Goncarov-Type Polynomials and Applications in Combinatorics

Size: px
Start display at page:

Download "Goncarov-Type Polynomials and Applications in Combinatorics"

Transcription

1 Goncarov-Type Polynomals and Applcatons n Combnatorcs Joseph P.S. Kung 1, Xnyu Sun 2, and Catherne Yan 3,4 1 Department of Mathematcs, Unversty of North Texas, Denton, TX ,3 Department of Mathematcs Texas A&M Unversty, College Staton, TX Center for Combnatorcs, LPMC Nanka Unversty, Tanjn , P.R. Chna 1 kung@unt.edu, 2 xsun@math.tamu.edu, 3 cyan@math.tamu.edu February, 2006 Key words and phrases. Goncarov Polynomal, parkng functons, lattce path, q-analog Mathematcs Subject Classfcaton. Abstract In ths paper we extend the work of [1] to study combnatoral problems va the theory of borthogonal polynomals. In partcular, we gve a unfed algebrac approach to several combnatoral objects, ncludng order statstcs of a real sequence, parkng functons, lattce paths, and area-enumerators of lattce paths, by descrbng the propertes of the sequence of Goncarov polynomals and ts varous generalzatons. 4 The thrd author was supported n part by NSF grant #DMS

2 1 Introducton The man content of ths paper s to use theory of sequences of polynomals borthogonal to a sequence of lnear operators to study combnatoral problems. In partcular, we descrbed the algebrac propertes of the sequence of Goncarov polynomals and ts varous generalzatons, whch gve a unfed algebrac approach to several combnatoral objects, ncludng (1) The cumulatve dstrbuton functons of the random vectors of order statstcs of n ndependent random varables wth unform dstrbuton on an nterval; (2) general parkng functons, that s, sequences (x 1, x 2,..., x n ) of ntegers whose order statstcs are bounded between two gven non-decreasng sequences; (3) Lattce paths that avod certan general boundares; and (4) The area-enumerator of lattce paths avodng certan general boundares. The object (2) can be vewed as a dscrete analog of (1). In lterature, objects (1) and (3) have been extensvely studed by probablstc argument and countng technques. General parkng functons wth one boundary has been studed n a prevous paper by the frst and the thrd author [2]. The contrbuton of the current paper s to put all four problems n the same umbrella, and present a unfed treatment. For object (1) and (2), the correspondng polynomal sequences s Goncarov polynomals, whch are outlned n Secton 2. Ths secton also contans an ntroducton to the theory of sequences of borthogonal polynomals. In Secton 3 we descrbe the sequences of dfference Goncarov polynomals. The combnatoral nterpretaton of dfference Goncarov polynomals s lattce paths wth one-sded boundary, whch s gven n Secton 4. Secton 5 and 6 are on q-analog of dfference Goncarov polynomals, and ts applcaton n enumeratng area of lattces paths wth one-sded boundary. The two-sded boundares for both parkng functons and lattce paths are treated n Secton 7. 2 Sequences of borthogonal polynomals and Goncarov polynomals We begn by gvng an outlne of the theory of sequences of polynomals borthogonal to a sequence of lnear functonals. The detals can be found n [1]. Let P be vector space of all polynomals n the varable x over a feld F of characterstc zero. Let D : P P be the dfferentaton operator. For a scalar a n the feld F, let ε(a) : P F, p(x) p(a) be the lnear functonal whch evaluates p(x) at a. 2

3 Let ϕ s (D), s = 0, 1, 2,... be a sequence of lnear operators on P of the form ϕ s (D) = D s b sr D r, (2.1) r=0 where the coeffcents b s0 are assumed to be non-zero. There exsts a unque sequence p n (x), n = 0, 1, 2,... of polynomals such that p n (x) has degree n and where δ sn s the Kronecker delta. ε(0)ϕ s (D)p n (x) = δ sn, (2.2) The polynomal sequence p n (x) s sad to be borthogonal to the sequence ϕ s (D) of operators, or, the sequence ε(0)ϕ s (D) of lnear functonals. Usng Cramer s rule to solve the lnear system and Laplace s expanson to group the results, we can express p n (x) by the the followng determnantal formula: p n (x) = b 00 b 10 b n0 b 00 b 01 b b 0,n 1 b 0n 0 b 10 b b 1,n 2 b 1,n b b 2,n 3 b 2,n b n 1,0 b n 1,1 1 x x 2 /2!... x n 1 /(n 1)! x n /. (2.3) Snce {p n (x)} n=0 forms a bass of P, any polynomal can be unquely expressed as a lnear combnaton of p n (x) s. Explctly, we have the expanson formula: If p(x) s a polynomal of degree n, then p(x) = d p (x), (2.4)! where d = ε(0)ϕ (D)p(x). In partcular, x n = b,n p (x), (2.5)! whch gves a lnear recurson for p n (x). Equvalently, one can wrte (2.5) n terms of formal power seres equatons, and obtan the Appell relaton e xt = n=0 p n (x)ϕ n (t), (2.6) 3

4 where ϕ n (t) = t s r=0 b srt r. A specal example of sequences of borthogonal polynomals s the Goncarov polynomals. Let (a 0, a 1, a 2,...) be a sequence of numbers or varables called nodes. The sequence of Gon carov polynomals g n (x; a 0, a 1,..., a n 1 ), n = 0, 1, 2,... s the sequence of polynomals borthogonal to the operators ϕ S (D) = D s a r sd r. r! As ndcated by the notaton, g n (x; a 0, a 1,..., a n 1 ) depends only on the nodes a 0, a 1,..., a n 1. Indeed, from equaton (2.3), we have the determnantal formula, a 1 a 2 0 a 3 0 a 0 2! 3!... n 1 0 (n 1)! a 0 1 a 2 1 a 1 2!... n 2 1 (n 2)! a g n (x; a 0, a 1,..., a n 1 ) = a 2... n 3 2 (n 3)! a n 1 x 1 x 2 x 3 x 2! 3!... n 1 x n (n 1)! r=0 From equatons (2.5) and (2.6), we have the lnear recurson and the Appell relaton x n = e xt = a n g (x; a 0, a 1,..., a 1 ) g n (x; a 0, a 1,..., a n 1 ) tn e ant. n=0 a n 0 a n 1 1 (n 1)! a n 2 2 (n 2)! Fnally, from equaton (2.4), we have the expanson formula. If p(x) s a polynomal of degree n, then ε(a )D p(x) p(x) = g (x; a 0, a 1,..., a 1 ).! The sequence of Goncarov polynomals possesses a set of specfc propertes, whch are lsted n the followng. The proofs can be found n [1].. 4

5 1. Dfferental relatons. The Gon carov polynomals can be equvalently defned by the dfferental relatons Dg n (x; a 0, a 1,..., a n 1 ) = ng n 1 (x; a 1, a 2,..., a n 1 ), wth ntal condtons g n (a 0 ; a 0, a 1,..., a n 1 ) = δ 0n. 2. Integral relatons. g n (x; a 0, a 1,..., a n 1 ) = n = 3. Shft nvarant formula. x a 0 g n 1 (t; a 1, a 2,..., a n 1 )dt x t1 tn 1 dt 1 dt 2 dt n. a 0 a 1 a n 1 g n (x + ξ; a 0 + ξ, a 1 + ξ,..., a n 1 + ξ) = g n (x; a 0, a 1,..., a n 1 ). 4. Perturbaton formula. g n (x; a 0,..., a m 1, a m + b m, a m+1,..., a n 1 ) = g n (x; a 0,... a m 1, a m, a m+1,..., a n 1 ) g n m (a m + b m ; a m, a m+1,..., a n 1 )g m (x; a 0, a 1,..., a m 1 ). m Applyng the perturbaton formula repeatedly, we can perturb any subset of nodes. For example, the followng formula allows us to perturb an ntal segment of length n m + 1 : g n (x; a 0 + b 0, a 1 + b 1,..., a n m + b n m, a n m+1,..., a n 1 ) = g n (x; a 0, a 1,..., a n m, a n m+1,..., a n 1 ) n m g n (a + b ; a, a +1,..., a n 1 )g (x; a 0 + b 0, a 1 + b 1,..., a 1 + b 1 ). 5. Bnomal expanson. g n (x + y; a 0,..., a n 1 ) = g n (y; a,..., a n 1 )x. 5

6 In partcular, g n (x; a 0,..., a n 1 ) = g n (0, a,..., a n 1 )x. That s, coeffcents of Goncarov polynomals are constant terms of (shfted) Goncarov polynomals. 6. Combnatoral representaton. Let u be a sequence of non-decreasng postve ntegers. A u- parkng functon of length n s a sequence (x 1, x 2,..., x n ) whose order statstcs (the sequence (x (1), x (2),..., x (n) ) obtaned by rearrangng the orgnal sequence n non-decreasng order) satsfy x () u. Goncarov polynomals form a natural bass of polynomals for workng wth u-parkng functons. Explctly, we have P n (u 1, u 2,..., u n ) = g n (x; x u 1, x u 2,..., x u n ) = g n (0; u 1, u 2,..., u n ) = ( 1) n g n (0; u 1, u 2,..., u n ). For more propertes and computatons of parkng functons va Goncarov polynomals, please refer to [1, 2, 3]. In partcular, the sum enumerator and factoral moments of the sums are computed. For u-parkng functons, the sum enumerator s a specalzaton of g n (x; a 0, a 1,..., a n 1 ) wth a = 1 + q + + q u 1. Generatng functons for factoral moments of sums of u-parkng functons are gven n [1], whle the explct formulas for the frst and second factoral moments of sums of u-parkng functons are gven n [2], and n [3] for all factoral moments for classcal parkng functons where u forms an arthmetc progresson. Remark. Sequences of polynomals of bnomal type and the related Sheffer sequences can be vewed as specal cases of sequences of borthogonal polynomals. We shall use a descrpton gven n the classcal paper of Rota, Kahaner and Odlyzko [9]. A delta operator B s a formal power seres of order 1 n the dervatve operator D, B(D) = D + b 2 D 2 + b 3 D 3 + A Sheffer sequence {s n } (for B) s a polynomal sequence such that Bs n = s n 1 for all n = 0, 1, 2,..., The basc sequence {b n } (for B) s the Sheffer sequence wth ntal values b n (0) = δ 0,n. Basc sequence s also called sequences of bnomal type, whch has generatng functon of the form b n (x) tn = exf(t), (2.7) n=0 6

