Generalized Little q-jacobi Polynomials as Eigensolutions of Higher-Order q-difference Operators

Size: px
Start display at page:

Download "Generalized Little q-jacobi Polynomials as Eigensolutions of Higher-Order q-difference Operators"

Transcription

1 Geeralized Little q-jacobi Polyomials as Eigesolutios of Higher-Order q-differece Operators Luc Viet Alexei Zhedaov CRM-2583 December 1998 Cetre de recherches mathématiques, Uiversité de Motréal, C.P. 6128, succ. Cetre-Ville, Motréal QC H3C 3J7, Caada. The work of L.V. is supported i part through fuds provided by NSERC (Caada) ad FCAR (Quebec), viet@crm.umotreal.ca. Doetsk Istitute for Physics ad Techology, Doetsk , Ukraie. The work of A.Zh. was supported i part through fuds provided by SCST (Ukraie) Project #2.4/197, INTAS grat ad project supported by RFBR (Russia). A.Zh. thaks the Cetre de recherches mathématiques of the Uiversité de Motréal for its hospitality, zhedaov@crm.umotreal.ca.

2

3 Abstract We cosider the polyomials p (x; a, b; M) obtaied from the little q-jacobi polyomials p (x; a, b) by isertig a discrete mass M at x = 0 i the orthogoality measure. We show that for a = q j, j = 0, 1, 2,... the polyomials p (x; a, b; M) are eigesolutios of a liear q-differece operator of order 2j + 4 with polyomial coefficiets. This provides a q-aalog of results recetly obtaied for the Krall polyomials. Keywords: Krall s polyomials, little q-jacobi polyomials. Mathematics Subject Classificatios: 33D45. Résumé Nous cosidéros les polyômes p (x; a, b; M) obteus des petits q-polyômes de Jacobi p (x; a, b) e isérat ue masse discrète M à x = 0 das la mesure. Nous motros que pour a = q j, j = 0, 1, 2,... les polyômes p (x; a, b; M) sot solutios propres d u opérateur liéaire aux q-différeces d ordre 2j + 4 avec coefficiets polyomiaux. Nous offros aisi u q-aalogue des résultats obteus récemmet pour les polyômes de Krall.

4

5 1 q-derivative operators ad their represetatio coefficiets Let T be the q-shift operator that acts o fuctios accordig to whith 0 < q < 1 a real umber. Obviously Itroduce the q-derivative operator (see, e.g. [2]) It is called q-derivative because its actio o moomials is with T F (x) = F (qx), (1.1) T F (x) = F (q x), = 0, ±1, ±2,.... (1.2) D q F (x) = (x(1 q)) 1 (1 T ). (1.3) D q x = [] x 1, (1.4) [] = (q 1)/(q 1) (1.5) the so-called q-umber. Moreover lim q 1 D q = D, where D is the ordiary derivative operator with respect to x: DF (x) = F (x). Cosider operators of the form L q = 2N k=0 a k (x) D k q, (1.6) where N is a fixed positive iteger ad a k (x) are polyomials i x of degrees ot exceedig k: a k (x) = k α ks x s, k = 0, 1,..., 2N. (1.7) s=0 Let us itroduce also the related operators L q = T N L q = 2N k=0 a k (q N x) T N D k q. (1.8) The operator L q is a liear combiatio of the operators T 2N, T 2N 1,..., T, T 0 = I, while the operator L q is a liear combiatio of the operators T N, T N 1,..., T 1 N, T N. For q 1 both operators L q ad L q become 2N-order differetial operators with polyomial coefficiets: lim L q = lim L q = q 1 q 1 2N k=0 a k (x) D k. (1.9) The operator L q will prove more practical i searchig for orthogoal polyomials P (x) satisfyig eigevalue equatios of the kid L q P (x) = λ P (x). (1.10) 1

6 It is kow that for N = 1, the little q-jacobi polyomials satisfy a equatio of the form (1.10) with N = 1 [4]. We wish to determie other systems of orthogoal polyomials satisfyig equatio (1.10) with N > 1. To this ed, we shall exted to q-differece operators, the method proposed i [7]. The mai idea of the method is the followig. Cosider the actio of the operator L q upo the moomials x. From (1.6) ad (1.7) we get where ad π s (q ) = α s0 + L q x = s=0 A (s) x s, (1.11) A (s) = q N(s ) [][ 1]... [ s + 1] π s (q ), (1.12) 2N s i=1 α s+i,i [ s][ s 1]... [ s i + 1] (1.13) are polyomials i z = q of degrees ot exceedig 2N s. It is clear that, moreover, A (s) = 0, s > 2N. (1.14) The coefficiets A (s) completely characterize the operator L q. We will call A (s) coefficiets of the operator L q. the represetatio Propositio 1.1 Assume that there are coefficiets A (s) expressible as i (1.12), where π s (q ) are arbitrary polyomials i q of degrees ot exceedig 2N s. Assume also that A (s) = 0, s > 2N (i.e. π s (q ) = 0 for s > 2N). The there exists a uique operator L q of the form (1.8) such that are its represetatio coefficiets. A (s) Proof. Ay polyomial π s (q ) of degree ot exceedig 2N s ca be preseted i form (1.13) with some coefficiets α ik. These coefficiets are determied usig Newto s iterpolatio formula α s+i,i = (q 1)i q si+i(i 1)/2 D i [i]! qπ s (x) i = 0, 1,..., 2N s, (1.15) x=q s, where [i]! = [1][2]... [i] is the q-factorial. Clearly, the coefficiets α ik are determied uiquely by (1.15) from the give polyomials π s (q ). Hece the operator L q is defied uiquely. 2 Basic relatios for polyomials satisfyig eigevalue equatio I this sectio we cosider the basic relatios betwee the represetatio coefficiets A (s) expasio coefficets of polyomials P (x) satisfyig eigevalue equatios. Assume that where B (s) are moic, i.e. that P (x) = s=0 ad the B (s) x s, (2.1) are expasio coefficiets. I what follows we will assume that the polyomials P (x) B (0) = 1. (2.2) 2

7 Substitutig (2.1) ito the eigevalue equatio (1.10) we arrive at the followig set of algebraic relatios s i=0 B (s i) These will be cetral i our aalysis. For s = 0, (2.3) gives A (i) s+i = λ B (s), s = 0, 1, 2,...,. (2.3) λ = A (0). (2.4) Thus from (1.12) we fid that the eigevalues λ have the followig expressio λ = q N π 0 (q ), (2.5) where π 0 (q ) is a polyomial i q of degree ot exceedig 2N. Similarly, for s = 1, (2.3) yields A (1) = Ω B (1), (2.6) where Ω = λ λ 1. From this relatio we fid that B (1) = [] Relatio (2.3) ca be rewritte i the form (λ λ s ) B (s) π 1 (q ) q N π 0 (q ) π 0 (q 1 ). (2.7) = B (s 1) A (1) s+1 + B (s 2) A (2) s A (s). (2.8) >From this relatio we ca coclude, by iductio, that the coefficiets B (s) are ratioal fuctios i q, amely that B (s) = [][ 1]... [ s + 1] Q 1,s(q ) Q 2,s (q ), (2.9) where Q 1,s (q ) is a polyomial of degree ot exceedig 2Ns s, whereas the degree of the polyomial Q 2,s (q ) does ot exceed 2Ns. The problem cosidered up to this poit of fidig the expasio coefficiets B (s) of the polyomials P (x) whe the represetatios coefficiets A (s) are give, always has a uique solutio. Propositio 2.1 Assume that the represetatio coefficiets A (s) of the operator L q satisfy the requiremet A (0) A (0) m, m. (2.10) The there exists a uique set of moic polyomials P (x), = 0, 1,... satisfyig equatio (1.10). Proof. We fid λ m from (2.4); i view of coditio (2.10), a uique B (1) is foud from (2.6). Assumig that all B (1), B (2),..., B (s 1) have thus bee foud recursively, B (s) is the determied i uambigous way owig (2.10). The polyomials P (x) are ot orthogoal i geeral. The requiremet that they form a orthogoal set implies strog additioal restrictios upo the coefficets B (s) ad A (s). Ideed, orthogoal polyomials satisfy three-term recurrece relatio of the form [1] P +1 (x) + b P (x) + u P 1 (x) = xp (x), (2.11) 3

