ISSN 2148-838Xhttp://dx.doi.org/10.13069/jacodesmath.451218 J. Algebra Comb. Discrete Appl. 5(3) • 137–142 Received: 11 April 2018 Accepted: 16 July 2018 Journal of Algebra Combinatorics Discrete Structures and Applications Finite Rogers–Ramanujan type continued fractions∗ Research Article Helmut Prodinger Abstract: New finite continued fractions related to Bressoud and Santos polynomials are established. 2010 MSC: 05A30, 11A55 Keywords: Bressoud polynomials, Santos polynomials, Rogers–Ramanujan identities 1. Introduction Define, as it is common today, (x; q)n := (1 − x)(1 − xq) . . . (1 − xqn−1), where we assume that |q| < 1, and we allow n also to be 0 and infinity. We also need the coefficients [ n k ] := (q;q)n (q;q)k(q;q)n−k . These standard notations can be found e. g. in the classic book [1]. The two Rogers-Ramanujan identities [1, 6] ∑ n≥0 qn 2 (q; q)n = 1 (q; q5)∞(q4; q5)∞ , ∑ n≥0 qn 2+n (q; q)n = 1 (q2; q5)∞(q3; q5)∞ are very popular, influential, useful and historically interesting. Let F(z) = ∑ n≥0 qn 2 zn (q; q)n and G(z) = ∑ n≥0 qn 2+nzn (q; q)n ; ∗ Dedicated to Peter Paule on the occasion of his 60th birthday. Helmut Prodinger; Department of Mathematics, University of Stellenbosch 7602, Stellenbosch, South Africa (email: hproding@sun.ac.za). 137 https://orcid.org/0000-0002-0009-8015 H. Prodinger / J. Algebra Comb. Discrete Appl. 5(3) (2018) 137–142 the continued fraction (due to Ramanujan) zG(z) F(z) = z 1 + zq 1 + zq2 1 + ... is also very well known, see [5, Entry 5] and [6, (6.1)]. There are several families of polynomials that approximate F(z) and G(z). Probably the the most well known are fn(z) = ∑ j≥0 qj 2 [ n + 1− j j ] zj → F(z) and gn(z) = ∑ j≥0 qj 2+j [ n− j j ] zj → G(z) for n →∞, because of their link to the Schur polynomials, see [1]. The finite continued fraction zgn(z) fn(z) = z 1 + zq 1 + zq2 ... 1 + zqn 1 is also known [5, Entry 16]. The polynomials sn(z) = ∑ j≥0 qj 2 [ n j ] zj → F(z) and tn(z) = ∑ j≥0 qj 2+j [ n j ] zj → G(z) for n →∞, due to Bressoud [7], are less well known; see also [8]. 2. Bressoud polynomials and continued fractions In this section, we will establish the following attractive finite continued fraction: Theorem 2.1. ztn(z) sn(z) = z 1 + zq(1−qn) 1 + zq2 1 + zq3(1−qn−1) 1 + zq4 1 + ... Proof. To prove this statement by induction, define the righthand side by Tn(z). It is plain to see that T0(z) = z, and Tn(z) = z 1 + zq(1−qn) 1 + Tn−1(zq2) . 138 H. Prodinger / J. Algebra Comb. Discrete Appl. 5(3) (2018) 137–142 We are left to prove that ztn(z) sn(z) = z 1 + zq(1−qn) 1 + ztn−1(zq 2) sn−1(zq2) = z 1 + zq(1−qn)sn−1(zq2) sn−1(zq2) + ztn−1(zq2) = z(sn−1(zq 2) + ztn−1(zq 2)) sn−1(zq2) + ztn−1(zq2) + zq(1−qn)sn−1(zq2) , which amounts to prove that tn(z) = sn−1(zq 2) + ztn−1(zq 2), sn(z) = sn−1(zq 2) + ztn−1(zq 2) + zq(1−qn)sn−1(zq2). We will show that the coefficients of zj coincide, which is trivial for j = 0, so we assume j ≥ 1: qj 2+j [ n j ] = qj 2+2j [ n−1 j ] + q(j−1) 2+3(j−1)+2 [ n−1 j −1 ] , which is equivalent to [ n j ] = qj [ n−1 j ] + [ n−1 j −1 ] and therefore true. The second one goes like this: qj 2 [ n j ] = qj 2+2j [ n−1 j ] + q(j−1) 2+3(j−1)+2 [ n−1 j −1 ] + q(1−qn)q(j−1) 2+2(j−1) [ n−1 j −1 ] , which is equivalent to [ n j ] = q2j [ n−1 j ] + qj [ n−1 j −1 ] + (1−qj) [ n j ] , and further to [ n j ] = qj [ n−1 j ] + [ n−1 j −1 ] , which finishes the proof. 