7 where f(t) s the compostonal nverse of B(x) = x + b 2 x 2 + b 3 x 3 +. Sheffer sequences have generatng functons of the form n=0 s n (x) tn = 1 s(t) exf(t), (2.8) where f(t) s as above, and s(t) = n 0 s n(0)t n s a formal power seres of order 0. Substtutng B(t) for t n (2.8), we obtan the Appell relaton e xt = n=0 s n (x) s(b(t))[b(t)]n. From ths we conclude that Sheffer polynomals can be vewed as sequences of polynomals borthogonal to operator sequences of the form ϕ s (D) = s(b(d))[b(d)] n, where B(t), s(t) are formal power seres wth s(0) 0, B(0) = 0 and B (0) 0. It s known that Sheffer sequences wth specal ntal values can be used to study lattce path enumeraton and emprcal dstrbuton functons, where the correspondng delta operators are D and the backward dfference operator. See [5, 6] and ther references. For example, n studyng the order statstcs of a set of unformly dstrbuted random varables n [0, 1], let s n (x) := g n (x; a n, a n 1,..., a 1 ). Snce Ds n (x) = ns n 1 (x), we get a Sheffer sequence {s n } wth ntal values s n (a n ) = δ 0,n. Hence computng the emprcal dstrbuton s reduced to compute Sheffer polynomals wth gven ntal values. For lattce path enumeraton, one just replace D wth, (See Secton 3 and 4 for detals). Nederhausen has used Umbral Calculus to fnd explct solutons for lattces paths n the followng cases: (1) the boundary ponts a n are pecewse affne n n, (2) the steps are n several drectons, and (3) lattce paths are weghted by the number of left turns. The Sheffer sequence s also used to enumerate lattce paths nsde a band parallel to the dagonal, whch s a specal case descrbed n Secton 7. In ths paper, we use the framework of sequences of borthogonal polynomals for the followng reason: (1) It s more general, whle almost all the nce formulas for Sheffer sequences can be extended to ths general settng, (2) It s a natural algebrac correspondence for workng wth parkng functons and lattce paths, by the combnatoral decomposton theorem for parkng functons [1, Theorem5.1], and ts analog n lattce paths (c.f. Secton 4). And (3). The theory of borthogonal polynomals gves a unfed treatment to several combnatoral objects smultaneously, ncludng parkng functons, order statstcs of a set of unformly dstrbuted random varables, lattce paths, and the area-enumerator of lattce paths. 7

8 3 Dfference Goncarov Polynomal In ths secton we dscuss the dfference analog of Goncarov polynomals, whch s the sequence of polynomals borthogonal to a sequence of lnear operators defned by formal power seres of the (backward) dfference operators. Explctly, let p(x) be a polynomal n the vector space P = F [x]. Defne p(x) = p(x) p(x 1). Note that p(x) s a polynomal of x whose degree s one less than that of p(x). We follow the conventon that the upper factoral x (n) s x(x + 1) (x + n 1). Observe that the polynomals p n (x) = x (n) form a bass of the vector space P; p n (x) = np n 1 (x); and p n (x) x=0 = 0, whenever < n. Gven a sequence b 0, b 1,..., let ψ S ( ), s = 0, 1, 2,... be the lnear operators The dfference Goncarov polynomals ψ s ( ) = r=0 b (r) s r! r+s. (3.1) g n (x; b 0,..., b n 1 ), n = 0, 1, 2,... s the the unque sequence of polynomals satsfyng deg( g n (x; b 0,..., b n 1 )) = n and ψ s ( ) g n (x; b 0,..., b n 1 ) x=0 = δ sn. Many propertes of Goncarov polynomals have a dfference analog. whch are lsted n the followng lst. Most proofs are smlar to that of the dfferental case, and hence omtted or only gven a sketch. 1. Determnantal formula. g n (x; b 0,..., b n 1 ) = b 1 b (2) 0 b (3) 0 0 2! 3! b 0 1 b (2) 1 1 2! b (n 1) 0 (n 1)! b (n 2) 1 (n 2)! b (n 3) 2 b (n) 0 b (n 1) 1 (n 1)! b (n 1) 2 (n 2)! b (n 3)! b n 1 1 x x (2) 2! x (3) 3! x (n 1) (n 1)! x (n). (3.2) 8

9 2. Expanson formula. If p(x) s a polynomal of degree n, then p(x) = ψ ( )(p(x)) x=0 g (x; b 0,..., b 1 ). (3.3)! It s obtaned by applyng D on both sdes and then settng x = Lnear recurrence. Let p(x) = x (n) n (3.3), we get x (n) = b (n ) g (x; b 0,..., b 1 ). (3.4) 4. Appell relaton. 5. Dfference relaton. (1 t) x = t n g n (x; b 0,..., b n 1 ) (1 t) bn. n=0 g n (x; b 0,..., b n 1 ) = n g n 1 (x; b 1,..., b n 1 ), (3.5) and g n (b 0 ; b 0,..., b n 1 ) = δ 0n. (3.6) The above dfference relaton and ntal condton unquely determne the sequence of dfference Goncarov polynomals. 6. Summaton formula. When x, b 0 are ntegers, solvng the dfference relaton, we have the summaton x g n (x; b 0, b 1,..., b n 1 ) = n g n 1 (t; b 1,..., b n 1 ). (3.7) t=b 0 +1 Iteratng ths when x, b Z, we have the summaton formula g n (x; b 0,..., b n 1 ) = x 1 1 =b =b 1 +1 n 1 n=b n , (3.8) where w 2 =w 1 α() = α(w 1 ) + α(w 1 + 1) + + α(w 2 ) f w 1 w 2 ; 0 f w 1 = w 2 + 1; α(w 2 + 1) α(w 2 + 2) α(w 1 1) f w 1 > w (3.9)

10 7. Shft-nvarant formula. Usng a change of varable, the summaton relaton (3.7), and nducton, one obtan the followng shft-nvarant formula g n (x + t; b 0 + t,..., b n 1 + t) = g n (x; b 0,..., b n 1 ). (3.10) Note that Equaton (3.10) holds for all x, t, and b s, snce t s a polynomal dentty whch s true for nfntely many values of x, t and b s. 8. Perturbaton formula. g n (x; b 0,..., b m 1, b m + δ m, b m+1,..., b n 1 ) = g n (x; b 0,..., b m 1, b m, b m+1,..., b n 1 ) (3.11) g n m (b m + δ m ; b m, b m+1,..., b n 1 ) g m (x; b 0,..., b m 1 ). m Applyng the perturbaton formula repeatly, we get g n (x; b 0 + δ 0, b 1 + δ 1,..., b n 1 + δ n 1 ) = g n (x; b 0,..., b n 1 ) (3.12) g n (b + δ ; b,..., b n 1 ) g (x; b 0 + δ 0,..., b 1 + δ 1 ). 9. Bnomal expanson. If we expand g n (x + y; b 0,..., b n 1 ) usng the bass {x (n) }, we can get g n (x + y; b 0,..., b n 1 ) = g n (y; b,..., b n 1 )x (). (3.13) To see ths, note that (x + y) () = (x + y) ( 1), and g n (x + y; b 0,..., b n 1 ) = n g n 1 (x + y; b 0,..., b n 1 ). Now apply to both sde of Equaton (3.13) and set x = 0. Equaton (3.13) follows from nducton. Dfference Goncarov polynomal of low degrees can be easly computed by the determnant formula or the summaton formula. For example, g 0 (y) = 1, g 1 (y; b 0 ) = y (1) b (1) 0, g 2 (y; b 0, b 1 ) = y (2) 2b (1) 1 y(1) + 2b (1) 0 b(1) 1 b (2) 0, g 3 (y; b 0, b 1, b 2 ) = y (3) 3b (1) 2 y(2) + (6b (1) 1 b(1) 2 3b (2) 1 )y(1) b (3) 0 + 3b (2) 0 b(1) 2 6b (1) 0 b(1) 1 b(1) 2 + 3b (1) 0 b(2) 1. 10

11 In the followng specal cases, dfference Goncarov polynomals have a nce closed-form expresson. Case 1 b = b for all. Then g n (x, b,..., b) = (x b) (n). Case 2 b = y + ( 1)b forms an arthmetc progresson. Then we have the dfference analog of Abel polynomals: { (x y)(x y nb + 1) (n 1) n > 0; g n (x, y, y + b,..., y + (n 1)b) = 1 n = 0. To see ths, verfy the dfference relaton that g n (x; b 0,..., b n 1 ) = n g n 1 (x; b 1,..., b n 1 ) and g n (b 0 ; b 0,..., b n 1 ) = δ 0n. In partcular, g n (0; 1,..., n) = n+1( 2n n ) = Cn, where C n = 1 n+1( 2n n ) s the famous Catalan number. 4 Dfference Goncarov Polynomals and Lattce Paths In ths secton we descrbe a combnatoral decomposton whch allows us to relate the dfference Goncarov polynomals wth certan lattce paths n plane. Let x, n be postve ntegers. Consder lattces paths from (0, 0) to (x 1, n) wth steps (1, 0) or (0, 1). Denote by the sequence (x 0,..., x n ) such a path whose rght-most pont on the -th row s (x, ). Obvously, we always have x n = x 1. Gven b 0 b 1 b n 1 x, let LP n (b 0,..., b n 1 ) be the number of paths (x 0,..., x n 1 ) from (0, 0) to (x 1, n) wth steps (1, 0) and (0, 1) such that x < b for 0 n 1. s It s well-known that the total number of the paths from (0, 0) to (x 1, n) n the grd (x 1) n ( ) x + n 1 LP n (x,..., x) = = x(n) n. Another way of countng paths n the grd (x 1) n s to decompose the paths nto several classes as follows. Let (x 0,..., x n ) be such a path and be the frst row that x b. Each of such paths conssts of three parts: the frst part s a path from (0, 0) to (b 1, ) that never touches the ponts (b j, j) for j = 0, 1,...,, the second path conssts of one step (1, 0), from (b 1, ) to (b, ), and the thrd part s a path that goes from (b, ) to (x 1, n). The number of paths of the frst knd s LP (b 0,..., b 1 ), whle that of the thrd knd s ( x 1 b ) +n = (x b ) (n ). Therefore the total number of paths s n LP (b 0,..., b 1 ) (x b ) (n ). (n )! 11 (n )!

