiete der Analyi
A NOTE ON ENNOLA RELATION. Jae Moon Kim and Jado Ryu* 1. INTRODUCTION
TAIWANESE JOURNAL OF MATHEMATICS Vol 8, No 5, pp 65-66, Ocober 04 DOI: 0650/m804665 Th paper avalable ole a hp://ouralawamahocorw A NOTE ON ENNOLA RELATION Jae Moo Km ad Jado Ryu* Abrac Eola ve a example
Commutative Monoids in Intuitionistic Fuzzy Sets
Commutative Monoids in Intuitionistic Fuzzy Sets S K Mala #1, Dr. MM Shanmugapriya *2 1 PhD Scholar in Mathematics, Karpagam University, Coimbatore, Tamilnadu- 641021 Assistant Professor of Mathematics,
ECE Spring Prof. David R. Jackson ECE Dept. Notes 2
ECE 634 Spring 6 Prof. David R. Jackson ECE Dept. Notes Fields in a Source-Free Region Example: Radiation from an aperture y PEC E t x Aperture Assume the following choice of vector potentials: A F = =
Deterministic Policy Gradient Algorithms: Supplementary Material
Determinitic Policy Gradient lgorithm: upplementary Material. Regularity Condition Within the text we have referred to regularity condition on the MDP: Regularity condition.1: p(, a), a p(, a), µ θ (),
The third moment for the parabolic Anderson model
The hird momen for he parabolic Anderson model Le Chen Universiy of Kansas Thursday nd Augus, 8 arxiv:69.5v mah.pr] 5 Sep 6 Absrac In his paper, we sudy he parabolic Anderson model saring from he Dirac
EXISTENCE AND UNIQUENESS THEOREM FOR FRACTIONAL DIFFERENTIAL EQUATION WITH INTEGRAL BOUNDARY CONDITION
Journal of Fractional Calculu and Application, Vol. 3, July 212, No. 6, pp. 1 9. ISSN: 29-5858. http://www.fcaj.web.com/ EXISTENCE AND UNIQUENESS THEOREM FOR FRACTIONAL DIFFERENTIAL EQUATION WITH INTEGRAL
3.4 SUM AND DIFFERENCE FORMULAS. NOTE: cos(α+β) cos α + cos β cos(α-β) cos α -cos β
3.4 SUM AND DIFFERENCE FORMULAS Page Theorem cos(αβ cos α cos β -sin α cos(α-β cos α cos β sin α NOTE: cos(αβ cos α cos β cos(α-β cos α -cos β Proof of cos(α-β cos α cos β sin α Let s use a unit circle
Homomorphism in Intuitionistic Fuzzy Automata
International Journal of Fuzzy Mathematics Systems. ISSN 2248-9940 Volume 3, Number 1 (2013), pp. 39-45 Research India Publications http://www.ripublication.com/ijfms.htm Homomorphism in Intuitionistic
Second Order Partial Differential Equations
Chapter 7 Second Order Partial Differential Equations 7.1 Introduction A second order linear PDE in two independent variables (x, y Ω can be written as A(x, y u x + B(x, y u xy + C(x, y u u u + D(x, y
Homework 8 Model Solution Section
MATH 004 Homework Solution Homework 8 Model Solution Section 14.5 14.6. 14.5. Use the Chain Rule to find dz where z cosx + 4y), x 5t 4, y 1 t. dz dx + dy y sinx + 4y)0t + 4) sinx + 4y) 1t ) 0t + 4t ) sinx
Differentiation exercise show differential equation
Differentiation exercise show differential equation 1. If y x sin 2x, prove that x d2 y 2 2 + 2y x + 4xy 0 y x sin 2x sin 2x + 2x cos 2x 2 2cos 2x + (2 cos 2x 4x sin 2x) x d2 y 2 2 + 2y x + 4xy (2x cos
ΜΟΝΑΔΕΣ ΑΡΙΣΤΕΙΑΣ ΑΝΟΙΧΤΟΥ ΛΟΓΙΣΜΙΚΟΥ
ΜΟΝΑΔΕΣ ΑΡΙΣΤΕΙΑΣ ΑΝΟΙΧΤΟΥ ΛΟΓΙΣΜΙΚΟΥ Συστήματα γεωγραφικών πληροφοριών 1 ος Κύκλος Εκπαίδευσης ο σεμινάριο Ιουνίου 0 Δρομολόγηση Η δρομολόγηση (rouing) είναι η διαδικασία εύρεσης των «καλύτερων» μονοπατιών
A Note on Intuitionistic Fuzzy. Equivalence Relation
International Mathematical Forum, 5, 2010, no. 67, 3301-3307 A Note on Intuitionistic Fuzzy Equivalence Relation D. K. Basnet Dept. of Mathematics, Assam University Silchar-788011, Assam, India dkbasnet@rediffmail.com
New bounds for spherical two-distance sets and equiangular lines
New bounds for spherical two-distance sets and equiangular lines Michigan State University Oct 8-31, 016 Anhui University Definition If X = {x 1, x,, x N } S n 1 (unit sphere in R n ) and x i, x j = a
Intuitionistic Fuzzy Ideals of Near Rings
International Mathematical Forum, Vol. 7, 202, no. 6, 769-776 Intuitionistic Fuzzy Ideals of Near Rings P. K. Sharma P.G. Department of Mathematics D.A.V. College Jalandhar city, Punjab, India pksharma@davjalandhar.com
Section 7.6 Double and Half Angle Formulas
09 Section 7. Double and Half Angle Fmulas To derive the double-angles fmulas, we will use the sum of two angles fmulas that we developed in the last section. We will let α θ and β θ: cos(θ) cos(θ + θ)
Oscillation Criteria for Nonlinear Damped Dynamic Equations on Time Scales
Oscillaion Crieria for Nonlinear Damped Dynamic Equaions on ime Scales Lynn Erbe, aher S Hassan, and Allan Peerson Absrac We presen new oscillaion crieria for he second order nonlinear damped delay dynamic
ORDINAL ARITHMETIC JULIAN J. SCHLÖDER
ORDINAL ARITHMETIC JULIAN J. SCHLÖDER Abstract. We define ordinal arithmetic and show laws of Left- Monotonicity, Associativity, Distributivity, some minor related properties and the Cantor Normal Form.
