Reccurence Relation of Generalized Mittag Lefer Function
|
|
- Λητώ Ουζουνίδης
- 5 χρόνια πριν
- Προβολές:
Transcript
1 Palestine Journal of Mathematics Vol. 6(2)(217), Palestine Polytechnic University-PPU 217 Reccurence Relation of Generalized Mittag Lefer Function Vana Agarwal Monika Malhotra Communicated by Ayman Badawi MSC 21 Classications: 33E12, 33B15, 11R32. Keywords phrases: Generalized Mittag-Lefer function; Recurrence relation: Wiman's function. The authors are thankful to Prof. Kantesh Gupta, Malviya National Institute of Technology, Jaipur for her valuable help constant encouragement. Abstract. The aim of the present paper is to investigate a recurrence relation an integral representation of generalized Mittag- Lefer function,p which can be reduced to H-function Hyper geometric function. In the end several special cases have also been discussed. 1 Introduction The Swedish Mathematician Gosta Mittag- Lefer [3] in 193, introduced the function E α (z), dened as E α (z) = (z) n, {α, z C; Re(α) > } (1.1) G(αn + 1) where z C G(z) is the Gamma function: α.the Mittag- Lefer function in (1.1) reduces immediately to the exponential function e z = E 1 (z) when α = 1. Mittag- Lefer function naturally occurs as the solution of fractional order differential equation or fractional order integral equation. In 195, Wiman [8] studied a function E (z),generalization of E α (z) dened as follows: E (z) = The function E (z) is known as Wiman function. (z) n, {α, β, z C; Re(α) >, Re(β) > } (1.2) G(αn + β) Prabhakar [4] introduced the function E γ (z) in the form of (see also Kilbas et al.[2]) E γ (z) = (γ) n G(αn + β) where (γ) n is the pochammer symbol (γ) n = G(γ + n) G(γ) (z) n, {α, β, γ, z C; Re(α) >, Re(β) >, Re(γ) > } (1.3) n! = N being the set of positive integers. { 1 (n =, γ ) γ(γ + 1)...(γ + n 1) (n N, γ C) Shukla Prajapati [6] dened investigated the function, E γ,q (z) as E γ,q (z) = (γ) qn (z) n G(αn + β) n! (1.4) {α, β, γ, z C; Re(α) >, Re(β) >, Re(γ) >, q (, 1) N}
2 Reccurence Relation of Generalized Mittag Lefer Function 563 (γ) qn = q qn q ( γ + r 1 ) n (q N, n N := N {}) q r=1 In the sequel of this study, Tariq Ahmad [5] dened the function,p (z) = (γ) qn (z) n (1.5) G(αn + β) (δ) pn {α, β, γ, z C; min{re(α), Re(β), Re(γ), Re(δ) > }, p, q >, q Re(α) + p} It is easily seen that (1.5) is an obvious generalization of (1.1) to (1.4) Setting δ = p = 1 it reduces to (1.4 ) dened by Shukla Prajapati [6], in addition to that if q = 1, then we get eq. (1.3) dened by Prabhakar [4]. On putting γ = δ = p = q = 1 in (1.5 ) it reduces to Wiman's function, moreover if β = 1, Mittag-Lefer function E α (z) will be the result. 2 Recurrence Relation Theorem 1 For (R(α + a) >, R(β + s) >, R(c) >, p, q (, 1) N), we get α+a,β+s+1,p (cz) Eγ,δ,q (cz) = (β + s)(β + s + 2)Eγ,δ,q (cz) +(α + a) 2 z 2 Ë γ,δ,q (cz) + (α + a)(α + a + 2(β + s + 1))z (cz) (2.1) Where,p (z) = d dz Eγ,δ,q,p (z) Ë γ,δ,q d2,p (z) = dz 2 Eγ,δ,q,p (z) By putting α + a = k β + s = m in this theorem, we get the following corollary Corollary 1
3 564 Vana Agarwal Monika Malhotra k,m+1,p (cz) Eγ,δ,q k,m+2,p (cz) = m(m + 2)Eγ,δ,q k,m+3,p (cz) + k2 z 2 Ë γ,δ,q k,m+3,p (cz) Proof of Theorem 1 +k(k + 2m + 2)z k,m+3,p (cz) (2.2) By the fundamental relation of Gamma function G(z + 1) = zgz to (1.5), we can write α+a,β+s+1,p (cz) = (2.3) {(α + a)n + β + s}g((α + a)n + β + s)(δ) pn (cz) = Equation (2.4) can be written as follows: {(α + a)n + β + s + 1}{(α + a)n + β + s}g((α + a)n + β + s)(δ) pn (2.4) (cz) = (cz) = Eγ,δ,q α+a,β+s+1,p 1 [ G((α + a)n + β + s)(δ) pn {(α + a)n + β + s} 1 {(α + a) + β + s + 1} ] For convenience we denote summation in (2.5) by S, {(α + a)n + β + s + 1}G((α + a)n + β + s)(δ) pn (2.5) S = Applying a simple identity {(α + a)n + β + s + 1}G((α + a)n + β + s)(δ) pn (2.6) = α+a,β+s+1,p (cz) Eγ,δ,q (cz) 1 u = 1 u(u + 1) + 1 u + 1 to (2.6) u = ((α + a)n + β + s + 1) + S = {(α + a)n + β + s} {(α + a)n + β + s}{(α + a)n + β + s + 1}