12 So x (n) = LP (b 0,..., b 1 ) (x a ) (n ). (4.1) (n )! Comparng Equatons (3.4) and (4.1), we get Theorem 4.1 LP (b 0,..., b 1 ) = 1! g (x; x b 0,..., x b n 1 ). In partcular, LP n (b 0,..., b n 1 ) = 1 g n(0; b 0,..., b n 1 ). (4.2) Usng the dentty ( x) (n) = ( 1) n x(x 1)(x 2) (x n + 1) = ( 1) n x (n) where x (n) s the lower factoral, and the determnant formula for g n, we get [( )] b LP n (b 0,..., b n 1 ) = det j ,j n 1 An equvalent descrpton for LP n (b 0,..., b n 1 ) s the number of nteger ponts n certan n- dmensonal polytope consdered by Ptman and Stanley n [8]. Let Π n (x) := {y R n : y 0 and y 1 + y y x x for all 1 n}, Ptman and Stanley computed the number of nteger ponts n the polytope Π n when x 1,..., x n are postve ntegers, and gave the formula where K n = {k N n : N(Π n (x)) = (x 1 + 1)(k1) k 1! k K n n =2 x (k ) k 2!, k j for all 1 n 1 and =1 k = n}. Lettng b 0 = x 0 + 1, b = 1 + j=0 x. Every nteger pont y = (y 1,..., y n ) Π n (x) corresponds unquely to a lattce path 0 r 0 r 1 r n 1 where r = y < b for all. Hence [( N(Π n (x)) = LP n (b 0, b 1,..., b n 1 ) = det 12 b j + 1 )] =1. (4.3) 0,j n 1

13 Formula (4.3) can also be derved from the Steck formula (c.f. Theorem 7.3) on the number of lattce paths lyng between two gven ncreasng sequences [11, 12]. The detaled can be found n the monograph [4] and correspondng theory of borthogonal polynomals are presented n Secton 7. As an applcaton of (4.2), let b =. Then LP n (1, 2,..., n) counts the number of Dyck paths. We have LP n (1,..., n) = 1 g n(0; 1,..., n) = n+1( 1 2n ) n, agan obtan the famous Catalan number. In general, we can consder the number of lattce paths from (0, 0) to (r + µn, n) (r, µ P), whch never touch the lne x = r + µy. Ths s just the case where b = r + ( 1)µ, and the number s gven by LP n (r, r + µ, r + 2µ,..., r + (n 1)µ) = 1 g n(0; r, r µ,..., r (n 1)µ) = 1 r(r + nµ + 1)(n 1) ( ) r r + n(µ + 1) =, (4.4) r + n(µ + 1) n a well-known result. (See, for example, [4, p.9]. In partcular, for r = 1 and µ = k, t counts the number of lattce paths from ( the orgn to (kn, n) that never pass below the lne y = x/k. The 1 formula (4.4) becomes (k+1)n ) kn+1 n, the nth k-catalan number [10, p. 175]. We can renterpret the perturbaton formula (3.12) usng paths. Gven two paths (a 0,..., a n 1 ) and (c 0, c 1,..., c n 1 ) wth a c, We consder all paths that never touch (c 0, c 1,..., c n 1 ). Frst, t s LP n (c 0,..., c n 1 ) as defned. Secondly, we can also count the paths that never touch (c 0,..., c n 1 ), whle they touch the path (a 0,..., a n ) on -th row for the frst tme. The total number of such paths s LP (a 0,..., a 1 )LP n (c a, c +1 a,..., c n 1 a ). So we have the formula LP n (c 0,..., c n 1 ) = LP (a 0,..., a 1 )LP n (c a, c +1 a,..., c n 1 a ) (4.5) +LP n (a 0,..., a n ). Convertng the equaton usng dfference Goncarov polynomals, we have g n (x; x a 0, x a 1,..., x a n 1 ) = g n (x; x c 0,..., x c n 1 ) g n (0; a c,..., a c n 1 ) g (x; x a 0,..., x a 1 ). Replacng x c wth b, c a wth δ, and usng the shft formula (3.10) on 13

14 g n (0; a c,..., a c n 1 ) by g n (0; a c,..., a c n 1 ) = g n (0; δ, b +1 b δ,..., b n 1 b δ ) we get the perturbaton formula (3.12) agan. = g n (b + δ ; b, b +1,..., b n 1 ), Remark. Let b 0 b 1 b n 1 be a sequence of ntegers. Denote by LP < n the set of nteger sequences (r 0 < r 1 < < r n 1 ) such that 0 r < b for = 0, 1,..., n 1. Then LP n <, the cardnalty of LP < n, can be obtaned as follows: Let s = r ( 1). Then s 0 s 1 s n 1 and 0 s < b ( 1). Hence LP n < (b 0,..., b n 1 ) = LP n (b 0, b 1 1,..., b n 1 n 1). Alternatvely, we can use the forward dfference operator f and ts basc polynomals x (n) = x(x 1)... (x n + 1) to replace and x (n) n (3.1), where f p(x) = p(x + 1) p(x). Explctly, let ψ S ( f ) = (b s) (r) r=0 r! r+s f. Denote the correspondng sequence of borthogonal polynomals by g f,n (x; b 0,..., b n 1 ). The determnant formula of g f,n (x; b 0,..., b n 1 ) s obtaned from (3.2) by replacng each upper factoral a () wth the lower factoral a () = a(a 1)... (a + 1). Under ths settng, we have LP n < (b 0,..., b n 1 ) = 1! g f,n(0; b 0,..., b n 1 ). The above two approaches yeld the followng determnant formulas for LP n < (b 0,..., b n 1 ). [( )] [( )] LP n < b b + j (b 0,..., b n 1 ) = det = det j + 1 j + 1 0,j<n. 0,j<n 5 q-goncarov Polynomal For u-parkng functons, the sum enumerator S n (q, u) = (a 1,...,a n) qa 1+a 2 + +a n, where (a 1,..., a n ) ranges over all u-parkng functons, s just the specalzaton of the (dfferental) Goncarov polynomals where u s replaced wth 1 + q + + q u 1. Ths s not the case for lattce paths and dfference Goncarov polynomals. Defne the area-enumerator of lattce paths to be Area n (q; b) := q x 0+x 1 + +x n 1, (5.1) (x 0,...,x n 1 ) LP n(b) where LP n (b) s the set of lattce paths from (0, 0) to (x 1, n) (x 1 b n 1 ) that never touch (b 0, b 1,..., b n 1 ). Note that x 0 + x x n 1 s the area of the regon bounded by the path and the lnes x = 0 and y = n. To study Area n (q; b), we develop the q-analog of dfference Goncarov polynomals. We use the followng the conventons that (n) q = 1 qn 1 q ; (n) q! = (1) q (n) q ; and the rsng q-factoral { (1 A) (1 Aq (A; q) n = n 1 ) f n > 0, 1 f n = 0. 14

15 Let p(y) be a polynomal n the rng F (q)[y]. Defne q p(y) = p(y) p(y/q) (1 q)y/q. It s easy to check that q p(y) s a polynomal of y whose degree s one less than that of p(y). Observe that the polynomals p n (y) = (y; q) n form a bass of the rng F (q)[y]; q p n (y) = (n) q p n 1 (y); and qp n (y) y=1 = 0, whenever < n. Let ψ q,s ( q ), s = 0, 1, 2,..., be the sequence of lnear operators ψ q,s (D q ) = s=0 (b s ; q) r r+s q, (5.2) (r) q! and defne the dfference q-goncarov polynomals g n (q; y; b) = g n (q; y; b 0,..., b n 1 ) to be the sequence of polynomals borthogonal to ψ q,s ( q ),.e., ψ q,s ( q )g n (y; b; q) y=1 = (n) q!δ sn. Smlar propertes satsfed by the regular Goncarov polynomals can be generalzed to a q-analog for the dfference q-goncarov polynomals. We lst the man results n the followng. 1. Determnantal formula. g n (q; y; b 0,..., b n 1 ) = (n) q! 1 (b 0 ; q) 1 (b 0 ;q) 2 (2) q! (b 0 ;q) 3 (3) q! 0 1 b 1 (b 1 ;q) 2 (2) q! b 2 (b 0 ;q) n 1 (n 1) q! (b 1 ;q) n 2 (n 2) q! (b 2 ;q) n 3 (n 3) q! (b 0 ;q) n (n) q! (b 1 ;q) n 1 (n 1) q! (b 2 ;q) n 1 (n 2) q! b n 1 1 (y; q) 1 (y;q) 2 (2) q! (y;q) 3 (3) q! (y;q) n 1 (n 1) q! (y;q) n (n) q!. 2. Expanson formula. For any polynomal p(y) F (q)[y], p(y) = To verfy, apply D on both sdes and then set y = 1. ψ q, ( q )(p(y)) y=1 g n (q; y; b 0,..., b 1 ), (5.3) () q! 3. Lnear recurson. (y; q) n = (b ; q) n g (q; y; b 0,..., b 1 ). (5.4) q 15

16 4. Appell Relaton. Snce n (a; q) n (q; q) n t n = (at; q) (t; q), where (a; q) = k=0 (1 aqk ), we have the generatng functon (yt; q) = g (q; y; b 0,..., b 1 ) (b t; q) t () q! 5. Dfference relaton. wth the ntal condtons q g n (q; y; b 0,..., b n 1 ) = (n) q g n 1 (q; y; b 1,..., b n 1 ), (5.5) g n (q; b 0 ; b 0,..., b n 1 ) = δ 0n. (5.6) 6. Bnomal expanson. The bnomal expanson of Goncarov polynomals becomes g n (q; ty; b 0,..., b n 1 ; q) = t g n (q; t; b,..., b n 1 )(y; q). (5.7) q Ths s because q (ty; q) = () q t(ty; q) 1, and q g n (q; ty; b 0,..., b n 1 ) = (n) q tg n 1 (q; ty; b 1,..., b n 1 ). Now apply q to both sde of the equaton and set y = Summaton formula. Let y = q x and b = q a, where x and a are ntegers, we have x g n (q; y; b 0,..., b n 1 ) = (1 q) q 1 (n) q g n 1 (q; q ; b 1,..., b n 1 ), =a 0 +1 where the sum s defned the same as n 3.9. Ths s because g n (q; y; b 0,..., b n 1 ) = g n (q; q x 1 ; b 0,..., b n 1 ) + (1 q)q x 1 (n) q g n 1 (q; q x ; b 1,..., b n 1 ) and the ntal condton (5.6). sum formula Iterate t we obtaned the g n (q; y; b 0,..., b n 1 ) = (1 q) n (n) q! x q q 2 1 From ths we derve the shft formula: 1 =a =a 1 +1 n 1 n=a n 1 +1 q n 1.(5.8) g n (q; yq ξ ; b 0 q ξ,..., b n 1 q ξ ) = q nξ g n (q; y; b 0,..., b n 1 ). (5.9) Snce g n (q; y; b) s a polynomal of y and b s over a feld and the equaton above holds for nfntely many y s and b s, t holds for all y and b s. 16

17 Examples of the q-goncarov polynomals follow. g 0 (q; y) = 1, g 1 (q; y; b 0 ) = (y; q) 1 (b 0 ; q) 1, g 2 (q; y; b 0, b 1 ) = (y; q) 2 (2) q!(b 1 ; q) 1 (y; q) 1 + (2) q!(b 0 ; q) 1 (b 1 ; q) 1 (b 0 ; q) 2, g 3 (q; y; b 0, b 1, b 2 ) = (y; q) 3 (3) q (b 2 ; q) 1 (y; q) 2 + ((3) q!(b 1 ; q) 1 (b 2 ; q) 1 (3) q (b 1 ; q) 2 )(y; q) 1 (b 0 ; q) 3 + (3) q (b 0 ; q) 2 (b 2 ; q) 1 (3) q!(b 0 ; q) 1 (b 1 ; q) 1 (b 2 ; q) 1 + (3) q (b 0 ; q) 1 (b 1 ; q) 2. In partcular, n some specal cases we have nce closed formula, g n (q; q x ; q b,..., q b ) = q nb (q x b ; q) n and g n (q; q x ; q y, q y+1,..., q y+n 1 ) = ( 1) n q (n 2) nx (q y x ; q) n. 6 q-goncarov Polynomals and Area of Lattce Paths Defne the q-upper factoral x (n) q = (1 q x ) (1 q x+n 1 )/(1 q) n. In ths secton we use the dfference q-goncarov polynomal developed n the prevous secton to represent the areaenumerator of lattce paths wth upper constrant. Consder an (x 1) by n grd consstng of vertcal and horzontal lnes. Let (x 0,..., x n 1 ) be a path that goes from (0, 0) to (x 1, n) along the grd, whle the rght-most pont on the -th row s (x, ) for = 0, 1,..., n 1. Gven a path (b 0, b 1,..., b n 1 ) wth b 0 b 1 b n 1 x 1, let Area n (q; b) be gven n Formula (5.1). We establsh a recurrence of Area n (q; b) by computng the area-enumerator of Area n (q; x 1, x 1,..., x 1) n two ways. Frst, t s well-known that the area-enumerators of all the paths n the grd (x 1) n s ( ) x + n 1 Area n (q; x 1,..., x 1) = n q = x(n) q (n) q!. Now apply the decomposton as n 4. Let (x 0,..., x n ) be a path n (x 1) n for whch be the frst row that the path touches the path (b 0,..., b n 1 ),.e., x b. Each of such paths conssts of two parts: the frst part s a path from (0, 0) to (b 1, ) that never touches the path (b 0,..., b 1 ), the second part conssts of one horzontal step from (b 1, ) to (b, ), and the thrd part s a path that goes from (b, ) to (x 1, n). The area contrbuted by the frst part s Area (q; b 0,..., b 1 ), whle 17

