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Some multivariate polynomials for doubled permutations

  • Received: 01 May 2020 Revised: 01 August 2020 Published: 16 September 2020
  • Primary: 05A05, 05A19; Secondary: 05A15

  • Flajolet and Françon [European. J. Combin. 10 (1989) 235-241] gave a combinatorial interpretation for the Taylor coefficients of the Jacobian elliptic functions in terms of doubled permutations. We show that a multivariable counting of the doubled permutations has also an explicit continued fraction expansion generalizing the continued fraction expansions of Rogers and Stieltjes. The second goal of this paper is to study the expansion of the Taylor coefficients of the generalized Jacobian elliptic functions, which implies the symmetric and unimodal property of the Taylor coefficients of the generalized Jacobian elliptic functions. The main tools are the combinatorial theory of continued fractions due to Flajolet and bijections due to Françon-Viennot, Foata-Zeilberger and Clarke-Steingrímsson-Zeng.

    Citation: Bin Han. Some multivariate polynomials for doubled permutations[J]. Electronic Research Archive, 2021, 29(2): 1925-1944. doi: 10.3934/era.2020098

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  • Flajolet and Françon [European. J. Combin. 10 (1989) 235-241] gave a combinatorial interpretation for the Taylor coefficients of the Jacobian elliptic functions in terms of doubled permutations. We show that a multivariable counting of the doubled permutations has also an explicit continued fraction expansion generalizing the continued fraction expansions of Rogers and Stieltjes. The second goal of this paper is to study the expansion of the Taylor coefficients of the generalized Jacobian elliptic functions, which implies the symmetric and unimodal property of the Taylor coefficients of the generalized Jacobian elliptic functions. The main tools are the combinatorial theory of continued fractions due to Flajolet and bijections due to Françon-Viennot, Foata-Zeilberger and Clarke-Steingrímsson-Zeng.



    For a fixed modulus x(0,1), the Jacobi elliptic function sn(z,x) is the inverse of an elliptic integral, i.e.,

    sn(z,x)=yiffz=y0dt(1t2)(1x2t2).

    The other two Jacobi elliptic functions are respectively defined by

    cn(z,x):=1sn2(z,x),dn(z,x):=1x2sn2(z,x).

    These functions appear in a variety of problems in physics and have been extensively studied in mathematical physics, algebraic geometry, combinatorics and number theory (see [5,6,8,9,11,12,19,20,21,27,28] for instance). When x=0 or x=1, the Jacobi elliptic functions degenerate into trigonometric or hyperbolic functions:

    sn(z,0)=sinz,cn(z,0)=cosz,dn(z,0)=1,sn(z,1)=tanhz,cn(z,1)=dn(z,1)=sech z.

    The three Jacobi elliptic functions are connected by the differential system (see [2]):

    {ddzsn(z,x)=cn(z,x)dn(z,x),ddzcn(z,x)=sn(z,x)dn(z,x),ddzdn(z,x)=x2sn(z,x)cn(z,x). (1)

    Note that

    (i)sn(iz,1)+cn(iz,1)=tanz+secz=n=0Enznn!, (2)

    where i=1 and En is the number of alternating permutations (also known as up-down permutations) in Sn (see [26]). The Taylor series expansions of these Jacobian elliptic functions are given as follows:

    sn(z,x)=z(1+x2)z33!+(1+14x2+x4)z55!(1+135x2+135x4+x6)+, (3)
    cn(z,x)=1z22!+(1+4x2)z44!(1+44x2+16x4)z66!+, (4)
    dn(z,x)=1x2z22!+x2(4+x2)z44!x2(16+44x2+x4)z66!+. (5)

    Defining the Laplace-Borel transforms of sn and cn by:

    S1(z,x)=0etsn(zt,x)dtandC0(z,x)=0etcn(zt,x)dt,

    i.e., the series obtained from (3) and (4) by replacing zn/n! by zn, Rogers and Stieltjes [21,27] found the following continued fractions expansions.

    S1(z,x)=z1+(1+x2)z21223x2z41+(1+x2)32z23425x2z41+(1+x2)52z2, (6)
    C0(z,x)=11+z21222x2z41+(32+22x2)z23242x2z41+(52+42x2)z2. (7)

    According to [12], the question of the possible combinatorial significance of the coefficients of Jn(x) in

    1+n=1(1)nJ2n(x)z2n(2n)!+n=0(1)nJ2n+1(x)z2n+1(2n+1)!=cn(z,x)+sn(z,x)

    was first raised by Schützenberger. The first combinatorial interpretation was given by Viennot [28], and is expressed in terms of so-called Jacobi permutations. Using his combinatorial theory of continued fractions Flajolet [11] proved that the coefficients of cn(z,x) count classes of alternating (up-and-down) permutations based on the parity of peaks. Dumont [8] finally discovered some further relations between these functions and the cycle structure of permutations. Flajolet-Françon [12] gave an interpretation of the elliptic functions as generating functions of doubled permutations.

    A polynomial f(x)=iaixiR[x] is called γ-positive if f(x)=n/2i=0γixi(1+x)n2i for nN and nonnegative reals γ0,γ1,,γn/2, the notion of γ-positivity appeared first in the work of Foata and Schützenberger [13]. A recent survey on γ-positivity in combinatorics and geometry was given by Athanasiadis [1]. In a series of papers Shin and Zeng [22,23,24] exploited the combinatorial theory of continued fractions to derive various γ-positivity results.