On homeomorphisms and C 1 maps
arxv:1804.10691v1 [mah.gm] 7 Apr 018 On homeomorphsms and C 1 maps Nkolaos E. Sofronds Deparmen of Economcs, Unversy of Ioannna, Ioannna 45110, Greece. nsofron@oene.gr, nsofron@cc.uo.gr Absrac Our purpose
Oscillation criteria for two-dimensional system of non-linear ordinary differential equations
Elecronic Journal of Qualiaive Theory of Differenial Equaions 216, No. 52, 1 17; doi: 1.14232/ejqde.216.1.52 hp://www.mah.u-szeged.hu/ejqde/ Oscillaion crieria for wo-dimensional sysem of non-linear ordinary
Econ 2110: Fall 2008 Suggested Solutions to Problem Set 8 questions or comments to Dan Fetter 1
Eon : Fall 8 Suggested Solutions to Problem Set 8 Email questions or omments to Dan Fetter Problem. Let X be a salar with density f(x, θ) (θx + θ) [ x ] with θ. (a) Find the most powerful level α test
Linear singular perturbations of hyperbolic-parabolic type
BULETINUL ACADEMIEI DE ŞTIINŢE A REPUBLICII MOLDOVA. MATEMATICA Number 4, 3, Pages 95 11 ISSN 14 7696 Linear singular perurbaions of hyperbolic-parabolic ype Perjan A. Absrac. We sudy he behavior of soluions
Lecture 2. Soundness and completeness of propositional logic
Lecture 2 Soundness and completeness of propositional logic February 9, 2004 1 Overview Review of natural deduction. Soundness and completeness. Semantics of propositional formulas. Soundness proof. Completeness
Appendix A. Stability of the logistic semi-discrete model.
Ecological Archiv E89-7-A Elizava Pachpky, Rogr M. Nib, and William W. Murdoch. 8. Bwn dicr and coninuou: conumr-rourc dynamic wih ynchronizd rproducion. Ecology 89:8-88. Appndix A. Sabiliy of h logiic
Statistical Inference I Locally most powerful tests
Statistical Inference I Locally most powerful tests Shirsendu Mukherjee Department of Statistics, Asutosh College, Kolkata, India. shirsendu st@yahoo.co.in So far we have treated the testing of one-sided
On the k-bessel Functions
International Mathematical Forum, Vol. 7, 01, no. 38, 1851-1857 On the k-bessel Functions Ruben Alejandro Cerutti Faculty of Exact Sciences National University of Nordeste. Avda. Libertad 5540 (3400) Corrientes,
1. Introduction and Preliminaries.
Faculty of Sciences and Mathematics, University of Niš, Serbia Available at: http://www.pmf.ni.ac.yu/filomat Filomat 22:1 (2008), 97 106 ON δ SETS IN γ SPACES V. Renuka Devi and D. Sivaraj Abstract We
Lecture 12 Modulation and Sampling
EE 2 spring 2-22 Handou #25 Lecure 2 Modulaion and Sampling The Fourier ransform of he produc of wo signals Modulaion of a signal wih a sinusoid Sampling wih an impulse rain The sampling heorem 2 Convoluion
Riemann Hypothesis: a GGC representation
Riemann Hypohesis: a GGC represenaion Nicholas G. Polson Universiy of Chicago Augus 8, 8 Absrac A GGC Generalized Gamma Convoluion represenaion for Riemann s reciprocal ξ-funcion is consruced. This provides
PROPERTIES OF CERTAIN INTEGRAL OPERATORS. a n z n (1.1)
GEORGIAN MATHEMATICAL JOURNAL: Vol. 2, No. 5, 995, 535-545 PROPERTIES OF CERTAIN INTEGRAL OPERATORS SHIGEYOSHI OWA Abstract. Two integral operators P α and Q α for analytic functions in the open unit disk
STAT200C: Hypothesis Testing
STAT200C: Hypothesis Testing Zhaoxia Yu Spring 2017 Some Definitions A hypothesis is a statement about a population parameter. The two complementary hypotheses in a hypothesis testing are the null hypothesis
The Number of Zeros of a Polynomial in a Disk as a Consequence of Restrictions on the Coefficients
The Number of Zeros of a Polynomial in a Disk as a Consequence of Restrictions on the Coefficients Robert Gardner Brett Shields Department of Mathematics and Statistics Department of Mathematics and Statistics