18 that of the second knd and the thrd s q b (n ) ( x 1 b + n n area-enumerator of all the paths s So whch leads to (q x ; q) n = x (n) q = Area (q; b 0,..., b )q b (n ) (x b ) (n ) q. (n ) q! )q = qb (n ) (x b ) (n ) q (n ) q!. Therefore the (n) q! (n ) q! Area (q; b 0,..., b )q (n )b (x b ) (n ) q, (6.1) (n) q! [ ] (n ) q! (1 q) (q x b ; q) n q (n )b Area (q; b 0,..., b ). (6.2) Comparng equatons (5.4) and (6.2), we need to make the power of q on the rght-hand sde of equaton (6.2) dependng only on and b. To acheve ths, we replace q by 1 q n equaton (6.2). Then (q x ; q) n becomes ( 1) n q (nx+(n 2)) (q x ; q) n, and (n) q! becomes q (n 2) (n)q!. Substtutng nto (6.2) and reorganzng the equaton, we get Then (q x ; q) n = ( n ) Comparng equatons (5.4) and (6.3), we obtan Area ( 1 q ; b 0,..., b ) = [ ] () q!( 1) (q x b ; q) n q x (1 1 q q ) Area ( 1 q ; b 0,..., b ). (6.3) ( 1) () q!q x (1 1 q ) g n(q; q x ; q x b 0,..., q x b 1 ). Let f(q; x, b 0,..., b n 1 ) be a polynomals of q wth parameters x, b 0,..., b n 1 gven by f(q; x, b 0,..., b n 1 ) = g n (q; q x ; q x b 0,..., q x b 1 ). Theorem 6.1 The area-enumerators of lattce paths n the rectangle (x 1) n that stays strctly above the path (b 0,..., b n ) s Area n (q; b) = = ( 1) n (1 q) n (n) q! q n(n 1) 2 +nx f( 1 q ; x, b 0,..., b n 1 ) ( 1) n (1 q) n (n) q! q n(n 1) 2 f n ( 1 q ; 0, b 0,..., b n 1 ). (6.4) 18

19 7 Two-Boundary Extensons Goncarov polynomals can be extended to represent parkng functons and lattce paths wth both both upper and lower boundares. 7.1 Parkng functons wth two-sded boundary u-parkng functons are nteger sequences whose order statstcs s bounded by a prefxed sequence u from above. We may consder parkng functons wth both upper and lower constrants. More precsely, let r 1 r 2 r n and s 1 s 2 s n be two sequence of non-decreasng ntegers. A (r, s)-parkng functon of length n s a sequence (x 1,..., x n ) whose order statstcs satsfy r x () < s. Denoted by P n (r, s) = P n (r 1,..., r n ; s 1,..., s n ) the number of (r, s)-parkng functons of length n. The formula P n (r, s) can also be expressed as borthogonal polynomals. Let (a 0, a 1, a 2,... ) and (b 0, b 1, b 2,... ) be two sequences of numbers. Goncarov polynomals Defne the extended g n(x; a, b) = g n(x; a 0, a 2,..., a n 1 ; b 0, b 1,..., b n 1 ), n = 0, 1, 2,..., to be the sequence of polynomals borthogonal to the operators ϕ s (D) = D s (b s a s+r 1 ) r +D r, (7.1) r! r=0 where x + = max(x, 0). (Here we set a 1 = 0.) By the determnant formula (2.3), (b 0 a 1 ) 1 (b 0 a 0 ) 2 + (b 0 a 2 ) 3 + (b 0 a n 2 ) + 2! 3!... n 1 + (b 0 a n 1 ) n + (n 1)! (b 1 a 2 ) 0 1 (b 1 a 1 ) 2 + (b 1 a n 2 ) + 2!... n 2 + (b 1 a n 1 ) n 1 + (n 2)! (n 1)! g n(x; (b 2 a n 2 ) a, b) = (b 2 a 2 ) +... n 3 + (b 2 a n 1 ) n 2 + (n 3)! (n 2)! (b n 1 a n 1 ) + x 1 x 2 x 3 x 2! 3!... n 1 x n (n 1)!. In partcular, g n(0; a, b)) = ( 1) n det[(b a j ) j +1 + /(j +1)!]. By the lnear recurrence equaton (2.5), we have x n = (b a n 1 ) + n g (x; a, b). 19

20 It follows that for n 1, (b a n 1 ) + n g (0; a, b) = 0. (7.2) The sequence {g n(0, a, b) s unquely determned by the above recurrence and ntal values g 0 (0; a, b) = 1, g 1 (0; a, b) = (b 0 a 0 ) +. Theorem 7.1 P n (r 1,..., r n ; s 1,..., s n ) = ( 1) n g n(0; r 1,..., r n ; s 1,..., s n ). (7.3) To prove Theorem 7.1, t s suffcent to show that ( 1) (s +1 r n ) n + P (r, s) = 0, (7.4) for n 0, and P 1 (r, s) = (s 1 r 1 ) +. The ntal value s clear. In the followng we gve two proof of equaton (7.4). The frst one s based on a weghted verson of ncluson-excluson prncple. The second s an nvoluton on the set of marked parkng functons, whch reveals some ntrnsc structures of two-sded parkng functons. Frst Proof of (7.4). Let M(S) be the set of all sequences α of length n such that α S s a (r, s)-parkng functon of length S, and each term n α S c les n [r n, s +1 ), where S c = [n] \ S. Then (7.4) s equvalent to S ( 1) S M(S) = 0, where the sum ranges over all subsets S [n]. For any sequence α, let T [α] = {S : α M(S)}. It s suffcent to show that ( 1) T = 0. (7.5) T T [α] Observe that f α M(S) and S S, then α M(S ). Hence T [α] s a flter n the power set of [n]. T [α] f and only f α s a (r, s)-parkng functon. When T [α], let S 1,..., S r be the mnmal elements of T [α]. S 1,..., S r satsfy the followng propertes. 1. S < n. For any (r, s)-parkng functon α, deletng the largest element whch s n [r n, s n ), the remanng s a (r, s)-parkng functon of length n 1. Hence T [α] {[n]}. 2. S 1 = S 2 = = S r = k for some k < n. Assume k = S 1 < S 2 = l. The condton α M(S 1 ) mples all terms of α are less than s k+1, and at least n k of them are larger than or equal to r n. In partcular, the largest element n α S2 les n [r n, s k+1 ). Then S 2 s not mnmal. 20

21 3. S 1 S 2 S r [n]. Otherwse, every term n α appears n some (r, s)-parkng functon of length k < n, and hence less than s k. And any term n a poston of S 1 \ S 2 s greater than or equal to r n. Hence the mnmal element of T [α] has length S 1 1, a contradcton. Denoted by F(S 1,..., S r ) the flter of the power set of [n] generated by S 1,..., S r, and W (F(S 1,..., S r )) = w(t ), T F(S 1,...,S r) for a weght functon w(t ). Note that F(S 1,... S r ) = F(S 1 )... F(S r ), and F(S ) F(S j ) = F(S S j ), usng Incluson-Excluson, we have W (F(S 1,..., S r )) = W (F(S )) W (F(S S j )) + W (F(S S j S k )). <j <j<k Lettng the weght w(t ) = ( 1) T. Formula (7.5) follows from the equaton W (F(S)) = ( 1) n S = 0 whenever S [n]. Second Proof of (7.4). ( n even We gve a bjectve proof for the equvalent form ) (s +1 r n ) n + P (r, s) = odd ( n ) (s +1 r n ) n + P (r, s). (7.6) The left-hand sde of (7.6) s the cardnalty of the set M of pars (α, S) where α s a sequence of length n, S [n] wth S even, such that α S s a (r, s)-parkng functon of length S, and any term n α S c les n [r n, s S +1 ). The rght-hand sde of (7.6) s the cardnalty of the set N of pars (α, S) where (α, S) s smlar as those appeared n M, except that S beng odd. For a sequence α, let m = max(α) be the frst maxmal entry of α. Let pos(m) be the poston of m. Defne σ : M N by lettng σ(α, S) = (α, T ) where { (α, S \ {pos(m)}), f pos(m) S, T = (α, S {pos(m)}), f pos(m) / S. The map σ s well-defned: For any par (α, S) wth S even, clearly T s odd. Case 1. If pos(m) S, then deletng m from the subsequence n S, we obtan a (r, s)-parkng functon of length S 1 = T. The condton that m = max(α) and m [r S, s S ) mples that for any term x n α T c, x m < s S = s T +1. In addton, f S c, then m x r n for any x S c ; f S c =, then α tself s a (r, s)-parkng functon of length n, hence m r n. Ths proves that n the case pos(m) S, (α, T ) N. Case 2. If pos(m) / S, then any term x S c les n [r n, s S +1 ) [r n, s S +2 ). As m [r n, s S +1 ), jonng m to the subsequence on S wll result n a (r, s)-parkng functon of length S + 1 = T. In both cases, σ maps a par n M to a par n N. 21

22 It s easly seen that σ has the nverse map σ 1 (α, T ) = (α, S) where { (α, T \ {pos(m)}), f pos(m) T, S = (α, T {pos(m)}), f pos(m) / T. Ths proved that σ s a bjecton from M to N. Equaton (7.1) should be compared wth followng formula of Steck [11, 12] for the cumulatve dstrbuton functon of the random vector of order statstcs of n ndependent random vaables wth unform dstrbuton on an nterval. Let 0 r 1 r 2 r n 1 0 s 1 s 2 s n 1, be gven constants such that r < v for = 1, 2,..., n. If X (1), X (2),..., X (n) are the order statstcs n ascendng order from a sample of n ndependent unform random varables wth ranges 0 to 1, then P r(r X () s, 1 n) = det[(s r j ) j +1 + /(j + 1)!]. (7.7) The dfference between equatons (7.1) and (7.7) s that n a (r, s)-parkng functon, the sequence can only assume nteger values. Whle a unform random varable n [0, 1] corresponds to realvalued parkng functons, [2]. Hence equaton (7.1) can be vewed as a dscrete extenson of the Steck formula (7.7). The equaton (7.4) can be extended to the sum-enumerator of (r, s)-parkng functons. Defne S n (q; r, s) = α=(a 1,...,a n) q a 1+ +a n where the sum ranges over all (r, s)-parkng functons of length n. Wth a smlar proof to that of (7.4), we can show that ( 1) ((s +1 ) q (r n ) q ) n S (q; r, s) = 0, where the factor s +1 ) q (r n ) q s 0 f r n s +1. Hence, the sum-enumerator s a specalzaton of the polynomal P n (r, s): Theorem 7.2 where and S n (q; r, s) = P n (r(q), s(q)), r(q) = ((r 1 ) q, (r 2 ) q,..., (r n ) q ), s(q) = ((s 1 ) q, (s 2 ) q,..., (s n ) q ). 22