8 with b ad u referred to as the recurrece parameters. From (2.11) ad (2.1) we get the set of relatios B (s+1) +1 B (s+1) + u B (s 1) 1 + b B (s) = 0, s = 0, 1,...,, (2.12) where it is assumed that B ( 1) = B (+1) Takig ito accout that the coefficiets B (s) propositio. = 0. Puttig s = 0 ad s = 1 i (2.12), we fid b = B (1) B (1) +1, u = B (2) B (2) +2 b B (1). (2.13) are ratioal fuctios i q we arrive at the followig Propositio 2.2 If the orthogoal polyomials P (x) are eigefuctios of the operator (1.8), their recurrece coefficiets b, u are ratioal fuctios of the argumet q. The problem of recostructig the represetatio coefficiets A (s) whe the expasio coefficiets B (s) are give, is more difficult. The coefficiets B (s) must of course be ratioal fuctios i q, sice otherwise the problem has o solutios. Assume therefore that B (s) = [][ 1]... [ s + 1] Q 1,s(q ) Q 2,s (q ), (2.14) where the degree of the polyomial Q 1,s (q ) does ot exceed 2Ms s whereas the degree of the polyomial Q 2,s (q ) does ot exceed 2Ms for some positive iteger M N. Cosider relatio (2.6) writte i the form A (1) Ω = [] Q 1,1(q ) Q 2,1 (q ). (2.15) Sice both A (1) ad Ω should be polyomials i q of degrees ot exceedig 2N, we have A (1) = q N(1 ) ρ 1 (q ) [] Q 1,1 (q ), Ω = q N(1 ) ρ 1 (q ) Q 1,2 (q ), (2.16) where ρ 1 (q ) is some polyomial of degree ot exceedig 2N 2M. The relatio (2.3), for s = 2, ca the be rewritte i the form A (2) = (λ λ 2 ) B (2) A (1) 1 B (1) = (Ω + Ω 1 ) B (2) A (1) 1 B (1). (2.17) The represetatio coefficiet A (2) is thus determied uiquely if A (1) ad Ω are kow. Assume that the coefficiets A (2), A (3),..., A (k 1) have bee determied iteratig this process. With s = k, (2.3) ca ow be rewritte i the form A (k) = (λ λ k )B (k) Takig ito accout the fact that B (k 1) A (1) k+1 B(k 2) A (2) λ λ k = Ω + Ω Ω k+1, k+2 B(1) A (k 1) 1. (2.18) we see that A (k) is completely determied from the coefficiets Ω, A (1),..., A (k 1). For the A (s) thus obtaied to actually be represetatio coefficiets of a operator L q, they ecessary eed to satisfy i additio, the coditios of Propositio (1.1). Whe this is so, the correspodig polyomials are eigefuctios of the operator L q. 4

9 3 Little q-jacobi polyomials The moic little q-jacobi polyomials [4] are defied as p (x; a, b) = ( 1) q( 1)/2 (aq; q) (abq +1 ; q) 2φ 1 ( ) q, abq +1 aq qx, (3.1) where (a; q) = (1 a)(1 aq)... (1 aq 1 ) is the q-shifted factorial ad 2 φ 1 deotes the q- hypergeometric fuctio (see, e.g. [2]). The orthogoality relatio is w k p (q k ; a, b) p m (q k ; a, b) = h δ m, (3.2) k=0 where h are appropriate ormalizatio costats, ad the ormalized weight fuctio is w k = (aq; q) (abq 2 ; q) (bq; q) k (aq) k (q; q) k. (3.3) It is assumed that 0 < aq < 1, b < q 1. The expasio coefficiets of the little q-jacobi polyomials are B (s) = b s (q, a 1 q ; q) s. (3.4) (q, a 1 b 1 q 2 ; q) s It is easily verified that equatios (2.8) have the followig solutios A (0) = λ = [](q 1 abq 2 ), A (1) = [](aq q 1 ), A (s) = 0, s 2. (3.5) Hece, the little q-jacobi polyomials satisfy a secod-order q-differece equatio as is well kow [4]. We also eed the value of the fuctio of secod kid, Q (z), at z = 0 (the poit z = 0 is a accumulatio poit of the orthogoality measure): Q (0; a, b) = k=0 P (q k ; a, b) w k q k. (3.6) This sum ca be evaluated usig the q-biomial theorem ad the q-saalschütz formula (see, e.g [2]): Takig ito accout that Q (0; a, b) = ( 1) +1 a ( 1)/2 1 abq q 1 a we ote that if a = q j, j = 1, 2, 3,..., P (0; a, b) = ( 1) q ( 1)/2 (q; q) (bq; q) (abq; q) (abq +1 ; q). (3.7) (aq; q) (abq +1 ; q), (3.8) Φ = Q (0; q j, b) + βp (0; q j, b) = ( 1) q ( 1)/2 (q j+1 ; q) (bq +j+1 ; q) ( β q j ) (1 bq j+1 ) (bq; q) j (q; q) j. (3.9) (1 q j ) (q +1 ; q) j (bq +1 ; q) j 5

10 4 Trasformed q-jacobi polyomials Let P (x) be arbitrary orthogoal polyomials with measure localized o the iterval [a, b]. The correspodig weight fuctio w(x) is assumed to be ormalized to 1, i.e. Itroduce the fuctios of secod kid b a Q (z) = w(x) dx = 1. b a P (x) w(x) dx. (4.1) z x Let c be a poit beyod the orthogoality iterval [a, b] such that Q (c) exists. Cosider the polyomials where G(c){P (x)} = P (x) Φ Φ 1 P 1 (x), = 1, 2,..., P0 (x) = 1, (4.2) Φ = Q (c) + β P (c). (4.3) The otatio G(c){P (x)} stads for the Geroimus trasformatio of the polyomials P (x) at the poit x = c (for details see, e.g. [6]). The weight fuctio w(x) of the polyomials G(c){P (x)} is ( ) w(x) w(x) = κ β δ(x c), (4.4) x c where κ is a appropriate ormalizatio costat. The Geroimus trasformatio thus iserts a cocetrated mass at the poit x = c. The value of this mass depeds o the parameter β. Retur to the case of the little q-jacobi polyomials with a = q j, j = 1, 2, 3,... Perform the Geroimus trasformatio (4.2) with Φ give by (3.9). (I this case c = 0.) The weight fuctio w(x) for the polyomials G(c){P (x)} is ( ) w(x) = κ w k δ(x q k ) β δ(x), (4.5) where k=0 w k = (qj+1 ; q) (bq j+2 ; q) The weight fuctio (4.5) ca be rewritte i the form where M = β (bq; q) k q jk (q; q) k. (4.6) w(x) = κ 1 (w(x; j 1) + M δ(x)), (4.7) 1 qj 1 bq j+1, κ 1 = κ 1 bqj+1 1 q j, ad w(x; j 1) is the weight fuctio correspodig to the q-little Jacobi polyomials with the parameter a = q j replaced with a = q j 1, i.e. w(x; j 1) = w k (j 1)δ(x q k ), (4.8) k=0 6

11 ad w k (j 1) = (qj ; q) (bq; q) k q jk. (4.9) (bq j+1 ; q) (q; q) k Thus the weight fuctio w(x; j) for the polyomials G(0){P (x)} is obtaied from the weight fuctio w(x; j 1) through the additio of a arbitrary mass M at the poit x = 0. I the expasio G(0){P (x)} = the coefficiets B (s) are foud from (3.1) ad (3.9) s=0 B (s) x s, (4.10) B (s) = b s (q ; q) s (q j ; q) s (q; q) s (b 1 q j 2 ; q) s ( 1 q +j s (1 bq )(1 q s ) (1 q +j )(1 bq j+2 s ) ) Y j (), (4.11) Y j ( 1) with Y j () = βq j (q +1 ; q) j (bq +1 ; q) j (q; q) j 1 (bq; q) j+1. (4.12) 5 Costructio of the coefficiets A (s). I this sectio we costruct the coefficiets A (s) for the q-differece operator L q that has the polyomials P (x) as eigefuctios. We start from the relatio A (1) = Ω B (1), (5.1) where Choose Ω proportioal to the deomiator of B (1) : Ω = λ λ 1 = A (0) A (0) 1. (5.2) Ω = bq +j 1 (q 1)(1 b 1 q 1 j 2 ) ( βq j( 1) (q ; q) j (bq ; q) j (bq; q) j+1 (q; q) j 1 ). (5.3) The from (5.1) we get for A (1) the expressio A (1) = (1 q ) ( βq j(1 ) (q +1 ; q) j (bq ; q) j (1 q 1 ) (q; q) j 1 (bq; q) j+1 (1 q +j 1 ) ). (5.4) Usig (5.2) it is ot difficult to show that A (0) = λ = β (q 1)q (j+1) 1 (q ; q) j+1 (bq ; q) j+1 1 q j 1 (Note that A (0) 0 = 0). 7 (q 1)(1 bq +j )(bq; q) j+1 (q; q) j 1. (5.5)