4 Reccurence Relation of Generalized Mittag Lefer Function 565 S = (α + a) +(β + s) +(α + a) 2 +u +v n n 2 n where u = (α + a)(2β + 2s + 1) v = (β + s)(β + s + 1) (2.7) Now express each summation on right h side of (2.7) as follows: From (2.8) we get d 2 dz 2 (z2 ) = (n + 2)(n + 1) (2.8) Considering n 2 = z 2 Ë γ,δ,q (cz) + 4z (cz) n 3 (2.9) G{(α + a)n + β + s + 3}(δ) pn Similarly we get d dz (zeγ,δ,q α+a,β+s+1,p ) = (n + 1) (2.1) Using (2.9) (2.11) we have n = z (cz) (2.11) n 2 = z 2 Ë γ,δ,q G((α + a)n + β + s + 3)(δ) (cz) + z (cz) (2.12) pn Using (2.11) (2.12) in (2.7), we get
5 566 Vana Agarwal Monika Malhotra S = (α + a) 2 [z 2 Ë γ,δ,q (cz) + z (cz)] +(α + a + u)z (cz) (β + s + v)eγ,δ,q (cz) (2.13) From (2.6) (2.13) we get the proof of theorem 1 3 Integral Representation Theorem 2 We get t β+s α+a,β+s,p (tα+a )dt = 1 c n [Eγ,δ,q α+a,β+s+1,p (c) Eγ,δ,q (c)] (3.1) (R(α + a) >, R(β + s) >, R(γ) >, q (, 1) N) Setting α + a = k N β + s = m N in (3.1) yields Corollary 2 Where t m k,m,p (tk )dt = 1 c n [Eγ,δ,q k,m+1,p (c) Eγ,δ,q k,m+2,p (c)] (3.2) k, m N Proof Putting z=1 in (2.6) gives It is easy to nd that (γ) qn (c) n G((α + a)n + β + s){(α + a)n + β + s + 1)}(δ) pn = [ α+a,β+s+1,p (c) Eγ,δ,q (c)] (3.3) t β+s α+a,β+s,p (tα+a )dt = For z = 1 in (3.4) (γ) qn (z) (α+a)n+β+s+1 {(α + a)n + β + s + 1)}G((α + a)n + β + s)(δ) pn (3.4) t β+s α+a,β+s,p (tα+a )dt = (γ) qn {(α + a)n + β + s + 1)}G((α + a)n + β + s)(δ) pn (3.5) On comparing (3.3) with the identity obtained in (3.5) is seen to yields (3.1) in theorem 3
6 Reccurence Relation of Generalized Mittag Lefer Function Special Cases (i) Setting α = 1, q = 1, p = 1, δ = 1, a = in (2.1) we get the following interesting relation (β + s + 2)(β + s + 1) F [γ, β + s + 1, cz] F [γ, β + s + 2, cz] = (β + s)(β + s + 2) F [γ, β + s + 3, cz] z 2 F [γ, β + s + 3, cz] +{1 + 2(β + s + 1)}z F [γ, β + s + 3, cz] (4.1) (ii) Setting δ = p = c = 1 in (2.1), we get a known recurrence relation of E γ,q (z) by Shukla Prajapati [[7],p.134,eq(2.1)]. where E γ,q (z) Eγ,q (z) = (β + s)(β + s + 2)Eγ,q (z) α+a,β+s+1 α+a,β+s+2 α+a,β+s+3 +(α + a) 2 z 2 Ë γ,q (z) + (α + a)(α + a + 2(β + s + 1))z E γ,q (z) (4.2) α+a,β+s+3 α+a,β+s+3 E γ,q (z) = d dz Eγ,q (z) Ë γ,q d2 (z) = dz 2 Eγ,q (z) (iii) Putting a =, δ = γ = q = 1; β + s = m N, p = 1 in (2.1), reduces to a known recurrence relation by Gupta Debnath [1] of E (z) Where E α,m+1 (z) = E α,m+2 (z) + m(m + 2)E α,m+3 (z) + α 2 z 2 Ë α,m+3 (z) +α(α + 2m + 2)z E α,m+3 (z) (4.3) E (z) = d dz E (z) Ë (z) = d2 dz 2 E (z) (iv) Substituting δ = 1, c = 1, p = 1 in (3.1), we get integral representation of E γ,q (z) by Shukla Prajapati [7] t β+s E γ,q α+a,β+s (tα+a )dt = [E γ,q (1) Eγ,q (1)] (4.4) α+a,β+s+1 α+a,β+s+2 (v) Substituting γ = 2, q = 1, α = 1, a =, β + s = 1, c = 1, z = 1, p = 1, δ = 1 in (3.1),we get te 2,1,1 1,1,1 (t)dt = [E2,1,1 1,2,1 (1) E2,1,1(1)] (4.5) 1,3,1 Putting γ = 1, δ = 1, q = 1, c = 1, k = 1, m = 1, p = 1 in (3.1) we get