23 7.2 Lattce paths wth two-sded boundary The number of lattce paths wth two boundares was obtaned as a determnant formula by Steck [11, 12]. Such enumeraton and varous generalzatons has been extensvely studed, for example, n [4, Chapter2]. Hence we just lst the man results on the subject, and explan the connecton to borthogonal polynomals. Theorem 7.3 (Steck) Let a 0 a 1 a m and b 0 b 1 b m be sequences of ntegers such that a, b. The number of sets of ntegers (r 0, r 1,..., r m ) such that r 0 < r 1 < < r m and a < r < b for 0 m s the (m + 1)-th determnant det(d j ) where d j = ( b a j +j 1) j +1 f j and b a j > 1. Otherwse d j = 0. Denoted by LP n (a, b) the number of lattce paths (x 0, x 1,..., x n 1 ) from (0, 0) to (x 1, n) satsfyng a x < b < x. Steck s formula gves [( )] (b a j ) + LP n (a, b) = det. (7.8) j + 1 Formula (7.8) s a specalzaton of extended dfference Goncarov polynomals. Gven two sequences a = (a 0, a 1, a 2,... ) and b = (b 0, b 1, b 2,... ), let g n(x; a, b) = g n(x; a 0, a 1,..., a n 1 ; b 0, b 1,..., b n 1 ) (n = 0, 1, 2... ) be the sequence of polynomals borthogonal to the operators ( ) ψ S ( ) = s ( 1) r (bs a s+r 1 ) + r. (7.9) r Then r=0 ( ) g n(0; (b a j ) + a, b)) = det[ ] = LP n (a, b). (7.10) j + 1 These equatons enable us to enumerate LP n (a, b) from the theory of borthogonal polynomals. Snce generally, recurrence relatons and generatng functons are major technques to solve a countng problem, we show how such results on LP n (a, b) follow from the propertes of g n(0; a, b)). Frst, the lnear recurrence (3.4) becomes x (n) =! ( 1)n ( (b a n 1 ) + n ) g (x; a, b) It follows that ( ) δ 0,n = ( 1) (b a n 1 ) + 1 ( ) n! g (0; a, b) = ( 1) (b a n 1 ) + LP (a, b). (7.11) n 23

24 Equaton (7.11) gves a lnear recurrence to compute LP n (a, b). Ths equaton has been obtaned n [4] as well, see equaton (2.37). One can also prove t combnatorally by countng alternatvely the set M of all pars (α, ) where α = (α 1, α 2,..., α n ) s an nteger sequence satsfyng (1) α 1 α 2 α, (2) a j α j < b j for each j = 0, 1,...,, and (3) α +1 < α +2 < < α n [a n, b +1 ) n. By a smlar argument, f one defne Area n (q; a, b) = x q x 0+x 1 + +x n 1 a 0 a n 1, Then δ 0,n = ( 1) ( (b a n 1 ) + n ) Area (q; a, b). q From the Appell relaton we get the dentty 1 (1 t) x = n=0 n=0 g n(x; a, b) ψ n(t), LP n (a, b) ψ n(t) where ψ n (t) s gven n (7.9). In partcular, when a = k + c, b = k + d wth c < d,.e., lattce paths are restrcted n a strp of wdth d c, ψ n (t) = t n f(t) where f(t) s a polynomals of degree. Hence the sequence LP n(a, b) has a ratonal generatng functon d c k n=0 = 1, LP n (a, b) tn = 1 f(t). It remans true even the ntal boundares a, b for = 0, 1,..., T are arbtrary. References 1. J. Kung and C. Yan, Goncarov polynomals and parkng functons, Journal of Combnatoral Theory, Seres A 102(2003), J. Kung and C. Yan, Expected Sums of Moments General Parkng Functons, Annals of Combnatorcs, vol. 7(2003), J. Kung and C. Yan, Exact Formula for Moments of Sums of Classcal Parkng Functons, Advances n Appled Mathematcs, vol 31(2003), 24

25 4. S. G. Mohanty, Lattce Path Countng and Applcatons, Academc Press, H. Nederhausen, Sheffer polynomals for computng exact Kolmogorov-Smrvov and Reny type dstrbutons. Annals of Statstcs 9(1981), H. Nederhausen, Lattce Path Enumeraton and Umbral Calculus, Advances n Combnatoral Methods and Applcaton s (edtor: N. Balakrshnan), Brkhuser Boston (1997). 7. E.J.G.Ptman, Smple proofs of Steck s determnantal expressons for probabltes n the Kolmogorov and Smrnov tests. Bull. Austral. Math. Soc., 7(1972), J. Ptman and R. Stanley, A polytope related to emprcal dstrbutons, plane trees, parkng functons, and the assocahedron, Dscrete Comput. Geom. 27(2002), no.4, G-C. Rota, D. Kahaner and A. Odlyzko, On the foundatons of combnatoral theory. VIII. Fnte operator calculus. J. Math. Anal. Appl. 42 (1973), R. Stanley, Enumeratve Combnatorcs, Volume 2. Cambrdge Unversty Press, G.P. Steck, The Smrnov two sample tests as rank tests, Ann. Math. Statst., 40: , G.P. Steck. Rectangle probabltes for unform order statstcs and the probablty that the emprcal dstrbuton functon les between two dstrbuton functons. Ann. Math. Statst., 42:1 11,

Ballot Paths Avoiding Depth Zero Patterns

Ballot Paths Avoiding Depth Zero Patterns Ballot Paths Avodng Depth Zero Patterns Henrch Nederhausen and Shaun Sullvan Florda Atlantc Unversty, Boca Raton, Florda nederha@fauedu, ssull21@fauedu 1 Introducton In a paper by Sapounaks, Tasoulas,

More information

Bezier curves. Michael S. Floater. August 25, These notes provide an introduction to Bezier curves. i=0

Bezier curves. Michael S. Floater. August 25, These notes provide an introduction to Bezier curves. i=0 Bezer curves Mchael S. Floater August 25, 211 These notes provde an ntroducton to Bezer curves. 1 Bernsten polynomals Recall that a real polynomal of a real varable x R, wth degree n, s a functon of the

More information

Difference Equations

Difference Equations Dfference Equatons c Jan Vrbk 1 Bascs Suppose a sequence of numbers, say a 0,a 1,a,a 3,... s defned by a certan general relatonshp between, say, three consecutve values of the sequence, e.g. a + +3a +1

More information

APPENDIX A Some Linear Algebra

APPENDIX A Some Linear Algebra APPENDIX A Some Lnear Algebra The collecton of m, n matrces A.1 Matrces a 1,1,..., a 1,n A = a m,1,..., a m,n wth real elements a,j s denoted by R m,n. If n = 1 then A s called a column vector. Smlarly,

More information

3.1 Expectation of Functions of Several Random Variables. )' be a k-dimensional discrete or continuous random vector, with joint PMF p (, E X E X1 E X

3.1 Expectation of Functions of Several Random Variables. )' be a k-dimensional discrete or continuous random vector, with joint PMF p (, E X E X1 E X Statstcs 1: Probablty Theory II 37 3 EPECTATION OF SEVERAL RANDOM VARIABLES As n Probablty Theory I, the nterest n most stuatons les not on the actual dstrbuton of a random vector, but rather on a number

More information

THE CHINESE REMAINDER THEOREM. We should thank the Chinese for their wonderful remainder theorem. Glenn Stevens

THE CHINESE REMAINDER THEOREM. We should thank the Chinese for their wonderful remainder theorem. Glenn Stevens THE CHINESE REMAINDER THEOREM KEITH CONRAD We should thank the Chnese for ther wonderful remander theorem. Glenn Stevens 1. Introducton The Chnese remander theorem says we can unquely solve any par of

More information

= z 20 z n. (k 20) + 4 z k = 4

= z 20 z n. (k 20) + 4 z k = 4 Problem Set #7 solutons 7.2.. (a Fnd the coeffcent of z k n (z + z 5 + z 6 + z 7 + 5, k 20. We use the known seres expanson ( n+l ( z l l z n below: (z + z 5 + z 6 + z 7 + 5 (z 5 ( + z + z 2 + z + 5 5

More information

More metrics on cartesian products

More metrics on cartesian products More metrcs on cartesan products If (X, d ) are metrc spaces for 1 n, then n Secton II4 of the lecture notes we defned three metrcs on X whose underlyng topologes are the product topology The purpose of

More information

Restricted divisor sums

Restricted divisor sums ACTA ARITHMETICA 02 2002) Restrcted dvsor sums by Kevn A Broughan Hamlton) Introducton There s a body of work n the lterature on varous restrcted sums of the number of dvsors of an nteger functon ncludng

More information

The Jacobsthal and Jacobsthal-Lucas Numbers via Square Roots of Matrices

The Jacobsthal and Jacobsthal-Lucas Numbers via Square Roots of Matrices Internatonal Mathematcal Forum, Vol 11, 2016, no 11, 513-520 HIKARI Ltd, wwwm-hkarcom http://dxdoorg/1012988/mf20166442 The Jacobsthal and Jacobsthal-Lucas Numbers va Square Roots of Matrces Saadet Arslan

More information

An efficient algorithm for multivariate Maclaurin Newton transformation

An efficient algorithm for multivariate Maclaurin Newton transformation Annales UMCS Informatca AI VIII, 2 2008) 5 14 DOI: 10.2478/v10065-008-0020-6 An effcent algorthm for multvarate Maclaurn Newton transformaton Joanna Kapusta Insttute of Mathematcs and Computer Scence,

More information

Bézier curves. Michael S. Floater. September 10, These notes provide an introduction to Bézier curves. i=0

Bézier curves. Michael S. Floater. September 10, These notes provide an introduction to Bézier curves. i=0 Bézer curves Mchael S. Floater September 1, 215 These notes provde an ntroducton to Bézer curves. 1 Bernsten polynomals Recall that a real polynomal of a real varable x R, wth degree n, s a functon of

More information

n α j x j = 0 j=1 has a nontrivial solution. Here A is the n k matrix whose jth column is the vector for all t j=0

n α j x j = 0 j=1 has a nontrivial solution. Here A is the n k matrix whose jth column is the vector for all t j=0 MODULE 2 Topcs: Lnear ndependence, bass and dmenson We have seen that f n a set of vectors one vector s a lnear combnaton of the remanng vectors n the set then the span of the set s unchanged f that vector

More information

Lectures - Week 4 Matrix norms, Conditioning, Vector Spaces, Linear Independence, Spanning sets and Basis, Null space and Range of a Matrix