3. Identities 39 and 38 from Slater’s list Slater [11] produced a list of Rogers-Ramanujan type series/product identities; Sills [10] in an amaz- ing effort reworked and annotated this list, providing, in particular, finite versions of all of them. Arguably the second most popular identities in the Rogers-Ramanujan world are Slater’s [11] iden- tities (39) and (38) ∑ n≥0 q2n 2 (q; q)2n = ∏ k≥1, k≡±2,±3,±4,±5 (mod 16) 1 1−qk , ∑ n≥0 q2n 2+2n (q; q)2n+1 = ∏ k≥1, k≡±1,±4,±6,±7 (mod 16) 1 1−qk . 139 H. Prodinger / J. Algebra Comb. Discrete Appl. 5(3) (2018) 137–142 Let sn(z) = ∑ 0≤2h≤n q2h 2 [ n 2h ] zh and tn(z) = ∑ 0≤2h≤n q2h 2+2h [ n 2h + 1 ] zh; these polynomials are called Santos polynomials [2–4]. In order to describe the finite continued fraction expansion of ztn(z)/sn(z), we define the following numbers and polynomials (power series) which were originally found by guessing: a2k := (1−q4k+1)(qn+1−2k; q2)2k q2k(qn−2k; q2)2k+1 , a2k+1 := (1−q4k+3)(qn−2k; q2)2k+1 q2k+2(qn−2k−1; q2)2k+2 ; S2i := ∑ j≥0 q2(i+j)(i+j+1)(qn−2i−2j; q)2j(q n−2i; q2)2i+1 (q; q)2j+1(q2j+3; q2)2i zj, S2i+1 := ∑ j≥0 q2(i+j+1) 2 (qn−1−2i−2j; q)2j(q n−1−2i; q2)2i+2 (q; q)2j+1(q2j+3; q2)2i+1 zj. Theorem 3.1. The polynomials Si satisfy the second order recurrence zSi+1 = Si−1−aiSi, S−1 = sn(z), S0 = tn(z). Consequently, we get the finite continued fraction expansion zt(n) s(n) = z a0 + z a1 + z a2 + z ... , or, more elegantly: zt(n) s(n) = zb0 1 + zb1 1 + zb2 1 + . . . with b0 = 1 a0 = 1−qn 1−q and bi = 1 ai−1ai = q2i(1−qn−i)(1−qn+i) (1−q2i−1)(1−q2i+1) for i ≥ 1. 140 H. Prodinger / J. Algebra Comb. Discrete Appl. 5(3) (2018) 137–142 Proof. The recursion will be shown for even i, the other instance being very similar: S2i−1 −a2iS2i = ∑ j≥0 q2(i+j) 2 (qn+1−2i−2j; q)2j(q n+1−2i; q2)2i (q; q)2j+1(q2j+3; q2)2i−1 zj − (1−q4i+1)(qn+1−2i; q2)2i q2i(qn−2i; q2)2i+1 ∑ j≥0 q2(i+j)(i+j+1)(qn−2i−2j; q)2j(q n−2i; q2)2i+1 (q; q)2j+1(q2j+3; q2)2i zj = (qn+1−2i; q2)2i ∑ j≥0 q2(i+j) 2 (qn+1−2i−2j; q)2j (q; q)2j+1(q2j+3; q2)2i−1 zj − (1−q4i+1)(qn+1−2i; q2)2i ∑ j≥0 q2(i+j) 2+2j(qn−2i−2j; q)2j (q; q)2j+1(q2j+3; q2)2i zj = (qn+1−2i; q2)2i ∑ j≥0 q2(i+j) 2 (qn+1−2i−2j; q)2j−1(1−qn−2i)(1−q2j+4i+1) (q; q)2j+1(q2j+3; q2)2i zj − (1−q4i+1)(qn+1−2i; q2)2i ∑ j≥0 q2(i+j) 2+2j(qn+1−2i−2j; q)2j−1(1−qn−2i−2j) (q; q)2j+1(q2j+3; q2)2i zj = (qn+1−2i; q2)2i ∑ j≥0 q2(i+j) 2 (qn+1−2i−2j; q)2j−1 (q; q)2j+1(q2j+3; q2)2i zj × [ (1−qn−2i)(1−q2j+4i+1)−q2j(1−q4i+1)(1−qn−2i−2j) ] = (qn+1−2i; q2)2i ∑ j≥0 q2(i+j) 2 (qn+1−2i−2j; q)2j−1 (q; q)2j+1(q2j+3; q2)2i zj(1−q2j)(1−qn+1+2i) = (qn+1−2i; q2)2i+1 ∑ j≥1 q2(i+j) 2 (qn+1−2i−2j; q)2j−1 (q; q)2j+1(q2j+3; q2)2i zj(1−q2j) = z(qn−1−2i; q2)2i+2 ∑ j≥0 q2(i+j+1) 2 (qn−1−2i−2j; q)2j (q; q)2j+1(q2j+3; q2)2i+1 zj = zS2i+1. Further, S−1 = ∑ j≥0 q2j 2 (qn+1−2j; q)2j (q; q)2j+1(q2j+3; q2)−1 zj = ∑ j≥0 q2j 2 (qn+1−2j; q)2j (q; q)2j zj = s0(z) and S0 = ∑ j≥0 q2j(j+1)(qn−2j; q)2j(1−qn) (q; q)2j+1 zj = ∑ j≥0 q2j(j+1)(qn−2j; q)2j+1 (q; q)2j+1 zj = t0(z). Now we can iterate this relation in the following form: zt(n) s(n) = zS0 S−1 = z a0 + zS1 S0 = z a0 + z a1 + zS2 S1 = . . . This is the desired (finite) continued fraction expansion. We remark that for n →∞, the quantities ai and Si appear already in [9]. 141 H. Prodinger / J. Algebra Comb. Discrete Appl. 5(3) (2018) 137–142 4. Conclusion We would like to mention that it is more challenging to find the continued fractions and the relevant quantities, as the present proofs (and possibly other ones) consist of routine manipulations. Since there are many Rogers-Ramanujan type identities and polynomials approximating them are not even unique, there might be additional additional results; compare our previous effort [9] for infinite versions. 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