7 568 Vana Agarwal Monika Malhotra or te 1,1,1 1,1,1 (t)dt = E1,1,1 1,2,1 (1) E1,1,1(1) (4.6) 1,3,1 te t dt = E 1,2 (1) E 1,3 (1) (4.7) References [1] I. S. Gupta L. Debnath, Some properties of the Mittag-Lefer functions, Integral Trans. Spec. Funct., 18(5) (27), [2] A. A. Kilbas, M. Siago, R.K. Saxena, Generalized Mittag-Lefer function generalized fractional calculus operators, Integral Transforms Spec. Funct. ; 15(24), [3] G. M. Mittag-Lefer, Sur la nouvelle function EÎś(x), C. R. Acad. Sci. Paris No 137 (193), [4] T. R. Prabhakar, A singular integral equation with a generalized Mittag-Lefer function in the Kernel,Yokohama Math. J.; 19 (1971), [5] T.O. Salim A.W.Faraj, A generalization of Mittag-Lefer function integral operator associated with fractional calculus, J. of Fract. Calc. Appl., 3 (212), [6] A.K. Shukla J.C. Prajapati, On a generalization of Mittag-Lefer function its properties, Math. Anal. Appl., 336 (27), [7] A. K. Shukla J. C. Prajapati, On a Recurrence Relation of Generalized Mittag-Lefer function, Surveys in Mathematics its Applications; 4(29), , [8] A. Wiman, Uber de fundamental satz in der theorie der funktionen EÎś(x), Acta Math. No. ; 29 (195), MR JFM Author information Vana Agarwal Monika Malhotra, Department of Mathematics, Vivekana Institute of Technology, Jaipur, India. vanamnit@gmail.com Received: December 12, 215. Accepted: October 1, 216.
The k-α-exponential Function
Int Journal of Math Analysis, Vol 7, 213, no 11, 535-542 The --Exponential Function Luciano L Luque and Rubén A Cerutti Faculty of Exact Sciences National University of Nordeste Av Libertad 554 34 Corrientes,
Διαβάστε περισσότεραOn 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,
Διαβάστε περισσότεραA summation formula ramified with hypergeometric function and involving recurrence relation
South Asian Journal of Mathematics 017, Vol. 7 ( 1): 1 4 www.sajm-online.com ISSN 51-151 RESEARCH ARTICLE A summation formula ramified with hypergeometric function and involving recurrence relation Salahuddin
Διαβάστε περισσότεραSCITECH 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
Διαβάστε περισσότερα2 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,
Διαβάστε περισσότεραHomomorphism 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
Διαβάστε περισσότερα4.6 Autoregressive Moving Average Model ARMA(1,1)
84 CHAPTER 4. STATIONARY TS MODELS 4.6 Autoregressive Moving Average Model ARMA(,) This section is an introduction to a wide class of models ARMA(p,q) which we will consider in more detail later in this
Διαβάστε περισσότεραThe k-bessel Function of the First Kind
International Mathematical Forum, Vol. 7, 01, no. 38, 1859-186 The k-bessel Function of the First Kin Luis Guillermo Romero, Gustavo Abel Dorrego an Ruben Alejanro Cerutti Faculty of Exact Sciences National
Διαβάστε περισσότεραCoefficient 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
Διαβάστε περισσότεραA General Note on δ-quasi Monotone and Increasing Sequence
International Mathematical Forum, 4, 2009, no. 3, 143-149 A General Note on δ-quasi Monotone and Increasing Sequence Santosh Kr. Saxena H. N. 419, Jawaharpuri, Badaun, U.P., India Presently working in
Διαβάστε περισσότεραA 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
Διαβάστε περισσότεραFinite 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
Διαβάστε περισσότεραderivation of the Laplacian from rectangular to spherical coordinates
derivation of the Laplacian from rectangular to spherical coordinates swapnizzle 03-03- :5:43 We begin by recognizing the familiar conversion from rectangular to spherical coordinates (note that φ is used
Διαβάστε περισσότεραΑπόκριση σε Μοναδιαία Ωστική Δύναμη (Unit Impulse) Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο. Απόστολος Σ.
Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο The time integral of a force is referred to as impulse, is determined by and is obtained from: Newton s 2 nd Law of motion states that the action
Διαβάστε περισσότεραON NEGATIVE MOMENTS OF CERTAIN DISCRETE DISTRIBUTIONS
Pa J Statist 2009 Vol 25(2), 135-140 ON NEGTIVE MOMENTS OF CERTIN DISCRETE DISTRIBUTIONS Masood nwar 1 and Munir hmad 2 1 Department of Maematics, COMSTS Institute of Information Technology, Islamabad,
Διαβάστε περισσότεραCommutative 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,
Διαβάστε περισσότεραThe k-fractional Hilfer Derivative
Int. Journal of Math. Analysis, Vol. 7, 213, no. 11, 543-55 The -Fractional Hilfer Derivative Gustavo Abel Dorrego and Rubén A. Cerutti Faculty of Exact Sciences National University of Nordeste. Av. Libertad
Διαβάστε περισσότεραPROPERTIES 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
Διαβάστε περισσότερα3.4 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
Διαβάστε περισσότεραSecond Order RLC Filters
ECEN 60 Circuits/Electronics Spring 007-0-07 P. Mathys Second Order RLC Filters RLC Lowpass Filter A passive RLC lowpass filter (LPF) circuit is shown in the following schematic. R L C v O (t) Using phasor
Διαβάστε περισσότεραRoman 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
Διαβάστε περισσότεραPalestine Journal of Mathematics Vol. 2(1) (2013), Palestine Polytechnic University-PPU 2013
Palestine Journal of Matheatics Vol. ( (03, 86 99 Palestine Polytechnic University-PPU 03 On Subclasses of Multivalent Functions Defined by a Multiplier Operator Involving the Koatu Integral Operator Ajad
Διαβάστε περισσότεραOrdinal 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
Διαβάστε περισσότεραOn a four-dimensional hyperbolic manifold with finite volume
BULETINUL ACADEMIEI DE ŞTIINŢE A REPUBLICII MOLDOVA. MATEMATICA Numbers 2(72) 3(73), 2013, Pages 80 89 ISSN 1024 7696 On a four-dimensional hyperbolic manifold with finite volume I.S.Gutsul Abstract. In
Διαβάστε περισσότεραDiracDelta. Notations. Primary definition. Specific values. General characteristics. Traditional name. Traditional notation
DiracDelta Notations Traditional name Dirac delta function Traditional notation x Mathematica StandardForm notation DiracDeltax Primary definition 4.03.02.000.0 x Π lim ε ; x ε0 x 2 2 ε Specific values
Διαβάστε περισσότεραExample 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
Διαβάστε περισσότεραHomework 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
Διαβάστε περισσότεραFourier 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)
Διαβάστε περισσότεραCongruence 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
Διαβάστε περισσότεραSection 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.
Διαβάστε περισσότεραMatrices 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
Διαβάστε περισσότεραFURTHER EXTENSION OF THE GENERALIZED HURWITZ-LERCH ZETA FUNCTION OF TWO VARIABLES
FURTHER EXTENSION OF THE GENERALIZED HURWITZ-LERCH ZETA FUNCTION OF TWO VARIABLES KOTTAKKARAN SOOPPY NISAR* Abstract. The main aim of this paper is to give a new generaliation of Hurwit-Lerch Zeta function
Διαβάστε περισσότεραg-selberg integrals MV Conjecture An A 2 Selberg integral Summary Long Live the King Ole Warnaar Department of Mathematics Long Live the King
Ole Warnaar Department of Mathematics g-selberg integrals The Selberg integral corresponds to the following k-dimensional generalisation of the beta integral: D Here and k t α 1 i (1 t i ) β 1 1 i
Διαβάστε περισσότεραCRASH COURSE IN PRECALCULUS
CRASH COURSE IN PRECALCULUS Shiah-Sen Wang The graphs are prepared by Chien-Lun Lai Based on : Precalculus: Mathematics for Calculus by J. Stuwart, L. Redin & S. Watson, 6th edition, 01, Brooks/Cole Chapter
Διαβάστε περισσότεραn=2 In the present paper, we introduce and investigate the following two more generalized
MATEMATIQKI VESNIK 59 (007), 65 73 UDK 517.54 originalni nauqni rad research paper SOME SUBCLASSES OF CLOSE-TO-CONVEX AND QUASI-CONVEX FUNCTIONS Zhi-Gang Wang Abstract. In the present paper, the author
Διαβάστε περισσότεραThe k-mittag-leffler Function
Int. J. Contemp. Math. Sciences, Vol. 7, 212, no. 15, 75-716 The -Mittag-Leffler Function Gustavo Abel Dorrego and Ruben Alejandro Cerutti Faculty of Exact Sciences National University of Nordeste. Avda.