Lectures - Week 4 Matrix norms, Conditioning, Vector Spaces, Linear Independence, Spanning sets and Basis, Null space and Range of a Matrix Lectures - Week 4 Matrx norms, Condtonng, Vector Spaces, Lnear Independence, Spannng sets and Bass, Null space and Range of a Matrx Matrx Norms Now we turn to assocatng a number to each matrx. We could

More information

HMMT February 2016 February 20, 2016

HMMT February 2016 February 20, 2016 HMMT February 016 February 0, 016 Combnatorcs 1. For postve ntegers n, let S n be the set of ntegers x such that n dstnct lnes, no three concurrent, can dvde a plane nto x regons (for example, S = {3,

More information

Bernoulli Numbers and Polynomials

Bernoulli Numbers and Polynomials Bernoull Numbers and Polynomals T. Muthukumar tmk@tk.ac.n 17 Jun 2014 The sum of frst n natural numbers 1, 2, 3,..., n s n n(n + 1 S 1 (n := m = = n2 2 2 + n 2. Ths formula can be derved by notng that

More information

Lecture 13 APPROXIMATION OF SECOMD ORDER DERIVATIVES

Lecture 13 APPROXIMATION OF SECOMD ORDER DERIVATIVES COMPUTATIONAL FLUID DYNAMICS: FDM: Appromaton of Second Order Dervatves Lecture APPROXIMATION OF SECOMD ORDER DERIVATIVES. APPROXIMATION OF SECOND ORDER DERIVATIVES Second order dervatves appear n dffusve

More information

College of Computer & Information Science Fall 2009 Northeastern University 20 October 2009

College of Computer & Information Science Fall 2009 Northeastern University 20 October 2009 College of Computer & Informaton Scence Fall 2009 Northeastern Unversty 20 October 2009 CS7880: Algorthmc Power Tools Scrbe: Jan Wen and Laura Poplawsk Lecture Outlne: Prmal-dual schema Network Desgn:

More information

MA 323 Geometric Modelling Course Notes: Day 13 Bezier Curves & Bernstein Polynomials

MA 323 Geometric Modelling Course Notes: Day 13 Bezier Curves & Bernstein Polynomials MA 323 Geometrc Modellng Course Notes: Day 13 Bezer Curves & Bernsten Polynomals Davd L. Fnn Over the past few days, we have looked at de Casteljau s algorthm for generatng a polynomal curve, and we have

More information

Inner Product. Euclidean Space. Orthonormal Basis. Orthogonal

Inner Product. Euclidean Space. Orthonormal Basis. Orthogonal Inner Product Defnton 1 () A Eucldean space s a fnte-dmensonal vector space over the reals R, wth an nner product,. Defnton 2 (Inner Product) An nner product, on a real vector space X s a symmetrc, blnear,

More information

Canonical transformations

Canonical transformations Canoncal transformatons November 23, 2014 Recall that we have defned a symplectc transformaton to be any lnear transformaton M A B leavng the symplectc form nvarant, Ω AB M A CM B DΩ CD Coordnate transformatons,

More information

Randić Energy and Randić Estrada Index of a Graph

Randić Energy and Randić Estrada Index of a Graph EUROPEAN JOURNAL OF PURE AND APPLIED MATHEMATICS Vol. 5, No., 202, 88-96 ISSN 307-5543 www.ejpam.com SPECIAL ISSUE FOR THE INTERNATIONAL CONFERENCE ON APPLIED ANALYSIS AND ALGEBRA 29 JUNE -02JULY 20, ISTANBUL

More information

Continuous Time Markov Chain

Continuous Time Markov Chain Contnuous Tme Markov Chan Hu Jn Department of Electroncs and Communcaton Engneerng Hanyang Unversty ERICA Campus Contents Contnuous tme Markov Chan (CTMC) Propertes of sojourn tme Relatons Transton probablty

More information

PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 125, Number 7, July 1997, Pages 2119{2125 S (97) THE STRONG OPEN SET CONDITION

PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 125, Number 7, July 1997, Pages 2119{2125 S (97) THE STRONG OPEN SET CONDITION PROCDINGS OF TH AMRICAN MATHMATICAL SOCITY Volume 125, Number 7, July 1997, Pages 2119{2125 S 0002-9939(97)03816-1 TH STRONG OPN ST CONDITION IN TH RANDOM CAS NORBRT PATZSCHK (Communcated by Palle. T.

More information

A be a probability space. A random vector

A be a probability space. A random vector Statstcs 1: Probablty Theory II 8 1 JOINT AND MARGINAL DISTRIBUTIONS In Probablty Theory I we formulate the concept of a (real) random varable and descrbe the probablstc behavor of ths random varable by

More information

FACTORIZATION IN KRULL MONOIDS WITH INFINITE CLASS GROUP

FACTORIZATION IN KRULL MONOIDS WITH INFINITE CLASS GROUP C O L L O Q U I U M M A T H E M A T I C U M VOL. 80 1999 NO. 1 FACTORIZATION IN KRULL MONOIDS WITH INFINITE CLASS GROUP BY FLORIAN K A I N R A T H (GRAZ) Abstract. Let H be a Krull monod wth nfnte class

More information

Bivariate Gončarov polynomials and integer sequences

Bivariate Gončarov polynomials and integer sequences SCIENCE CHINA Mathematcs. ARTICLES. August 2014 Vol. 57 No. 8: 1561 1578 do: 10.1007/s11425-014-4827-x Bvarate Gončarov polynomals and nteger sequences KHARE Nraj 1, LORENTZ Rudolph 1 & YAN Catherne Huafe

More information

A summation on Bernoulli numbers

A summation on Bernoulli numbers Journal of Number Theory 111 (005 37 391 www.elsever.com/locate/jnt A summaton on Bernoull numbers Kwang-Wu Chen Department of Mathematcs and Computer Scence Educaton, Tape Muncpal Teachers College, No.

More information

Short running title: A generating function approach A GENERATING FUNCTION APPROACH TO COUNTING THEOREMS FOR SQUARE-FREE POLYNOMIALS AND MAXIMAL TORI

Short running title: A generating function approach A GENERATING FUNCTION APPROACH TO COUNTING THEOREMS FOR SQUARE-FREE POLYNOMIALS AND MAXIMAL TORI Short runnng ttle: A generatng functon approach A GENERATING FUNCTION APPROACH TO COUNTING THEOREMS FOR SQUARE-FREE POLYNOMIALS AND MAXIMAL TORI JASON FULMAN Abstract. A recent paper of Church, Ellenberg,

More information

Affine transformations and convexity

Affine transformations and convexity Affne transformatons and convexty The purpose of ths document s to prove some basc propertes of affne transformatons nvolvng convex sets. Here are a few onlne references for background nformaton: http://math.ucr.edu/

More information

1 Generating functions, continued

1 Generating functions, continued Generatng functons, contnued. Exponental generatng functons and set-parttons At ths pont, we ve come up wth good generatng-functon dscussons based on 3 of the 4 rows of our twelvefold way. Wll our nteger-partton

More information

ON A DETERMINATION OF THE INITIAL FUNCTIONS FROM THE OBSERVED VALUES OF THE BOUNDARY FUNCTIONS FOR THE SECOND-ORDER HYPERBOLIC EQUATION

ON A DETERMINATION OF THE INITIAL FUNCTIONS FROM THE OBSERVED VALUES OF THE BOUNDARY FUNCTIONS FOR THE SECOND-ORDER HYPERBOLIC EQUATION Advanced Mathematcal Models & Applcatons Vol.3, No.3, 2018, pp.215-222 ON A DETERMINATION OF THE INITIAL FUNCTIONS FROM THE OBSERVED VALUES OF THE BOUNDARY FUNCTIONS FOR THE SECOND-ORDER HYPERBOLIC EUATION

More information

NUMERICAL DIFFERENTIATION

NUMERICAL DIFFERENTIATION NUMERICAL DIFFERENTIATION 1 Introducton Dfferentaton s a method to compute the rate at whch a dependent output y changes wth respect to the change n the ndependent nput x. Ths rate of change s called the

More information

PHYS 705: Classical Mechanics. Canonical Transformation II

PHYS 705: Classical Mechanics. Canonical Transformation II 1 PHYS 705: Classcal Mechancs Canoncal Transformaton II Example: Harmonc Oscllator f ( x) x m 0 x U( x) x mx x LT U m Defne or L p p mx x x m mx x H px L px p m p x m m H p 1 x m p m 1 m H x p m x m m

More information

Numerical Heat and Mass Transfer

Numerical Heat and Mass Transfer Master degree n Mechancal Engneerng Numercal Heat and Mass Transfer 06-Fnte-Dfference Method (One-dmensonal, steady state heat conducton) Fausto Arpno f.arpno@uncas.t Introducton Why we use models and

More information

Lecture 5 Decoding Binary BCH Codes

Lecture 5 Decoding Binary BCH Codes Lecture 5 Decodng Bnary BCH Codes In ths class, we wll ntroduce dfferent methods for decodng BCH codes 51 Decodng the [15, 7, 5] 2 -BCH Code Consder the [15, 7, 5] 2 -code C we ntroduced n the last lecture

More information

2.3 Nilpotent endomorphisms

2.3 Nilpotent endomorphisms s a block dagonal matrx, wth A Mat dm U (C) In fact, we can assume that B = B 1 B k, wth B an ordered bass of U, and that A = [f U ] B, where f U : U U s the restrcton of f to U 40 23 Nlpotent endomorphsms

More information

8.4 COMPLEX VECTOR SPACES AND INNER PRODUCTS

8.4 COMPLEX VECTOR SPACES AND INNER PRODUCTS SECTION 8.4 COMPLEX VECTOR SPACES AND INNER PRODUCTS 493 8.4 COMPLEX VECTOR SPACES AND INNER PRODUCTS All the vector spaces you have studed thus far n the text are real vector spaces because the scalars

More information

BOUNDEDNESS OF THE RIESZ TRANSFORM WITH MATRIX A 2 WEIGHTS

BOUNDEDNESS OF THE RIESZ TRANSFORM WITH MATRIX A 2 WEIGHTS BOUNDEDNESS OF THE IESZ TANSFOM WITH MATIX A WEIGHTS Introducton Let L = L ( n, be the functon space wth norm (ˆ f L = f(x C dx d < For a d d matrx valued functon W : wth W (x postve sem-defnte for all

More information

Lecture 12: Discrete Laplacian

Lecture 12: Discrete Laplacian Lecture 12: Dscrete Laplacan Scrbe: Tanye Lu Our goal s to come up wth a dscrete verson of Laplacan operator for trangulated surfaces, so that we can use t n practce to solve related problems We are mostly

More information

SL n (F ) Equals its Own Derived Group

SL n (F ) Equals its Own Derived Group Internatonal Journal of Algebra, Vol. 2, 2008, no. 12, 585-594 SL n (F ) Equals ts Own Derved Group Jorge Macel BMCC-The Cty Unversty of New York, CUNY 199 Chambers street, New York, NY 10007, USA macel@cms.nyu.edu

More information

5 The Rational Canonical Form

5 The Rational Canonical Form 5 The Ratonal Canoncal Form Here p s a monc rreducble factor of the mnmum polynomal m T and s not necessarly of degree one Let F p denote the feld constructed earler n the course, consstng of all matrces