12 Usig ow the explicit expressios for B (1,2) ad A (0,1), we fid A (2) = β(q 1)q (2 )(j+1) 1 (1 q j )(q 2 ; q) j+3 (bq ; q) j 1 (q; q) 2. (5.6) Repeatig this procedure we arrive at the expressio A (s) = β(q 1)q (s )(j+1) 1 (q j ; q) s 1 (q s ; q) s+j+1 (bq ; q) j s+1 (q; q) s + ξ δ s,1 + η δ s,0, (5.7) where ξ = (q 1)(q; q) j 1 (bq; q) j+1 (1 q j+ 1 ), η = (1 q )(1 bq +j )(bq; q) j+1 (q; q) j 1, ad s = 0, 1, 2,.... Propositio 5.1 The coefficiets A (s) give by (5.7) satisfy the basic relatios s i=0 B (s i) A (i) s+i = A(0) B (s). (5.8) Proof. Usig the explicit expressios for B (s) ad A (s) we ca rewrite the lhs of (5.8) i the form s i=0 B (s i) A (i) s+i = η sb (s) + ξ s+1 B (s 1) + κ (S 1 + ν S 2 ), (5.9) where κ = β(q 1)b s q (j+1)(s ) 1 (q ; q) s (q j ; q) s (q s ; q) j+1 (bq s ; q) j+1, (q; q) s (b 1 q j 2 ; q) s (1 q j 1 ) q +j (1 bq )(1 q s )Y j () ν = (1 q +j )(1 bq j+2 s )Y j ( 1), ad S 1, S 2 are the sums S 1 = S 2 = s i=0 s i=0 q i (q s ; q) i (bq j+2+1 s ; q) i (q j 1 ; q) i (q; q) i (q +1 s ; q) i (bq s ; q) i, q i (q 1 s ; q) i (bq j+2 s ; q) i (q j 1 ; q) i (q; q) i (q +1 s ; q) i (bq s ; q) i. These sums ca be evaluated usig the q-aalog of the Saalschütz formula [2]: S 1 = q (j+1)s (b 1 q j, q 1 j ; q) s (b 1 q 1, q ; q) s, S 2 = q (j+1)(s 1) (b 1 q 1 j, q j ; q) s 1 (b 1 q 2, q 1 ; q) s 1. 8

13 Relatio (5.8) ow becomes (η s λ )B (s) + ξ s+1 B (s 1) + κ (S 1 + ν S 2 ) = 0 (5.10) ad is see to be idetically satisfied. This proves the propositio. Note that A (s) = 0, if s j + 2. (5.11) Moreover, for s < j + 2 the coefficiets A (s) Q 2j+2 (q ; s) is a polyomial i q of degree 2j + 2. Hece we have have the form A (s) = q (j+1) Q 2j+2 (q ; s), where Propositio 5.2 The polyomials G(0){P (x; q j, b)} are the eigefuctios of a q-differece operator L q of order 2N = 2j + 2. We kow that the polyomials G(0){p (x; q j, b)} coicide with the polyomials p (x; q j 1, b; M) obtaied from the little q-jacobi polyomials by addig to the orthogoality measure a mass M at x = 0. We thus have equivaletly the followig Propositio 5.3 The polyomials p (x; q j, b; M) obtaied from the little q-jacobi polyomials by isertig a discrete mass at x = 0 i the orthogoality measure are the eigefuctios of a q- differece operator of order 2N = 2j The case of little q-laguerre polyomials The moic little q-laguerre polyomials [4] p (x; a) = ( 1) q ( 1)/2 (aq; q) 2 φ 1 ( q, 0 aq ) qx, (6.1) are obtaied from the little q-jacobi polyomials by settig b = 0. Hece, these polyomials also satisfy a q-differece equatio. Cosider the polyomials G(0){p (x; q j )}, obtaied from the little q-laguerre polyomials by the Geroimus trasformatio at x = 0. All formulas for these polyomials are obtaied from those for little q-jacobi polyomials by puttig b = 0. I particular, their coefficiets A (s) are easily obtaied from (5.7). We thus have Propositio 6.1 The polyomials G(0){p (x; q j )} are the eigefuctios of a q-differece operator of order 2N = 2j + 2. I this case, the polyomials G(0){p (x; q j )} coicide with polyomials p (x; q j 1 ; M) obtaied from the little q-laguerre polyomials by addig to the orthogoality measure a mass M at x = 0. Hece Propositio 6.2 The polyomials p (x; q j ; M) are the eigefuctios of a q-differece operator of order 2N = 2j + 4. Whe q 1 we get Koorwider s geeralized Laguerre polyomials [5] L (j;m) (x) whose measure differs from that of the ordiary Laguerre polyomials L (j) (x) by isertig a cocetrated mass M at the edpoit x = 0 of the orthogoality iterval (0, ). These polyomials are kow to satisfy a differetial equatio of order 2j + 4 [3]. 9

14 Refereces [1] T. Chihara, A Itroductio to Orthogoal Polyomials, Gordo ad Breach, NY, [2] G. Gasper ad M. Rahma, Basic hypergeometric series, Cambridge Uiversity Press, Cambridge, [3] J. Koekoek ad R. Koekoek, O a differetial equatio for Koorwider s geeralized Laguerre polyomials, Proc. Amer. Math. Soc. 112 (1991), [4] R. Koekoek ad R. F. Swarttouw 1994 The Askey scheme of hypergeometric orthogoal polyomials ad its q-aalogue, Report 94-05, Faculty of Techical Mathematics ad Iformatics, Delft Uiversity of techology. [5] T. H. Koorwider, Orthogoal polyomials with weight fuctio (1 x) α (1 + x) β + Mδ(x + 1) + Nδ(x 1) Ca.Math.Bull. 27, (1984), [6] A. Zhedaov, Ratioal spectral trasformatios ad orthogoal polyomials, J. Comput. ad Appl.Math. 85 (1997), [7] A. Zhedaov, A method of costructig Krall s polyomials, Preprit (1998). 10

Roger Apéry's proof that zeta(3) is irrational

Roger Apéry's proof that zeta(3) is irrational Cliff Bott cliffbott@hotmail.com 11 October 2011 Roger Apéry's proof that zeta(3) is irratioal Roger Apéry developed a method for searchig for cotiued fractio represetatios of umbers that have a form such

More information

Fibonacci numbers and orthogonal polynomials

Fibonacci numbers and orthogonal polynomials Fiboacci umbers ad orthogoal polyomials Christia Berg April 10, 2006 Abstract We prove that the sequece (1/F +2 0 of reciprocals of the Fiboacci umbers is a momet sequece of a certai discrete probability,

More information

Assignment 2 Solutions SOLUTION. ϕ 1 Â = 3 ϕ 1 4i ϕ 2. The other case can be dealt with in a similar way. { ϕ 2 Â} χ = { 4i ϕ 1 3 ϕ 2 } χ.