Διαβάστε περισσότεραLecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3
Lecture 2: Dirac notation and a review of linear algebra Read Sakurai chapter 1, Baym chatper 3 1 State vector space and the dual space Space of wavefunctions The space of wavefunctions is the set of all
Διαβάστε περισσότεραThe Negative Neumann Eigenvalues of Second Order Differential Equation with Two Turning Points
Applied Mathematical Sciences, Vol. 3, 009, no., 6-66 The Negative Neumann Eigenvalues of Second Order Differential Equation with Two Turning Points A. Neamaty and E. A. Sazgar Department of Mathematics,
Διαβάστε περισσότεραChapter 6: Systems of Linear Differential. be continuous functions on the interval
Chapter 6: Systems of Linear Differential Equations Let a (t), a 2 (t),..., a nn (t), b (t), b 2 (t),..., b n (t) be continuous functions on the interval I. The system of n first-order differential equations
Διαβάστε περισσότεραGenerating Set of the Complete Semigroups of Binary Relations
Applied Mathematics 06 7 98-07 Published Online January 06 in SciRes http://wwwscirporg/journal/am http://dxdoiorg/036/am067009 Generating Set of the Complete Semigroups of Binary Relations Yasha iasamidze
Διαβάστε περισσότερα6.1. Dirac Equation. Hamiltonian. Dirac Eq.
6.1. Dirac Equation Ref: M.Kaku, Quantum Field Theory, Oxford Univ Press (1993) η μν = η μν = diag(1, -1, -1, -1) p 0 = p 0 p = p i = -p i p μ p μ = p 0 p 0 + p i p i = E c 2 - p 2 = (m c) 2 H = c p 2
Διαβάστε περισσότεραMINIMAL CLOSED SETS AND MAXIMAL CLOSED SETS
MINIMAL CLOSED SETS AND MAXIMAL CLOSED SETS FUMIE NAKAOKA AND NOBUYUKI ODA Received 20 December 2005; Revised 28 May 2006; Accepted 6 August 2006 Some properties of minimal closed sets and maximal closed
Διαβάστε περισσότεραJesse Maassen and Mark Lundstrom Purdue University November 25, 2013
Notes on Average Scattering imes and Hall Factors Jesse Maassen and Mar Lundstrom Purdue University November 5, 13 I. Introduction 1 II. Solution of the BE 1 III. Exercises: Woring out average scattering
Διαβάστε περισσότεραProblem Set 9 Solutions. θ + 1. θ 2 + cotθ ( ) sinθ e iφ is an eigenfunction of the ˆ L 2 operator. / θ 2. φ 2. sin 2 θ φ 2. ( ) = e iφ. = e iφ cosθ.
Chemistry 362 Dr Jean M Standard Problem Set 9 Solutions The ˆ L 2 operator is defined as Verify that the angular wavefunction Y θ,φ) Also verify that the eigenvalue is given by 2! 2 & L ˆ 2! 2 2 θ 2 +
Διαβάστε περισσότεραThe Simply Typed Lambda Calculus
Type Inference Instead of writing type annotations, can we use an algorithm to infer what the type annotations should be? That depends on the type system. For simple type systems the answer is yes, and
Διαβάστε περισσότεραRisk! " #$%&'() *!'+,'''## -. / # $
Risk! " #$%&'(!'+,'''## -. / 0! " # $ +/ #%&''&(+(( &'',$ #-&''&$ #(./0&'',$( ( (! #( &''/$ #$ 3 #4&'',$ #- &'',$ #5&''6(&''&7&'',$ / ( /8 9 :&' " 4; < # $ 3 " ( #$ = = #$ #$ ( 3 - > # $ 3 = = " 3 3, 6?3
Διαβάστε περισσότεραw o = R 1 p. (1) R = p =. = 1
Πανεπιστήµιο Κρήτης - Τµήµα Επιστήµης Υπολογιστών ΗΥ-570: Στατιστική Επεξεργασία Σήµατος 205 ιδάσκων : Α. Μουχτάρης Τριτη Σειρά Ασκήσεων Λύσεις Ασκηση 3. 5.2 (a) From the Wiener-Hopf equation we have:
Διαβάστε περισσότερα1. 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
Διαβάστε περισσότεραHomomorphism of Intuitionistic Fuzzy Groups
International Mathematical Forum, Vol. 6, 20, no. 64, 369-378 Homomorphism o Intuitionistic Fuzz Groups P. K. Sharma Department o Mathematics, D..V. College Jalandhar Cit, Punjab, India pksharma@davjalandhar.com
Διαβάστε περισσότεραApproximation 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
Διαβάστε περισσότεραEvery 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