More information

Remarks on the Properties of a Quasi-Fibonacci-like Polynomial Sequence

Remarks on the Properties of a Quasi-Fibonacci-like Polynomial Sequence Remarks on the Propertes of a Quas-Fbonacc-lke Polynomal Sequence Brce Merwne LIU Brooklyn Ilan Wenschelbaum Wesleyan Unversty Abstract Consder the Quas-Fbonacc-lke Polynomal Sequence gven by F 0 = 1,

More information

Foundations of Arithmetic

Foundations of Arithmetic Foundatons of Arthmetc Notaton We shall denote the sum and product of numbers n the usual notaton as a 2 + a 2 + a 3 + + a = a, a 1 a 2 a 3 a = a The notaton a b means a dvdes b,.e. ac = b where c s an

More information

Module 3 LOSSY IMAGE COMPRESSION SYSTEMS. Version 2 ECE IIT, Kharagpur

Module 3 LOSSY IMAGE COMPRESSION SYSTEMS. Version 2 ECE IIT, Kharagpur Module 3 LOSSY IMAGE COMPRESSION SYSTEMS Verson ECE IIT, Kharagpur Lesson 6 Theory of Quantzaton Verson ECE IIT, Kharagpur Instructonal Objectves At the end of ths lesson, the students should be able to:

More information

A new Approach for Solving Linear Ordinary Differential Equations

A new Approach for Solving Linear Ordinary Differential Equations , ISSN 974-57X (Onlne), ISSN 974-5718 (Prnt), Vol. ; Issue No. 1; Year 14, Copyrght 13-14 by CESER PUBLICATIONS A new Approach for Solvng Lnear Ordnary Dfferental Equatons Fawz Abdelwahd Department of

More information

Formulas for the Determinant

Formulas for the Determinant page 224 224 CHAPTER 3 Determnants e t te t e 2t 38 A = e t 2te t e 2t e t te t 2e 2t 39 If 123 A = 345, 456 compute the matrx product A adj(a) What can you conclude about det(a)? For Problems 40 43, use

More information

Maximizing the number of nonnegative subsets

Maximizing the number of nonnegative subsets Maxmzng the number of nonnegatve subsets Noga Alon Hao Huang December 1, 213 Abstract Gven a set of n real numbers, f the sum of elements of every subset of sze larger than k s negatve, what s the maxmum

More information

Random Walks on Digraphs

Random Walks on Digraphs Random Walks on Dgraphs J. J. P. Veerman October 23, 27 Introducton Let V = {, n} be a vertex set and S a non-negatve row-stochastc matrx (.e. rows sum to ). V and S defne a dgraph G = G(V, S) and a drected

More information

Beyond Zudilin s Conjectured q-analog of Schmidt s problem

Beyond Zudilin s Conjectured q-analog of Schmidt s problem Beyond Zudln s Conectured q-analog of Schmdt s problem Thotsaporn Ae Thanatpanonda thotsaporn@gmalcom Mathematcs Subect Classfcaton: 11B65 33B99 Abstract Usng the methodology of (rgorous expermental mathematcs

More information

An (almost) unbiased estimator for the S-Gini index

An (almost) unbiased estimator for the S-Gini index An (almost unbased estmator for the S-Gn ndex Thomas Demuynck February 25, 2009 Abstract Ths note provdes an unbased estmator for the absolute S-Gn and an almost unbased estmator for the relatve S-Gn for

More information

Using T.O.M to Estimate Parameter of distributions that have not Single Exponential Family

Using T.O.M to Estimate Parameter of distributions that have not Single Exponential Family IOSR Journal of Mathematcs IOSR-JM) ISSN: 2278-5728. Volume 3, Issue 3 Sep-Oct. 202), PP 44-48 www.osrjournals.org Usng T.O.M to Estmate Parameter of dstrbutons that have not Sngle Exponental Famly Jubran

More information

Combined Wronskian solutions to the 2D Toda molecule equation

Combined Wronskian solutions to the 2D Toda molecule equation Combned Wronskan solutons to the 2D Toda molecule equaton Wen-Xu Ma Department of Mathematcs and Statstcs, Unversty of South Florda, Tampa, FL 33620-5700, USA Abstract By combnng two peces of b-drectonal

More information

Asymptotics of the Solution of a Boundary Value. Problem for One-Characteristic Differential. Equation Degenerating into a Parabolic Equation

Asymptotics of the Solution of a Boundary Value. Problem for One-Characteristic Differential. Equation Degenerating into a Parabolic Equation Nonl. Analyss and Dfferental Equatons, ol., 4, no., 5 - HIKARI Ltd, www.m-har.com http://dx.do.org/.988/nade.4.456 Asymptotcs of the Soluton of a Boundary alue Problem for One-Characterstc Dfferental Equaton

More information

The Order Relation and Trace Inequalities for. Hermitian Operators

The Order Relation and Trace Inequalities for. Hermitian Operators Internatonal Mathematcal Forum, Vol 3, 08, no, 507-57 HIKARI Ltd, wwwm-hkarcom https://doorg/0988/mf088055 The Order Relaton and Trace Inequaltes for Hermtan Operators Y Huang School of Informaton Scence

More information

COMPARISON OF SOME RELIABILITY CHARACTERISTICS BETWEEN REDUNDANT SYSTEMS REQUIRING SUPPORTING UNITS FOR THEIR OPERATIONS

COMPARISON OF SOME RELIABILITY CHARACTERISTICS BETWEEN REDUNDANT SYSTEMS REQUIRING SUPPORTING UNITS FOR THEIR OPERATIONS Avalable onlne at http://sck.org J. Math. Comput. Sc. 3 (3), No., 6-3 ISSN: 97-537 COMPARISON OF SOME RELIABILITY CHARACTERISTICS BETWEEN REDUNDANT SYSTEMS REQUIRING SUPPORTING UNITS FOR THEIR OPERATIONS

More information

COMPLEX NUMBERS AND QUADRATIC EQUATIONS

COMPLEX NUMBERS AND QUADRATIC EQUATIONS COMPLEX NUMBERS AND QUADRATIC EQUATIONS INTRODUCTION We know that x 0 for all x R e the square of a real number (whether postve, negatve or ero) s non-negatve Hence the equatons x, x, x + 7 0 etc are not

More information

CHAPTER 14 GENERAL PERTURBATION THEORY

CHAPTER 14 GENERAL PERTURBATION THEORY CHAPTER 4 GENERAL PERTURBATION THEORY 4 Introducton A partcle n orbt around a pont mass or a sphercally symmetrc mass dstrbuton s movng n a gravtatonal potental of the form GM / r In ths potental t moves

More information

Module 2. Random Processes. Version 2 ECE IIT, Kharagpur

Module 2. Random Processes. Version 2 ECE IIT, Kharagpur Module Random Processes Lesson 6 Functons of Random Varables After readng ths lesson, ou wll learn about cdf of functon of a random varable. Formula for determnng the pdf of a random varable. Let, X be

More information

1 Generating functions, continued

1 Generating functions, continued Generatng functons, contnued. Generatng functons and parttons We can make use of generatng functons to answer some questons a bt more restrctve than we ve done so far: Queston : Fnd a generatng functon

More information

COMBINATORIAL IDENTITIES DERIVING FROM THE n-th POWER OF A 2 2 MATRIX

COMBINATORIAL IDENTITIES DERIVING FROM THE n-th POWER OF A 2 2 MATRIX COMBINATORIAL IDENTITIES DERIVING FROM THE n-th POWER OF A MATRIX J Mc Laughln 1 Mathematcs Department Trnty College 300 Summt Street, Hartford, CT 06106-3100 amesmclaughln@trncolledu Receved:, Accepted:,

More information

Week3, Chapter 4. Position and Displacement. Motion in Two Dimensions. Instantaneous Velocity. Average Velocity

Week3, Chapter 4. Position and Displacement. Motion in Two Dimensions. Instantaneous Velocity. Average Velocity Week3, Chapter 4 Moton n Two Dmensons Lecture Quz A partcle confned to moton along the x axs moves wth constant acceleraton from x =.0 m to x = 8.0 m durng a 1-s tme nterval. The velocty of the partcle

More information

Chapter 5. Solution of System of Linear Equations. Module No. 6. Solution of Inconsistent and Ill Conditioned Systems

Chapter 5. Solution of System of Linear Equations. Module No. 6. Solution of Inconsistent and Ill Conditioned Systems Numercal Analyss by Dr. Anta Pal Assstant Professor Department of Mathematcs Natonal Insttute of Technology Durgapur Durgapur-713209 emal: anta.bue@gmal.com 1 . Chapter 5 Soluton of System of Lnear Equatons

More information

arxiv: v1 [math.co] 12 Sep 2014

arxiv: v1 [math.co] 12 Sep 2014 arxv:1409.3707v1 [math.co] 12 Sep 2014 On the bnomal sums of Horadam sequence Nazmye Ylmaz and Necat Taskara Department of Mathematcs, Scence Faculty, Selcuk Unversty, 42075, Campus, Konya, Turkey March

More information

ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM

ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM An elastc wave s a deformaton of the body that travels throughout the body n all drectons. We can examne the deformaton over a perod of tme by fxng our look

More information

Feb 14: Spatial analysis of data fields

Feb 14: Spatial analysis of data fields Feb 4: Spatal analyss of data felds Mappng rregularly sampled data onto a regular grd Many analyss technques for geophyscal data requre the data be located at regular ntervals n space and/or tme. hs s

More information

DIFFERENTIAL FORMS BRIAN OSSERMAN

DIFFERENTIAL FORMS BRIAN OSSERMAN DIFFERENTIAL FORMS BRIAN OSSERMAN Dfferentals are an mportant topc n algebrac geometry, allowng the use of some classcal geometrc arguments n the context of varetes over any feld. We wll use them to defne

More information

2 Finite difference basics

2 Finite difference basics Numersche Methoden 1, WS 11/12 B.J.P. Kaus 2 Fnte dfference bascs Consder the one- The bascs of the fnte dfference method are best understood wth an example. dmensonal transent heat conducton equaton T

More information

FINITELY-GENERATED MODULES OVER A PRINCIPAL IDEAL DOMAIN

FINITELY-GENERATED MODULES OVER A PRINCIPAL IDEAL DOMAIN FINITELY-GENERTED MODULES OVER PRINCIPL IDEL DOMIN EMMNUEL KOWLSKI Throughout ths note, s a prncpal deal doman. We recall the classfcaton theorem: Theorem 1. Let M be a fntely-generated -module. (1) There

More information

Solutions to exam in SF1811 Optimization, Jan 14, 2015

Solutions to exam in SF1811 Optimization, Jan 14, 2015 Solutons to exam n SF8 Optmzaton, Jan 4, 25 3 3 O------O -4 \ / \ / The network: \/ where all lnks go from left to rght. /\ / \ / \ 6 O------O -5 2 4.(a) Let x = ( x 3, x 4, x 23, x 24 ) T, where the varable

More information

= = = (a) Use the MATLAB command rref to solve the system. (b) Let A be the coefficient matrix and B be the right-hand side of the system.