Assignment 2 Solutions SOLUTION. ϕ 1  = 3 ϕ 1 4i ϕ 2. The other case can be dealt with in a similar way. { ϕ 2 Â} χ = { 4i ϕ 1 3 ϕ 2 } χ. PHYSICS 34 QUANTUM PHYSICS II (25) Assigmet 2 Solutios 1. With respect to a pair of orthoormal vectors ϕ 1 ad ϕ 2 that spa the Hilbert space H of a certai system, the operator  is defied by its actio

More information

An Interpolation Process on Laguerre Polynomial

An Interpolation Process on Laguerre Polynomial Global Joural of Pure ad Applied Mathematics. ISSN 0973-1768 Volume 13, Number 10 (2017), pp. 7089-7099 Research Idia Publicatios http://www.ripublicatio.com A Iterpolatio Process o Laguerre Polyomial

More information

Sequences of Definite Integrals, Factorials and Double Factorials

Sequences of Definite Integrals, Factorials and Double Factorials 47 6 Joural of Iteger Sequeces, Vol. 8 (5), Article 5.4.6 Sequeces of Defiite Itegrals, Factorials ad Double Factorials Thierry Daa-Picard Departmet of Applied Mathematics Jerusalem College of Techology

More information

arxiv: v1 [math.fa] 3 Apr 2016

arxiv: v1 [math.fa] 3 Apr 2016 Aticommutator Norm Formula for Proectio Operators arxiv:164.699v1 math.fa] 3 Apr 16 Sam Walters Uiversity of Norther British Columbia ABSTRACT. We prove that for ay two proectio operators f, g o Hilbert

More information

Zeros of Polynomials

Zeros of Polynomials Math 160 www.timetodare.com 4.5 4.6 Zeros of Polyomials I these sectios we will study polyomials algebraically. Most of our work will be cocered with fidig the solutios of polyomial equatios of ay degree

More information

1. Hydrogen Atom: 3p State

1. Hydrogen Atom: 3p State 7633A QUANTUM MECHANICS I - solutio set - autum. Hydroge Atom: 3p State Let us assume that a hydroge atom is i a 3p state. Show that the radial part of its wave fuctio is r u 3(r) = 4 8 6 e r 3 r(6 r).

More information

Recurrence Relations

Recurrence Relations Recurrece Relatios Aalysis of recursive algorithms, such as: it factorial (it ) { if (==0) retur ; else retur ( * factorial(-)); } Let t be the umber of multiplicatios eeded to calculate factorial(). The

More information

SOME RELATIONS ON HERMITE MATRIX POLYNOMIALS. Levent Kargin and Veli Kurt

SOME RELATIONS ON HERMITE MATRIX POLYNOMIALS. Levent Kargin and Veli Kurt Mathematical ad Computatioal Applicatios, Vol. 18, No. 3, pp. 33-39, 013 SOME RELATIONS ON HERMITE MATRIX POLYNOMIALS Levet Kargi ad Veli Kurt Departmet of Mathematics, Faculty Sciece, Uiversity of Adeiz

More information

Comparison Study of Series Approximation. and Convergence between Chebyshev. and Legendre Series

Comparison Study of Series Approximation. and Convergence between Chebyshev. and Legendre Series Applied Mathematical Scieces, Vol. 7, 03, o. 6, 3-337 HIKARI Ltd, www.m-hikari.com http://d.doi.org/0.988/ams.03.3430 Compariso Study of Series Approimatio ad Covergece betwee Chebyshev ad Legedre Series

More information

DETERMINATION OF MECHANICAL PROPERTIES OF A NON- UNIFORM BEAM USING THE MEASUREMENT OF THE EXCITED LONGITUDINAL ELASTIC VIBRATIONS.

DETERMINATION OF MECHANICAL PROPERTIES OF A NON- UNIFORM BEAM USING THE MEASUREMENT OF THE EXCITED LONGITUDINAL ELASTIC VIBRATIONS. ICSV4 Cairs Australia 9- July 7 DTRMINATION OF MCHANICAL PROPRTIS OF A NON- UNIFORM BAM USING TH MASURMNT OF TH XCITD LONGITUDINAL LASTIC VIBRATIONS Pavel Aokhi ad Vladimir Gordo Departmet of the mathematics

More information

The log-behavior of n p(n) and n p(n)/n

The log-behavior of n p(n) and n p(n)/n Ramauja J. 44 017, 81-99 The log-behavior of p ad p/ William Y.C. Che 1 ad Ke Y. Zheg 1 Ceter for Applied Mathematics Tiaji Uiversity Tiaji 0007, P. R. Chia Ceter for Combiatorics, LPMC Nakai Uivercity

More information

Subject: Differential Equations & Mathematical Modeling-III

Subject: Differential Equations & Mathematical Modeling-III Power Series Solutios of Differetial Equatios about Sigular poits Subject: Differetial Equatios & Mathematical Modelig-III Lesso: Power series solutios of differetial equatios about Sigular poits Lesso

More information

Taylor polynomial solution of difference equation with constant coefficients via time scales calculus

Taylor polynomial solution of difference equation with constant coefficients via time scales calculus TMSCI 3, o 3, 129-135 (2015) 129 ew Treds i Mathematical Scieces http://wwwtmscicom Taylor polyomial solutio of differece equatio with costat coefficiets via time scales calculus Veysel Fuat Hatipoglu

More information

Random Models. Tusheng Zhang. February 14, 2013

Random Models. Tusheng Zhang. February 14, 2013 Radom Models Tusheg Zhag February 14, 013 1 Radom Walks Let me describe the model. Radom walks are used to describe the motio of a movig particle (object). Suppose that a particle (object) moves alog the

More information

arxiv: v3 [math.ca] 25 Nov 2010

arxiv: v3 [math.ca] 25 Nov 2010 A LIMIT q = 1 FOR THE BIG Q-JACOBI POLYNOMIALS arxiv:1011.149v3 [math.ca] 5 Nov 010 LUC VINET AND ALEXEI ZHEDANOV Abstract. We study a ew family of classical orthogoal polyomials, here called big -1 Jacobi

More information

We are mainly going to be concerned with power series in x, such as. (x)} converges - that is, lims N n

We are mainly going to be concerned with power series in x, such as. (x)} converges - that is, lims N n Review of Power Series, Power Series Solutios A power series i x - a is a ifiite series of the form c (x a) =c +c (x a)+(x a) +... We also call this a power series cetered at a. Ex. (x+) is cetered at

More information

k-generalized FIBONACCI NUMBERS CLOSE TO THE FORM 2 a + 3 b + 5 c 1. Introduction

k-generalized FIBONACCI NUMBERS CLOSE TO THE FORM 2 a + 3 b + 5 c 1. Introduction Acta Math. Uiv. Comeiaae Vol. LXXXVI, 2 (2017), pp. 279 286 279 k-generalized FIBONACCI NUMBERS CLOSE TO THE FORM 2 a + 3 b + 5 c N. IRMAK ad M. ALP Abstract. The k-geeralized Fiboacci sequece { F (k)

More information

62. Power series Definition 16. (Power series) Given a sequence {c n }, the series. c n x n = c 0 + c 1 x + c 2 x 2 + c 3 x 3 +

62. Power series Definition 16. (Power series) Given a sequence {c n }, the series. c n x n = c 0 + c 1 x + c 2 x 2 + c 3 x 3 + 62. Power series Defiitio 16. (Power series) Give a sequece {c }, the series c x = c 0 + c 1 x + c 2 x 2 + c 3 x 3 + is called a power series i the variable x. The umbers c are called the coefficiets of

More information

ECE-S352 Introduction to Digital Signal Processing Lecture 3A Direct Solution of Difference Equations

ECE-S352 Introduction to Digital Signal Processing Lecture 3A Direct Solution of Difference Equations ECE-S352 Itroductio to Digital Sigal Processig Lecture 3A Direct Solutio of Differece Equatios Discrete Time Systems Described by Differece Equatios Uit impulse (sample) respose h() of a DT system allows

More information

-ORDER CONVERGENCE FOR FINDING SIMPLE ROOT OF A POLYNOMIAL EQUATION

-ORDER CONVERGENCE FOR FINDING SIMPLE ROOT OF A POLYNOMIAL EQUATION NEW NEWTON-TYPE METHOD WITH k -ORDER CONVERGENCE FOR FINDING SIMPLE ROOT OF A POLYNOMIAL EQUATION R. Thukral Padé Research Cetre, 39 Deaswood Hill, Leeds West Yorkshire, LS7 JS, ENGLAND ABSTRACT The objective