Διαβάστε περισσότεραON INTEGRAL MEANS FOR FRACTIONAL CALCULUS OPERATORS OF MULTIVALENT FUNCTIONS. S. Sümer Eker 1, H. Özlem Güney 2, Shigeyoshi Owa 3
ON INTEGRAL MEANS FOR FRACTIONAL CALCULUS OPERATORS OF MULTIVALENT FUNCTIONS S. Sümer Eker 1, H. Özlem Güney 2, Shigeyoshi Owa 3 Dedicated to Professor Megumi Saigo, on the occasion of his 7th birthday
Διαβάστε περισσότεραOther 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 :
Διαβάστε περισσότεραSPECIAL FUNCTIONS and POLYNOMIALS
SPECIAL FUNCTIONS and POLYNOMIALS Gerard t Hooft Stefan Nobbenhuis Institute for Theoretical Physics Utrecht University, Leuvenlaan 4 3584 CC Utrecht, the Netherlands and Spinoza Institute Postbox 8.195
Διαβάστε περισσότεραHOMEWORK 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
Διαβάστε περισσότεραSecond 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
Διαβάστε περισσότεραM a t h e m a t i c a B a l k a n i c a. On Some Generalizations of Classical Integral Transforms. Nina Virchenko
M a t h e m a t i c a B a l k a n i c a New Series Vol. 26, 212, Fasc. 1-2 On Some Generalizations of Classical Integral Transforms Nina Virchenko Presented at 6 th International Conference TMSF 211 Using
Διαβάστε περισσότεραST5224: 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
Διαβάστε περισσότεραPartial Differential Equations in Biology The boundary element method. March 26, 2013
The boundary element method March 26, 203 Introduction and notation The problem: u = f in D R d u = ϕ in Γ D u n = g on Γ N, where D = Γ D Γ N, Γ D Γ N = (possibly, Γ D = [Neumann problem] or Γ N = [Dirichlet
Διαβάστε περισσότεραJ. of Math. (PRC) Banach, , X = N(T ) R(T + ), Y = R(T ) N(T + ). Vol. 37 ( 2017 ) No. 5
Vol. 37 ( 2017 ) No. 5 J. of Math. (PRC) 1,2, 1, 1 (1., 225002) (2., 225009) :. I +AT +, T + = T + (I +AT + ) 1, T +. Banach Hilbert Moore-Penrose.. : ; ; Moore-Penrose ; ; MR(2010) : 47L05; 46A32 : O177.2
Διαβάστε περισσότεραChapter 6: Systems of Linear Differential. be continuous functions on the interval
Chapter 6: Systems of Linear Differential Equations Let a (t), a 2 (t),..., a nn (t), b (t), b 2 (t),..., b n (t) be continuous functions on the interval I. The system of n first-order differential equations
Διαβάστε περισσότεραOn a Subclass of k-uniformly Convex Functions with Negative Coefficients
International Mathematical Forum, 1, 2006, no. 34, 1677-1689 On a Subclass of k-uniformly Convex Functions with Negative Coefficients T. N. SHANMUGAM Department of Mathematics Anna University, Chennai-600
Διαβάστε περισσότεραSTRONG DIFFERENTIAL SUBORDINATIONS FOR HIGHER-ORDER DERIVATIVES OF MULTIVALENT ANALYTIC FUNCTIONS DEFINED BY LINEAR OPERATOR
Khayyam J. Math. 3 217, no. 2, 16 171 DOI: 1.2234/kjm.217.5396 STRONG DIFFERENTIA SUBORDINATIONS FOR HIGHER-ORDER DERIVATIVES OF MUTIVAENT ANAYTIC FUNCTIONS DEFINED BY INEAR OPERATOR ABBAS KAREEM WANAS
Διαβάστε περισσότεραGÖKHAN ÇUVALCIOĞLU, KRASSIMIR T. ATANASSOV, AND SINEM TARSUSLU(YILMAZ)
IFSCOM016 1 Proceeding Book No. 1 pp. 155-161 (016) ISBN: 978-975-6900-54-3 SOME RESULTS ON S α,β AND T α,β INTUITIONISTIC FUZZY MODAL OPERATORS GÖKHAN ÇUVALCIOĞLU, KRASSIMIR T. ATANASSOV, AND SINEM TARSUSLU(YILMAZ)
Διαβάστε περισσότεραEE512: 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
Διαβάστε περισσότεραTridiagonal matrices. Gérard MEURANT. October, 2008
Tridiagonal matrices Gérard MEURANT October, 2008 1 Similarity 2 Cholesy factorizations 3 Eigenvalues 4 Inverse Similarity Let α 1 ω 1 β 1 α 2 ω 2 T =......... β 2 α 1 ω 1 β 1 α and β i ω i, i = 1,...,
Διαβάστε περισσότεραAreas 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
Διαβάστε περισσότεραEvaluation 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