= = = (a) Use the MATLAB command rref to solve the system. (b) Let A be the coefficient matrix and B be the right-hand side of the system. Chapter Matlab Exercses Chapter Matlab Exercses. Consder the lnear system of Example n Secton.. x x x y z y y z (a) Use the MATLAB command rref to solve the system. (b) Let A be the coeffcent matrx and

More information

REGULAR POSITIVE TERNARY QUADRATIC FORMS. 1. Introduction

REGULAR POSITIVE TERNARY QUADRATIC FORMS. 1. Introduction REGULAR POSITIVE TERNARY QUADRATIC FORMS BYEONG-KWEON OH Abstract. A postve defnte quadratc form f s sad to be regular f t globally represents all ntegers that are represented by the genus of f. In 997

More information

Chapter 12. Ordinary Differential Equation Boundary Value (BV) Problems

Chapter 12. Ordinary Differential Equation Boundary Value (BV) Problems Chapter. Ordnar Dfferental Equaton Boundar Value (BV) Problems In ths chapter we wll learn how to solve ODE boundar value problem. BV ODE s usuall gven wth x beng the ndependent space varable. p( x) q(

More information

Lecture 2: Numerical Methods for Differentiations and Integrations

Lecture 2: Numerical Methods for Differentiations and Integrations Numercal Smulaton of Space Plasmas (I [AP-4036] Lecture 2 by Lng-Hsao Lyu March, 2018 Lecture 2: Numercal Methods for Dfferentatons and Integratons As we have dscussed n Lecture 1 that numercal smulaton

More information

Determinants Containing Powers of Generalized Fibonacci Numbers

Determinants Containing Powers of Generalized Fibonacci Numbers 1 2 3 47 6 23 11 Journal of Integer Sequences, Vol 19 (2016), Artcle 1671 Determnants Contanng Powers of Generalzed Fbonacc Numbers Aram Tangboonduangjt and Thotsaporn Thanatpanonda Mahdol Unversty Internatonal

More information

Planar maps and continued fractions

Planar maps and continued fractions Batz 2010 p. 1/4 Planar maps and contnued fractons n collaboraton wth Jéréme Boutter 1 3 3 2 0 3 1 maps and dstances: generaltes Batz 2010 p. 2/4 Batz 2010 p. 3/4 degree of a face = number of ncdent edge

More information

Hidden Markov Models & The Multivariate Gaussian (10/26/04)

Hidden Markov Models & The Multivariate Gaussian (10/26/04) CS281A/Stat241A: Statstcal Learnng Theory Hdden Markov Models & The Multvarate Gaussan (10/26/04) Lecturer: Mchael I. Jordan Scrbes: Jonathan W. Hu 1 Hdden Markov Models As a bref revew, hdden Markov models

More information

The equation of motion of a dynamical system is given by a set of differential equations. That is (1)

The equation of motion of a dynamical system is given by a set of differential equations. That is (1) Dynamcal Systems Many engneerng and natural systems are dynamcal systems. For example a pendulum s a dynamcal system. State l The state of the dynamcal system specfes t condtons. For a pendulum n the absence

More information

An Introduction to Morita Theory

An Introduction to Morita Theory An Introducton to Morta Theory Matt Booth October 2015 Nov. 2017: made a few revsons. Thanks to Nng Shan for catchng a typo. My man reference for these notes was Chapter II of Bass s book Algebrac K-Theory

More information

1 Matrix representations of canonical matrices

1 Matrix representations of canonical matrices 1 Matrx representatons of canoncal matrces 2-d rotaton around the orgn: ( ) cos θ sn θ R 0 = sn θ cos θ 3-d rotaton around the x-axs: R x = 1 0 0 0 cos θ sn θ 0 sn θ cos θ 3-d rotaton around the y-axs:

More information

Week 2. This week, we covered operations on sets and cardinality.

Week 2. This week, we covered operations on sets and cardinality. Week 2 Ths week, we covered operatons on sets and cardnalty. Defnton 0.1 (Correspondence). A correspondence between two sets A and B s a set S contaned n A B = {(a, b) a A, b B}. A correspondence from

More information

The Multiple Classical Linear Regression Model (CLRM): Specification and Assumptions. 1. Introduction

The Multiple Classical Linear Regression Model (CLRM): Specification and Assumptions. 1. Introduction ECONOMICS 5* -- NOTE (Summary) ECON 5* -- NOTE The Multple Classcal Lnear Regresson Model (CLRM): Specfcaton and Assumptons. Introducton CLRM stands for the Classcal Lnear Regresson Model. The CLRM s also

More information

Self-complementing permutations of k-uniform hypergraphs

Self-complementing permutations of k-uniform hypergraphs Dscrete Mathematcs Theoretcal Computer Scence DMTCS vol. 11:1, 2009, 117 124 Self-complementng permutatons of k-unform hypergraphs Artur Szymańsk A. Paweł Wojda Faculty of Appled Mathematcs, AGH Unversty

More information

PHYS 705: Classical Mechanics. Calculus of Variations II

PHYS 705: Classical Mechanics. Calculus of Variations II 1 PHYS 705: Classcal Mechancs Calculus of Varatons II 2 Calculus of Varatons: Generalzaton (no constrant yet) Suppose now that F depends on several dependent varables : We need to fnd such that has a statonary

More information

THERE ARE INFINITELY MANY FIBONACCI COMPOSITES WITH PRIME SUBSCRIPTS

THERE ARE INFINITELY MANY FIBONACCI COMPOSITES WITH PRIME SUBSCRIPTS Research and Communcatons n Mathematcs and Mathematcal Scences Vol 10, Issue 2, 2018, Pages 123-140 ISSN 2319-6939 Publshed Onlne on November 19, 2018 2018 Jyot Academc Press http://jyotacademcpressorg

More information

Anti-van der Waerden numbers of 3-term arithmetic progressions.

Anti-van der Waerden numbers of 3-term arithmetic progressions. Ant-van der Waerden numbers of 3-term arthmetc progressons. Zhanar Berkkyzy, Alex Schulte, and Mchael Young Aprl 24, 2016 Abstract The ant-van der Waerden number, denoted by aw([n], k), s the smallest

More information

Causal Diamonds. M. Aghili, L. Bombelli, B. Pilgrim

Causal Diamonds. M. Aghili, L. Bombelli, B. Pilgrim Causal Damonds M. Aghl, L. Bombell, B. Plgrm Introducton The correcton to volume of a causal nterval due to curvature of spacetme has been done by Myrhem [] and recently by Gbbons & Solodukhn [] and later

More information

General viscosity iterative method for a sequence of quasi-nonexpansive mappings

General viscosity iterative method for a sequence of quasi-nonexpansive mappings Avalable onlne at www.tjnsa.com J. Nonlnear Sc. Appl. 9 (2016), 5672 5682 Research Artcle General vscosty teratve method for a sequence of quas-nonexpansve mappngs Cuje Zhang, Ynan Wang College of Scence,

More information

U.C. Berkeley CS294: Spectral Methods and Expanders Handout 8 Luca Trevisan February 17, 2016

U.C. Berkeley CS294: Spectral Methods and Expanders Handout 8 Luca Trevisan February 17, 2016 U.C. Berkeley CS94: Spectral Methods and Expanders Handout 8 Luca Trevsan February 7, 06 Lecture 8: Spectral Algorthms Wrap-up In whch we talk about even more generalzatons of Cheeger s nequaltes, and

More information

Math 217 Fall 2013 Homework 2 Solutions

Math 217 Fall 2013 Homework 2 Solutions Math 17 Fall 013 Homework Solutons Due Thursday Sept. 6, 013 5pm Ths homework conssts of 6 problems of 5 ponts each. The total s 30. You need to fully justfy your answer prove that your functon ndeed has

More information

NP-Completeness : Proofs

NP-Completeness : Proofs NP-Completeness : Proofs Proof Methods A method to show a decson problem Π NP-complete s as follows. (1) Show Π NP. (2) Choose an NP-complete problem Π. (3) Show Π Π. A method to show an optmzaton problem

More information

Section 8.3 Polar Form of Complex Numbers

Section 8.3 Polar Form of Complex Numbers 80 Chapter 8 Secton 8 Polar Form of Complex Numbers From prevous classes, you may have encountered magnary numbers the square roots of negatve numbers and, more generally, complex numbers whch are the

More information

Perfect Competition and the Nash Bargaining Solution

Perfect Competition and the Nash Bargaining Solution Perfect Competton and the Nash Barganng Soluton Renhard John Department of Economcs Unversty of Bonn Adenauerallee 24-42 53113 Bonn, Germany emal: rohn@un-bonn.de May 2005 Abstract For a lnear exchange

More information

The exponential map of GL(N)

The exponential map of GL(N) The exponental map of GLN arxv:hep-th/9604049v 9 Apr 996 Alexander Laufer Department of physcs Unversty of Konstanz P.O. 5560 M 678 78434 KONSTANZ Aprl 9, 996 Abstract A fnte expanson of the exponental

More information

Binomial transforms of the modified k-fibonacci-like sequence

Binomial transforms of the modified k-fibonacci-like sequence Internatonal Journal of Mathematcs and Computer Scence, 14(2019, no. 1, 47 59 M CS Bnomal transforms of the modfed k-fbonacc-lke sequence Youngwoo Kwon Department of mathematcs Korea Unversty Seoul, Republc

More information

Physics 5153 Classical Mechanics. D Alembert s Principle and The Lagrangian-1

Physics 5153 Classical Mechanics. D Alembert s Principle and The Lagrangian-1 P. Guterrez Physcs 5153 Classcal Mechancs D Alembert s Prncple and The Lagrangan 1 Introducton The prncple of vrtual work provdes a method of solvng problems of statc equlbrum wthout havng to consder the

More information

Appendix for Causal Interaction in Factorial Experiments: Application to Conjoint Analysis

Appendix for Causal Interaction in Factorial Experiments: Application to Conjoint Analysis A Appendx for Causal Interacton n Factoral Experments: Applcaton to Conjont Analyss Mathematcal Appendx: Proofs of Theorems A. Lemmas Below, we descrbe all the lemmas, whch are used to prove the man theorems

More information

Combinatorial Identities for Incomplete Tribonacci Polynomials

Combinatorial Identities for Incomplete Tribonacci Polynomials Avalable at http://pvamu.edu/aam Appl. Appl. Math. ISSN: 1932-9466 Vol. 10, Issue 1 (June 2015, pp. 40 49 Applcatons and Appled Mathematcs: An Internatonal Journal (AAM Combnatoral Identtes for Incomplete

More information

CALCULUS CLASSROOM CAPSULES

CALCULUS CLASSROOM CAPSULES CALCULUS CLASSROOM CAPSULES SESSION S86 Dr. Sham Alfred Rartan Valley Communty College salfred@rartanval.edu 38th AMATYC Annual Conference Jacksonvlle, Florda November 8-, 202 2 Calculus Classroom Capsules

More information

Another converse of Jensen s inequality

Another converse of Jensen s inequality Another converse of Jensen s nequalty Slavko Smc Abstract. We gve the best possble global bounds for a form of dscrete Jensen s nequalty. By some examples ts frutfulness s shown. 1. Introducton Throughout

More information