More information

3. Z Transform. Recall that the Fourier transform (FT) of a DT signal xn [ ] is ( ) [ ] = In order for the FT to exist in the finite magnitude sense,

3. Z Transform. Recall that the Fourier transform (FT) of a DT signal xn [ ] is ( ) [ ] = In order for the FT to exist in the finite magnitude sense, 3. Z Trasform Referece: Etire Chapter 3 of text. Recall that the Fourier trasform (FT) of a DT sigal x [ ] is ω ( ) [ ] X e = j jω k = xe I order for the FT to exist i the fiite magitude sese, S = x [

More information

A Note On The Exponential Of A Matrix Whose Elements Are All 1

A Note On The Exponential Of A Matrix Whose Elements Are All 1 Applied Mathematics E-Notes, 8(208), 92-99 c ISSN 607-250 Available free at mirror sites of http://wwwmaththuedutw/ ame/ A Note O The Expoetial Of A Matrix Whose Elemets Are All Reza Farhadia Received

More information

Algebra of Least Squares

Algebra of Least Squares October 19, 2018 Algebra of Least Squares Geometry of Least Squares Recall that out data is like a table [Y X] where Y collects observatios o the depedet variable Y ad X collects observatios o the k-dimesioal

More information

Some properties of Boubaker polynomials and applications

Some properties of Boubaker polynomials and applications Some properties of Boubaker polyomials ad applicatios Gradimir V. Milovaović ad Duša Joksimović Citatio: AIP Cof. Proc. 179, 1050 (2012); doi: 10.1063/1.756326 View olie: http://dx.doi.org/10.1063/1.756326

More information

Some remarks for codes and lattices over imaginary quadratic

Some remarks for codes and lattices over imaginary quadratic Some remarks for codes ad lattices over imagiary quadratic fields Toy Shaska Oaklad Uiversity, Rochester, MI, USA. Caleb Shor Wester New Eglad Uiversity, Sprigfield, MA, USA. shaska@oaklad.edu Abstract

More information

The Riemann Zeta Function

The Riemann Zeta Function Physics 6A Witer 6 The Riema Zeta Fuctio I this ote, I will sketch some of the mai properties of the Riema zeta fuctio, ζ(x). For x >, we defie ζ(x) =, x >. () x = For x, this sum diverges. However, we

More information

SOLUTIONS TO EXAM 3. Solution: Note that this defines two convergent geometric series with respective radii r 1 = 2/5 < 1 and r 2 = 1/5 < 1.

SOLUTIONS TO EXAM 3. Solution: Note that this defines two convergent geometric series with respective radii r 1 = 2/5 < 1 and r 2 = 1/5 < 1. SOLUTIONS TO EXAM 3 Problem Fid the sum of the followig series 2 + ( ) 5 5 2 5 3 25 2 2 This series diverges Solutio: Note that this defies two coverget geometric series with respective radii r 2/5 < ad

More information

Some families of generating functions for the multiple orthogonal polynomials associated with modified Bessel K-functions

Some families of generating functions for the multiple orthogonal polynomials associated with modified Bessel K-functions J. Math. Aal. Appl. 297 2004 186 193 www.elsevier.com/locate/jmaa Some families of geeratig fuctios for the multiple orthogoal polyomials associated with modified Bessel K-fuctios M.A. Özarsla, A. Altı

More information

A note on the p-adic gamma function and q-changhee polynomials

A note on the p-adic gamma function and q-changhee polynomials Available olie at wwwisr-publicatioscom/jmcs J Math Computer Sci, 18 (2018, 11 17 Research Article Joural Homepage: wwwtjmcscom - wwwisr-publicatioscom/jmcs A ote o the p-adic gamma fuctio ad q-chaghee

More information

Inverse Nodal Problems for Differential Equation on the Half-line

Inverse Nodal Problems for Differential Equation on the Half-line Australia Joural of Basic ad Applied Scieces, 3(4): 4498-4502, 2009 ISSN 1991-8178 Iverse Nodal Problems for Differetial Equatio o the Half-lie 1 2 3 A. Dabbaghia, A. Nematy ad Sh. Akbarpoor 1 Islamic

More information

SOLUTION SET VI FOR FALL [(n + 2)(n + 1)a n+2 a n 1 ]x n = 0,

SOLUTION SET VI FOR FALL [(n + 2)(n + 1)a n+2 a n 1 ]x n = 0, 4. Series Solutios of Differetial Equatios:Special Fuctios 4.. Illustrative examples.. 5. Obtai the geeral solutio of each of the followig differetial equatios i terms of Maclauri series: d y (a dx = xy,

More information

Physics 324, Fall Dirac Notation. These notes were produced by David Kaplan for Phys. 324 in Autumn 2001.

Physics 324, Fall Dirac Notation. These notes were produced by David Kaplan for Phys. 324 in Autumn 2001. Physics 324, Fall 2002 Dirac Notatio These otes were produced by David Kapla for Phys. 324 i Autum 2001. 1 Vectors 1.1 Ier product Recall from liear algebra: we ca represet a vector V as a colum vector;

More information

AMS Mathematics Subject Classification : 40A05, 40A99, 42A10. Key words and phrases : Harmonic series, Fourier series. 1.

AMS Mathematics Subject Classification : 40A05, 40A99, 42A10. Key words and phrases : Harmonic series, Fourier series. 1. J. Appl. Math. & Computig Vol. x 00y), No. z, pp. A RECURSION FOR ALERNAING HARMONIC SERIES ÁRPÁD BÉNYI Abstract. We preset a coveiet recursive formula for the sums of alteratig harmoic series of odd order.

More information

Factors of alternating sums of products of binomial and q-binomial coefficients

Factors of alternating sums of products of binomial and q-binomial coefficients ACTA ARITHMETICA 1271 (2007 Factors of alteratig sums of products of biomial ad q-biomial coefficiets by Victor J W Guo (Shaghai Frédéric Jouhet (Lyo ad Jiag Zeg (Lyo 1 Itroductio I 1998 Cali [4 proved

More information

Math 155 (Lecture 3)

Math 155 (Lecture 3) Math 55 (Lecture 3) September 8, I this lecture, we ll cosider the aswer to oe of the most basic coutig problems i combiatorics Questio How may ways are there to choose a -elemet subset of the set {,,,

More information

MAT1026 Calculus II Basic Convergence Tests for Series

MAT1026 Calculus II Basic Convergence Tests for Series MAT026 Calculus II Basic Covergece Tests for Series Egi MERMUT 202.03.08 Dokuz Eylül Uiversity Faculty of Sciece Departmet of Mathematics İzmir/TURKEY Cotets Mootoe Covergece Theorem 2 2 Series of Real

More information

Subject: Differential Equations & Mathematical Modeling -III. Lesson: Power series solutions of Differential Equations. about ordinary points

Subject: Differential Equations & Mathematical Modeling -III. Lesson: Power series solutions of Differential Equations. about ordinary points Power series solutio of Differetial equatios about ordiary poits Subject: Differetial Equatios & Mathematical Modelig -III Lesso: Power series solutios of Differetial Equatios about ordiary poits Lesso

More information

Math 104: Homework 2 solutions

Math 104: Homework 2 solutions Math 04: Homework solutios. A (0, ): Sice this is a ope iterval, the miimum is udefied, ad sice the set is ot bouded above, the maximum is also udefied. if A 0 ad sup A. B { m + : m, N}: This set does

More information

SOME NEW IDENTITIES INVOLVING π,

SOME NEW IDENTITIES INVOLVING π, SOME NEW IDENTITIES INVOLVING π, HENG HUAT CHAN π AND π. Itroductio The umber π, as we all ow, is defied to be the legth of a circle of diameter. The first few estimates of π were 3 Egypt aroud 9 B.C.,

More information

3.2 Properties of Division 3.3 Zeros of Polynomials 3.4 Complex and Rational Zeros of Polynomials

3.2 Properties of Division 3.3 Zeros of Polynomials 3.4 Complex and Rational Zeros of Polynomials Math 60 www.timetodare.com 3. Properties of Divisio 3.3 Zeros of Polyomials 3.4 Complex ad Ratioal Zeros of Polyomials I these sectios we will study polyomials algebraically. Most of our work will be cocered

More information

ON THE LEHMER CONSTANT OF FINITE CYCLIC GROUPS

ON THE LEHMER CONSTANT OF FINITE CYCLIC GROUPS ON THE LEHMER CONSTANT OF FINITE CYCLIC GROUPS NORBERT KAIBLINGER Abstract. Results of Lid o Lehmer s problem iclude the value of the Lehmer costat of the fiite cyclic group Z/Z, for 5 ad all odd. By complemetary

More information

PROBLEM SET 5 SOLUTIONS 126 = , 37 = , 15 = , 7 = 7 1.