Διαβάστε περισσότεραNormalization of the generalized K Mittag-Leffler function and ratio to its sequence of partial sums
Normalization of the generalized K Mittag-Leffler function ratio to its sequence of partial sums H. Rehman, M. Darus J. Salah Abstract. In this article we introduce an operator L k,α (β, δ)(f)(z) associated
Διαβάστε περισσότεραFractional Calculus of a Class of Univalent Functions With Negative Coefficients Defined By Hadamard Product With Rafid -Operator
EUROPEAN JOURNAL OF PURE AND APPLIED MATHEMATICS Vol. 4, No. 2, 2, 62-73 ISSN 37-5543 www.ejpam.com Fractional Calculus of a Class of Univalent Functions With Negative Coefficients Defined By Hadamard
Διαβάστε περισσότεραforms This gives Remark 1. How to remember the above formulas: Substituting these into the equation we obtain with
Week 03: C lassification of S econd- Order L inear Equations In last week s lectures we have illustrated how to obtain the general solutions of first order PDEs using the method of characteristics. We
Διαβάστε περισσότεραBessel functions. ν + 1 ; 1 = 0 for k = 0, 1, 2,..., n 1. Γ( n + k + 1) = ( 1) n J n (z). Γ(n + k + 1) k!
Bessel functions The Bessel function J ν (z of the first kind of order ν is defined by J ν (z ( (z/ν ν Γ(ν + F ν + ; z 4 ( k k ( Γ(ν + k + k! For ν this is a solution of the Bessel differential equation
Διαβάστε περισσότεραSOME INCLUSION RELATIONSHIPS FOR CERTAIN SUBCLASSES OF MEROMORPHIC FUNCTIONS ASSOCIATED WITH A FAMILY OF INTEGRAL OPERATORS. f(z) = 1 z + a k z k,
Acta Math. Univ. Comenianae Vol. LXXVIII, 2(2009), pp. 245 254 245 SOME INCLUSION RELATIONSHIPS FOR CERTAIN SUBCLASSES OF MEROMORPHIC FUNCTIONS ASSOCIATED WITH A FAMILY OF INTEGRAL OPERATORS C. SELVARAJ
Διαβάστε περισσότεραOn Generating Relations of Some Triple. Hypergeometric Functions
It. Joural of Math. Aalysis, Vol. 5,, o., 5 - O Geeratig Relatios of Some Triple Hypergeometric Fuctios Fadhle B. F. Mohse ad Gamal A. Qashash Departmet of Mathematics, Faculty of Educatio Zigibar Ade
Διαβάστε περισσότεραUniform 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
Διαβάστε περισσότεραConcrete Mathematics Exercises from 30 September 2016
Concrete Mathematics Exercises from 30 September 2016 Silvio Capobianco Exercise 1.7 Let H(n) = J(n + 1) J(n). Equation (1.8) tells us that H(2n) = 2, and H(2n+1) = J(2n+2) J(2n+1) = (2J(n+1) 1) (2J(n)+1)
Διαβάστε περισσότεραFractional 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
Διαβάστε περισσότεραThe Spiral of Theodorus, Numerical Analysis, and Special Functions
Theo p. / The Spiral of Theodorus, Numerical Analysis, and Special Functions Walter Gautschi wxg@cs.purdue.edu Purdue University Theo p. 2/ Theodorus of ca. 46 399 B.C. Theo p. 3/ spiral of Theodorus 6
Διαβάστε περισσότεραHeisenberg Uniqueness pairs
Heisenberg Uniqueness pairs Philippe Jaming Bordeaux Fourier Workshop 2013, Renyi Institute Joint work with K. Kellay Heisenberg Uniqueness Pairs µ : finite measure on R 2 µ(x, y) = R 2 e i(sx+ty) dµ(s,
Διαβάστε περισσότεραOn class of functions related to conic regions and symmetric points
Palestine Journal of Mathematics Vol. 4(2) (2015), 374 379 Palestine Polytechnic University-PPU 2015 On class of functions related to conic regions and symmetric points FUAD. S. M. AL SARARI and S.LATHA
Διαβάστε περισσότεραC.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
Διαβάστε περισσότεραDIRECT PRODUCT AND WREATH PRODUCT OF TRANSFORMATION SEMIGROUPS
GANIT J. Bangladesh Math. oc. IN 606-694) 0) -7 DIRECT PRODUCT AND WREATH PRODUCT OF TRANFORMATION EMIGROUP ubrata Majumdar, * Kalyan Kumar Dey and Mohd. Altab Hossain Department of Mathematics University
Διαβάστε περισσότεραk A = [k, k]( )[a 1, a 2 ] = [ka 1,ka 2 ] 4For the division of two intervals of confidence in R +