PROBLEM SET 5 SOLUTIONS 126 = , 37 = , 15 = , 7 = 7 1. Math 7 Sprig 06 PROBLEM SET 5 SOLUTIONS Notatios. Give a real umber x, we will defie sequeces (a k ), (x k ), (p k ), (q k ) as i lecture.. (a) (5 pts) Fid the simple cotiued fractio represetatios of 6

More information

Chapter 4. Fourier Series

Chapter 4. Fourier Series Chapter 4. Fourier Series At this poit we are ready to ow cosider the caoical equatios. Cosider, for eample the heat equatio u t = u, < (4.) subject to u(, ) = si, u(, t) = u(, t) =. (4.) Here,

More information

Harmonic Number Identities Via Euler s Transform

Harmonic Number Identities Via Euler s Transform 1 2 3 47 6 23 11 Joural of Iteger Sequeces, Vol. 12 2009), Article 09.6.1 Harmoic Number Idetities Via Euler s Trasform Khristo N. Boyadzhiev Departmet of Mathematics Ohio Norther Uiversity Ada, Ohio 45810

More information

NEW FAST CONVERGENT SEQUENCES OF EULER-MASCHERONI TYPE

NEW FAST CONVERGENT SEQUENCES OF EULER-MASCHERONI TYPE UPB Sci Bull, Series A, Vol 79, Iss, 207 ISSN 22-7027 NEW FAST CONVERGENT SEQUENCES OF EULER-MASCHERONI TYPE Gabriel Bercu We itroduce two ew sequeces of Euler-Mascheroi type which have fast covergece

More information

On the Krall-type discrete polynomials

On the Krall-type discrete polynomials O the Krall-type discrete polyomials R. Álvarez-Nodarse 1 ad J. Petroilho 2 1 Departameto de Aálisis Matemático, Uiversidad de Sevilla. Apdo. 1160, E-41080 Sevilla, Spai ad Istituto Carlos I de Física

More information

Enumerative & Asymptotic Combinatorics

Enumerative & Asymptotic Combinatorics C50 Eumerative & Asymptotic Combiatorics Stirlig ad Lagrage Sprig 2003 This sectio of the otes cotais proofs of Stirlig s formula ad the Lagrage Iversio Formula. Stirlig s formula Theorem 1 (Stirlig s

More information

TEACHER CERTIFICATION STUDY GUIDE

TEACHER CERTIFICATION STUDY GUIDE COMPETENCY 1. ALGEBRA SKILL 1.1 1.1a. ALGEBRAIC STRUCTURES Kow why the real ad complex umbers are each a field, ad that particular rigs are ot fields (e.g., itegers, polyomial rigs, matrix rigs) Algebra

More information

6.3 Testing Series With Positive Terms

6.3 Testing Series With Positive Terms 6.3. TESTING SERIES WITH POSITIVE TERMS 307 6.3 Testig Series With Positive Terms 6.3. Review of what is kow up to ow I theory, testig a series a i for covergece amouts to fidig the i= sequece of partial

More information

Generating Functions for Laguerre Type Polynomials. Group Theoretic method

Generating Functions for Laguerre Type Polynomials. Group Theoretic method It. Joural of Math. Aalysis, Vol. 4, 2010, o. 48, 257-266 Geeratig Fuctios for Laguerre Type Polyomials α of Two Variables L ( xy, ) by Usig Group Theoretic method Ajay K. Shula* ad Sriata K. Meher** *Departmet

More information

NICK DUFRESNE. 1 1 p(x). To determine some formulas for the generating function of the Schröder numbers, r(x) = a(x) =

NICK DUFRESNE. 1 1 p(x). To determine some formulas for the generating function of the Schröder numbers, r(x) = a(x) = AN INTRODUCTION TO SCHRÖDER AND UNKNOWN NUMBERS NICK DUFRESNE Abstract. I this article we will itroduce two types of lattice paths, Schröder paths ad Ukow paths. We will examie differet properties of each,

More information

1 Generating functions for balls in boxes

1 Generating functions for balls in boxes Math 566 Fall 05 Some otes o geeratig fuctios Give a sequece a 0, a, a,..., a,..., a geeratig fuctio some way of represetig the sequece as a fuctio. There are may ways to do this, with the most commo ways

More information

subcaptionfont+=small,labelformat=parens,labelsep=space,skip=6pt,list=0,hypcap=0 subcaption ALGEBRAIC COMBINATORICS LECTURE 8 TUESDAY, 2/16/2016

subcaptionfont+=small,labelformat=parens,labelsep=space,skip=6pt,list=0,hypcap=0 subcaption ALGEBRAIC COMBINATORICS LECTURE 8 TUESDAY, 2/16/2016 subcaptiofot+=small,labelformat=pares,labelsep=space,skip=6pt,list=0,hypcap=0 subcaptio ALGEBRAIC COMBINATORICS LECTURE 8 TUESDAY, /6/06. Self-cojugate Partitios Recall that, give a partitio λ, we may

More information

Ma 530 Introduction to Power Series

Ma 530 Introduction to Power Series Ma 530 Itroductio to Power Series Please ote that there is material o power series at Visual Calculus. Some of this material was used as part of the presetatio of the topics that follow. What is a Power

More information

Find quadratic function which pass through the following points (0,1),(1,1),(2, 3)... 11

Find quadratic function which pass through the following points (0,1),(1,1),(2, 3)... 11 Adrew Powuk - http://www.powuk.com- Math 49 (Numerical Aalysis) Iterpolatio... 4. Polyomial iterpolatio (system of equatio)... 4.. Lier iterpolatio... 5... Fid a lie which pass through (,) (,)... 8...

More information

Discrete Orthogonal Moment Features Using Chebyshev Polynomials

Discrete Orthogonal Moment Features Using Chebyshev Polynomials Discrete Orthogoal Momet Features Usig Chebyshev Polyomials R. Mukuda, 1 S.H.Og ad P.A. Lee 3 1 Faculty of Iformatio Sciece ad Techology, Multimedia Uiversity 75450 Malacca, Malaysia. Istitute of Mathematical

More information

1 1 2 = show that: over variables x and y. [2 marks] Write down necessary conditions involving first and second-order partial derivatives for ( x0, y

1 1 2 = show that: over variables x and y. [2 marks] Write down necessary conditions involving first and second-order partial derivatives for ( x0, y Questio (a) A square matrix A= A is called positive defiite if the quadratic form waw > 0 for every o-zero vector w [Note: Here (.) deotes the traspose of a matrix or a vector]. Let 0 A = 0 = show that:

More information

arxiv: v1 [cs.sc] 2 Jan 2018

arxiv: v1 [cs.sc] 2 Jan 2018 Computig the Iverse Melli Trasform of Holoomic Sequeces usig Kovacic s Algorithm arxiv:8.9v [cs.sc] 2 Ja 28 Research Istitute for Symbolic Computatio RISC) Johaes Kepler Uiversity Liz, Alteberger Straße

More information

REGULARIZATION OF CERTAIN DIVERGENT SERIES OF POLYNOMIALS

REGULARIZATION OF CERTAIN DIVERGENT SERIES OF POLYNOMIALS REGULARIZATION OF CERTAIN DIVERGENT SERIES OF POLYNOMIALS LIVIU I. NICOLAESCU ABSTRACT. We ivestigate the geeralized covergece ad sums of series of the form P at P (x, where P R[x], a R,, ad T : R[x] R[x]