Chapter 3. Fuzzy Arithmetic 3- Fuzzy arithmetic: ~Addition(+) and subtraction (-): Let A = [a and B = [b, b in R If x [a and y [b, b than x+y [a +b +b Symbolically,we write A(+)B = [a (+)[b, b = [a +b
Διαβάστε περισσότεραAreas 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
Διαβάστε περισσότεραω ω ω ω ω ω+2 ω ω+2 + ω ω ω ω+2 + ω ω+1 ω ω+2 2 ω ω ω ω ω ω ω ω+1 ω ω2 ω ω2 + ω ω ω2 + ω ω ω ω2 + ω ω+1 ω ω2 + ω ω+1 + ω ω ω ω2 + ω
0 1 2 3 4 5 6 ω ω + 1 ω + 2 ω + 3 ω + 4 ω2 ω2 + 1 ω2 + 2 ω2 + 3 ω3 ω3 + 1 ω3 + 2 ω4 ω4 + 1 ω5 ω 2 ω 2 + 1 ω 2 + 2 ω 2 + ω ω 2 + ω + 1 ω 2 + ω2 ω 2 2 ω 2 2 + 1 ω 2 2 + ω ω 2 3 ω 3 ω 3 + 1 ω 3 + ω ω 3 +
Διαβάστε περισσότεραGeneralized fractional calculus of the multiindex Bessel function
Available online at www.isr-publications.com/mns Math. Nat. Sci., 1 2017, 26 32 Research Article Journal Homepage:www.isr-publications.com/mns Generalized ractional calculus o the multiindex Bessel unction.
Διαβάστε περισσότεραInverse trigonometric functions & General Solution of Trigonometric Equations. ------------------ ----------------------------- -----------------
Inverse trigonometric functions & General Solution of Trigonometric Equations. 1. Sin ( ) = a) b) c) d) Ans b. Solution : Method 1. Ans a: 17 > 1 a) is rejected. w.k.t Sin ( sin ) = d is rejected. If sin
Διαβάστε περισσότεραDifferential equations
Differential equations Differential equations: An equation inoling one dependent ariable and its deriaties w. r. t one or more independent ariables is called a differential equation. Order of differential
Διαβάστε περισσότεραStrain gauge and rosettes
Strain gauge and rosettes Introduction A strain gauge is a device which is used to measure strain (deformation) on an object subjected to forces. Strain can be measured using various types of devices classified
Διαβάστε περισσότεραPhys460.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
Διαβάστε περισσότεραIntuitionistic 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
Διαβάστε περισσότεραPractice 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
Διαβάστε περισσότεραSpace-Time Symmetries
Chapter Space-Time Symmetries In classical fiel theory any continuous symmetry of the action generates a conserve current by Noether's proceure. If the Lagrangian is not invariant but only shifts by a
Διαβάστε περισσότεραCERTAIN SUBCLASSES OF UNIFORMLY STARLIKE AND CONVEX FUNCTIONS DEFINED BY CONVOLUTION WITH NEGATIVE COEFFICIENTS
MATEMATIQKI VESNIK 65, 1 (2013), 14 28 March 2013 originalni nauqni rad research paper CERTAIN SUBCLASSES OF UNIFORMLY STARLIKE AND CONVEX FUNCTIONS DEFINED BY CONVOLUTION WITH NEGATIVE COEFFICIENTS M.K.
Διαβάστε περισσότεραSection 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)
Διαβάστε περισσότεραInclusion properties of Generalized Integral Transform using Duality Techniques
DOI.763/s4956-6-8-y Moroccan J. Pure and Appl. Anal.MJPAA Volume 22, 26, Pages 9 6 ISSN: 235-8227 RESEARCH ARTICLE Inclusion properties of Generalied Integral Transform using Duality Techniques Satwanti
Διαβάστε περισσότεραSolution 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
Διαβάστε περισσότεραExercises 10. Find a fundamental matrix of the given system of equations. Also find the fundamental matrix Φ(t) satisfying Φ(0) = I. 1.
Exercises 0 More exercises are available in Elementary Differential Equations. If you have a problem to solve any of them, feel free to come to office hour. Problem Find a fundamental matrix of the given
Διαβάστε περισσότεραStatistical 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
Διαβάστε περισσότεραNowhere-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
Διαβάστε περισσότερα