More information

A Note on the Symmetric Powers of the Standard Representation of S n

A Note on the Symmetric Powers of the Standard Representation of S n A Note o the Symmetric Powers of the Stadard Represetatio of S David Savitt 1 Departmet of Mathematics, Harvard Uiversity Cambridge, MA 0138, USA dsavitt@mathharvardedu Richard P Staley Departmet of Mathematics,

More information

Weighted Approximation by Videnskii and Lupas Operators

Weighted Approximation by Videnskii and Lupas Operators Weighted Approximatio by Videsii ad Lupas Operators Aif Barbaros Dime İstabul Uiversity Departmet of Egieerig Sciece April 5, 013 Aif Barbaros Dime İstabul Uiversity Departmet Weightedof Approximatio Egieerig

More information

Math 61CM - Solutions to homework 3

Math 61CM - Solutions to homework 3 Math 6CM - Solutios to homework 3 Cédric De Groote October 2 th, 208 Problem : Let F be a field, m 0 a fixed oegative iteger ad let V = {a 0 + a x + + a m x m a 0,, a m F} be the vector space cosistig

More information

ON SOLVING A FORMAL HYPERBOLIC PARTIAL DIFFERENTIAL EQUATION IN THE COMPLEX FIELD

ON SOLVING A FORMAL HYPERBOLIC PARTIAL DIFFERENTIAL EQUATION IN THE COMPLEX FIELD A. Şt. Uiv. Ovidius Costaţa Vol. (), 003, 69 78 ON SOLVING A FORMAL HYPERBOLIC PARTIAL DIFFERENTIAL EQUATION IN THE COMPLEX FIELD Nicolae Popoviciu To Professor Silviu Sburla, at his 60 s aiversary Abstract

More information

Chapter 8. Euler s Gamma function

Chapter 8. Euler s Gamma function Chapter 8 Euler s Gamma fuctio The Gamma fuctio plays a importat role i the fuctioal equatio for ζ(s that we will derive i the ext chapter. I the preset chapter we have collected some properties of the

More information

6. Uniform distribution mod 1

6. Uniform distribution mod 1 6. Uiform distributio mod 1 6.1 Uiform distributio ad Weyl s criterio Let x be a seuece of real umbers. We may decompose x as the sum of its iteger part [x ] = sup{m Z m x } (i.e. the largest iteger which

More information

ENGI Series Page 6-01

ENGI Series Page 6-01 ENGI 3425 6 Series Page 6-01 6. Series Cotets: 6.01 Sequeces; geeral term, limits, covergece 6.02 Series; summatio otatio, covergece, divergece test 6.03 Stadard Series; telescopig series, geometric series,

More information

w (1) ˆx w (1) x (1) /ρ and w (2) ˆx w (2) x (2) /ρ.

w (1) ˆx w (1) x (1) /ρ and w (2) ˆx w (2) x (2) /ρ. 2 5. Weighted umber of late jobs 5.1. Release dates ad due dates: maximimizig the weight of o-time jobs Oce we add release dates, miimizig the umber of late jobs becomes a sigificatly harder problem. For

More information

arxiv: v1 [math.nt] 16 Nov 2009

arxiv: v1 [math.nt] 16 Nov 2009 Complete Bell polyomials ad ew geeralized idetities for polyomials of higher order arxiv:0911.3069v1 math.nt] 16 Nov 2009 Boris Rubistei, Stowers Istitute for Medical Research 1000 50th St., Kasas City,

More information

Lesson 10: Limits and Continuity

Lesson 10: Limits and Continuity www.scimsacademy.com Lesso 10: Limits ad Cotiuity SCIMS Academy 1 Limit of a fuctio The cocept of limit of a fuctio is cetral to all other cocepts i calculus (like cotiuity, derivative, defiite itegrals

More information

You may work in pairs or purely individually for this assignment.

You may work in pairs or purely individually for this assignment. CS 04 Problem Solvig i Computer Sciece OOC Assigmet 6: Recurreces You may work i pairs or purely idividually for this assigmet. Prepare your aswers to the followig questios i a plai ASCII text file or

More information

PLEASE MARK YOUR ANSWERS WITH AN X, not a circle! 1. (a) (b) (c) (d) (e) 3. (a) (b) (c) (d) (e) 5. (a) (b) (c) (d) (e) 7. (a) (b) (c) (d) (e)

PLEASE MARK YOUR ANSWERS WITH AN X, not a circle! 1. (a) (b) (c) (d) (e) 3. (a) (b) (c) (d) (e) 5. (a) (b) (c) (d) (e) 7. (a) (b) (c) (d) (e) Math 0560, Exam 3 November 6, 07 The Hoor Code is i effect for this examiatio. All work is to be your ow. No calculators. The exam lasts for hour ad 5 mi. Be sure that your ame is o every page i case pages

More information

CHAPTER 10 INFINITE SEQUENCES AND SERIES

CHAPTER 10 INFINITE SEQUENCES AND SERIES CHAPTER 10 INFINITE SEQUENCES AND SERIES 10.1 Sequeces 10.2 Ifiite Series 10.3 The Itegral Tests 10.4 Compariso Tests 10.5 The Ratio ad Root Tests 10.6 Alteratig Series: Absolute ad Coditioal Covergece

More information

Appendix K. The three-point correlation function (bispectrum) of density peaks

Appendix K. The three-point correlation function (bispectrum) of density peaks Appedix K The three-poit correlatio fuctio (bispectrum) of desity peaks Cosider the smoothed desity field, ρ (x) ρ [ δ (x)], with a geeral smoothig kerel W (x) δ (x) d yw (x y)δ(y). (K.) We defie the peaks

More information

Benaissa Bernoussi Université Abdelmalek Essaadi, ENSAT de Tanger, B.P. 416, Tanger, Morocco

Benaissa Bernoussi Université Abdelmalek Essaadi, ENSAT de Tanger, B.P. 416, Tanger, Morocco EXTENDING THE BERNOULLI-EULER METHOD FOR FINDING ZEROS OF HOLOMORPHIC FUNCTIONS Beaissa Beroussi Uiversité Abdelmalek Essaadi, ENSAT de Tager, B.P. 416, Tager, Morocco e-mail: Beaissa@fstt.ac.ma Mustapha

More information

ANOTHER GENERALIZED FIBONACCI SEQUENCE 1. INTRODUCTION

ANOTHER GENERALIZED FIBONACCI SEQUENCE 1. INTRODUCTION ANOTHER GENERALIZED FIBONACCI SEQUENCE MARCELLUS E. WADDILL A N D LOUIS SACKS Wake Forest College, Wisto Salem, N. C., ad Uiversity of ittsburgh, ittsburgh, a. 1. INTRODUCTION Recet issues of umerous periodicals

More information

CHAPTER 5. Theory and Solution Using Matrix Techniques

CHAPTER 5. Theory and Solution Using Matrix Techniques A SERIES OF CLASS NOTES FOR 2005-2006 TO INTRODUCE LINEAR AND NONLINEAR PROBLEMS TO ENGINEERS, SCIENTISTS, AND APPLIED MATHEMATICIANS DE CLASS NOTES 3 A COLLECTION OF HANDOUTS ON SYSTEMS OF ORDINARY DIFFERENTIAL

More information

Polynomials with Rational Roots that Differ by a Non-zero Constant. Generalities

Polynomials with Rational Roots that Differ by a Non-zero Constant. Generalities Polyomials with Ratioal Roots that Differ by a No-zero Costat Philip Gibbs The problem of fidig two polyomials P(x) ad Q(x) of a give degree i a sigle variable x that have all ratioal roots ad differ by

More information

Vienna, Austria α n (1 x 2 ) n (x)

Vienna, Austria  α n (1 x 2 ) n (x) ON TURÁN S INEQUALITY FOR LEGENDRE POLYNOMIALS HORST ALZER a, STEFAN GERHOLD b, MANUEL KAUERS c2, ALEXANDRU LUPAŞ d a Morsbacher Str. 0, 5545 Waldbröl, Germay alzerhorst@freeet.de b Christia Doppler Laboratory

More information

Linear regression. Daniel Hsu (COMS 4771) (y i x T i β)2 2πσ. 2 2σ 2. 1 n. (x T i β y i ) 2. 1 ˆβ arg min. β R n d

Linear regression. Daniel Hsu (COMS 4771) (y i x T i β)2 2πσ. 2 2σ 2. 1 n. (x T i β y i ) 2. 1 ˆβ arg min. β R n d Liear regressio Daiel Hsu (COMS 477) Maximum likelihood estimatio Oe of the simplest liear regressio models is the followig: (X, Y ),..., (X, Y ), (X, Y ) are iid radom pairs takig values i R d R, ad Y

More information

Modified Decomposition Method by Adomian and. Rach for Solving Nonlinear Volterra Integro- Differential Equations

Modified Decomposition Method by Adomian and. Rach for Solving Nonlinear Volterra Integro- Differential Equations Noliear Aalysis ad Differetial Equatios, Vol. 5, 27, o. 4, 57-7 HIKARI Ltd, www.m-hikari.com https://doi.org/.2988/ade.27.62 Modified Decompositio Method by Adomia ad Rach for Solvig Noliear Volterra Itegro-

More information

Marcinkiwiecz-Zygmund Type Inequalities for all Arcs of the Circle

Marcinkiwiecz-Zygmund Type Inequalities for all Arcs of the Circle Marcikiwiecz-ygmud Type Iequalities for all Arcs of the Circle C.K. Kobidarajah ad D. S. Lubisky Mathematics Departmet, Easter Uiversity, Chekalady, Sri Laka; Mathematics Departmet, Georgia Istitute of

More information

Polynomial Functions and Their Graphs

Polynomial Functions and Their Graphs Polyomial Fuctios ad Their Graphs I this sectio we begi the study of fuctios defied by polyomial expressios. Polyomial ad ratioal fuctios are the most commo fuctios used to model data, ad are used extesively

More information

METHOD OF FUNDAMENTAL SOLUTIONS FOR HELMHOLTZ EIGENVALUE PROBLEMS IN ELLIPTICAL DOMAINS

METHOD OF FUNDAMENTAL SOLUTIONS FOR HELMHOLTZ EIGENVALUE PROBLEMS IN ELLIPTICAL DOMAINS Please cite this article as: Staisław Kula, Method of fudametal solutios for Helmholtz eigevalue problems i elliptical domais, Scietific Research of the Istitute of Mathematics ad Computer Sciece, 009,

More information

GENERALIZED HARMONIC NUMBER IDENTITIES AND A RELATED MATRIX REPRESENTATION

GENERALIZED HARMONIC NUMBER IDENTITIES AND A RELATED MATRIX REPRESENTATION J Korea Math Soc 44 (2007), No 2, pp 487 498 GENERALIZED HARMONIC NUMBER IDENTITIES AND A RELATED MATRIX REPRESENTATION Gi-Sag Cheo ad Moawwad E A El-Miawy Reprited from the Joural of the Korea Mathematical

More information

TR/46 OCTOBER THE ZEROS OF PARTIAL SUMS OF A MACLAURIN EXPANSION A. TALBOT

TR/46 OCTOBER THE ZEROS OF PARTIAL SUMS OF A MACLAURIN EXPANSION A. TALBOT TR/46 OCTOBER 974 THE ZEROS OF PARTIAL SUMS OF A MACLAURIN EXPANSION by A. TALBOT .. Itroductio. A problem i approximatio theory o which I have recetly worked [] required for its solutio a proof that the

More information

Factors of sums and alternating sums involving binomial coefficients and powers of integers

Factors of sums and alternating sums involving binomial coefficients and powers of integers Factors of sums ad alteratig sums ivolvig biomial coefficiets ad powers of itegers Victor J. W. Guo 1 ad Jiag Zeg 2 1 Departmet of Mathematics East Chia Normal Uiversity Shaghai 200062 People s Republic

More information

Riesz-Fischer Sequences and Lower Frame Bounds

Riesz-Fischer Sequences and Lower Frame Bounds Zeitschrift für Aalysis ud ihre Aweduge Joural for Aalysis ad its Applicatios Volume 1 (00), No., 305 314 Riesz-Fischer Sequeces ad Lower Frame Bouds P. Casazza, O. Christese, S. Li ad A. Lider Abstract.

More information

Lecture Notes for CS 313H, Fall 2011

Lecture Notes for CS 313H, Fall 2011 Lecture Notes for CS 313H, Fall 011 August 5. We start by examiig triagular umbers: T () = 1 + + + ( = 0, 1,,...). Triagular umbers ca be also defied recursively: T (0) = 0, T ( + 1) = T () + + 1, or usig

More information

KU Leuven Department of Computer Science

KU Leuven Department of Computer Science O orthogoal polyomials related to arithmetic ad harmoic sequeces Adhemar Bultheel ad Adreas Lasarow Report TW 687, February 208 KU Leuve Departmet of Computer Sciece Celestijelaa 200A B-300 Heverlee (Belgium)

More information

Linear Regression Demystified

Linear Regression Demystified Liear Regressio Demystified Liear regressio is a importat subject i statistics. I elemetary statistics courses, formulae related to liear regressio are ofte stated without derivatio. This ote iteds to

More information

A NOTE ON BOUNDARY BLOW-UP PROBLEM OF u = u p

A NOTE ON BOUNDARY BLOW-UP PROBLEM OF u = u p A NOTE ON BOUNDARY BLOW-UP PROBLEM OF u = u p SEICK KIM Abstract. Assume that Ω is a bouded domai i R with 2. We study positive solutios to the problem, u = u p i Ω, u(x) as x Ω, where p > 1. Such solutios

More information

Sequences and Limits

Sequences and Limits Chapter Sequeces ad Limits Let { a } be a sequece of real or complex umbers A ecessary ad sufficiet coditio for the sequece to coverge is that for ay ɛ > 0 there exists a iteger N > 0 such that a p a q

More information

Enumerative & Asymptotic Combinatorics

Enumerative & Asymptotic Combinatorics C50 Eumerative & Asymptotic Combiatorics Notes 4 Sprig 2003 Much of the eumerative combiatorics of sets ad fuctios ca be geeralised i a maer which, at first sight, seems a bit umotivated I this chapter,

More information

MATH 324 Summer 2006 Elementary Number Theory Solutions to Assignment 2 Due: Thursday July 27, 2006

MATH 324 Summer 2006 Elementary Number Theory Solutions to Assignment 2 Due: Thursday July 27, 2006 MATH 34 Summer 006 Elemetary Number Theory Solutios to Assigmet Due: Thursday July 7, 006 Departmet of Mathematical ad Statistical Scieces Uiversity of Alberta Questio [p 74 #6] Show that o iteger of the

More information

1 6 = 1 6 = + Factorials and Euler s Gamma function

1 6 = 1 6 = + Factorials and Euler s Gamma function Royal Holloway Uiversity of Lodo Departmet of Physics Factorials ad Euler s Gamma fuctio Itroductio The is a self-cotaied part of the course dealig, essetially, with the factorial fuctio ad its geeralizatio

More information

PAijpam.eu ON DERIVATION OF RATIONAL SOLUTIONS OF BABBAGE S FUNCTIONAL EQUATION

PAijpam.eu ON DERIVATION OF RATIONAL SOLUTIONS OF BABBAGE S FUNCTIONAL EQUATION Iteratioal Joural of Pure ad Applied Mathematics Volume 94 No. 204, 9-20 ISSN: 3-8080 (prited versio); ISSN: 34-3395 (o-lie versio) url: http://www.ijpam.eu doi: http://dx.doi.org/0.2732/ijpam.v94i.2 PAijpam.eu

More information

A CONTINUED FRACTION EXPANSION FOR A q-tangent FUNCTION

A CONTINUED FRACTION EXPANSION FOR A q-tangent FUNCTION Sémiaire Lotharigie de Combiatoire 45 001, Article B45b A CONTINUED FRACTION EXPANSION FOR A q-tangent FUNCTION MARKUS FULMEK Abstract. We prove a cotiued fractio expasio for a certai q taget fuctio that

More information

Numerical Method for Blasius Equation on an infinite Interval

Numerical Method for Blasius Equation on an infinite Interval Numerical Method for Blasius Equatio o a ifiite Iterval Alexader I. Zadori Omsk departmet of Sobolev Mathematics Istitute of Siberia Brach of Russia Academy of Scieces, Russia zadori@iitam.omsk.et.ru 1

More information