    In this paper, by generalizing the continued fraction expansions of Rogers and Stieltjes, we generalize Flajolet and Françon's the combinatorial interpretation of the Taylor coefficients of the Jacobian elliptic functions. Furthermore, we show that the Taylor coefficients of the generalized Jacobian elliptic functions are γ-positive. The main tools are the combinatorial theory of continued fractions due to Flajolet and bijections due to Françon-Viennot, Foata-Zeilberger and Clarke-Steingrímsson-Zeng.

    We follow [4,17,16,22,23] for notations and the nomenclature of various permutation statistics. First we recall three classical involutions defined on Sn, namely, the reverse, complement and the composition of the two. For πSn,

    πr:=π(n)π(2)π(1),πc:=(n+1π(1))(n+1π(2))(n+1π(n)),πrc:=(n+1π(n))(n+1π(2))(n+1π(1)).

    Denote by π1 the inverse permutation of π. If we use the standard two-line notation to write π, then π1 is obtained by switching the two lines and rearranging the columns to make the first line increasing. For instance, if π=(123231), then π1=(123312).

    Let Sn be the set of permutations of [n]={1,2,,n}. Given a permutation π=π(1)π(2)π(n)Sn we say that i[n1] is a descent (resp. excedance) of π if π(i)>π(i+1) (resp. π(i)>i). Let desπ (resp. excπ) denote the number of descents (resp. excedances) of π.

    Definition 2.1. For πSn, let π(0)=π(n+1)=0. Then any entry π(i) (i[n]) can be classified according to their ordinal type into four categories:

    ● a peak if π(i1)<π(i) and π(i)>π(i+1);

    ● a valley if π(i1)>π(i) and π(i)<π(i+1);

    ● a double ascent if π(i1)<π(i) and π(i)<π(i+1);

    ● a double descent if π(i1)>π(i) and π(i)>π(i+1).

    Let pkπ (resp. valπ, daπ, ddπ) be the number of peaks (resp. valleys, double ascents, double descents) in π. Note that for πSn, pkπ+ddπ=desπ+1.

    For σSn with convention 0–, i.e., σ(0)=0 and σ(n+1)=, any entry π(i) (i[n]) can be classified according to their left ordinal type into four categories: let Lpk (resp. Lval, Lda, Ldd) be the set of peaks (resp. valleys, doubleascents and doubledecents) and denote the corresponding cardinality by lpk (resp. lval, lda and ldd).

    Definition 2.2. For σ=σ(1)σ(n)Sn, we define its star compagnon σ as a permutation of {0,,n} by

    σ=(012nnσ(1)1σ(2)1σ(n)1). (8)

    Any entry π(i) (i[n]) can be classified according to their star cyclic type into four categories:

    Cpeakσ={i[n1]:(σ)1(i)<i>σ(i)}, (9)
    Cvalσ={i[n1]:(σ)1(i)>i<σ(i)}, (10)
    CdaσFixσ={i[n1]:(σ)1(i)<i<σ(i)}{i[n1]:i=σ(i)}, (11)
    Cddσ={i[n1]:(σ)1(i)>i>σ(i)}. (12)

    The corresponding cardinalties are denoted by cpk, cval, cdafix and cdd respectively.

    Definition 2.3. A permutation is a doubled permutation iff for all 0i(n2)/2, elements (i.e. values) 2i+1 and 2i+2 are of the same ordinal type. The set of doubled permutations is denoted by DPn. A permutation is a star doubled permutation iff for all 0i(n2)/2, elements (i.e. values) 2i+1 and 2i+2 are of the same star cyclic type. The set of star doubled permutations is denoted by DPn.

    For example, π1=6315427DP7 since 1 and 2 (resp. 3 and 4, 5 and 6) are valleys (resp. double descents, peaks) of π1. π2=6732451DP7 since {1,2}Cvalπ2, {3,4}Cddπ2 and {5,6}Cpeakπ2.

    The first goal of this paper is to explore the coefficients in the Taylor series expansion of Jacobi elliptic functions sn(z,x) by generalizing the continued fractions of (6).

    For σSn, the statistic (31-2)σ (resp. (13-2)σ) is the number of pairs (i,j) such that 2i<jn and σ(i1)>σ(j)>σ(i) (resp. σ(i1)<σ(j)<σ(i)). Similarly, the statistic (2-13)σ (resp. (2-31)σ) is the number of pairs (i,j) such that 1i<jn1 and σ(j+1)>σ(i)>σ(j) (resp. σ(j+1)<σ(i)<σ(j)). Moreover, define

    crosiσ=#{j:j<i<σ(j)<σ(i)orσ(i)<σ(j)i<j}, (13)
    nestiσ=#{j:j<i<σ(i)<σ(j)orσ(j)<σ(i)i<j}. (14)

    Let cros=ni=1crosi and nest=ni=1nesti.

    Let J2n+1(p,q,x,u,v,w) be the polynomials defined by the continued fraction expansion

    n0(1)nJ2n+1(p,q,x,u,v,w)z2n+1=z1+(u2+x2v2)[1]2p,qz2[1]p,q[2]2p,q[3]p,qx2w2z41+(u2+x2v2)[3]2p,qz2[3]p,q[4]2p,q[5]p,qx2w2z4, (15)

    where [n]p,q=(pnqn)/(pq).

    Theorem 2.4. We have

    J2n+1(p,q,x,u,v,w):=πDP2n+1p(2-13)πq(31-2)πxdesπudaπvddπwvalπ (16)
    =πDP2n+1pnestπqcrosπxexcπucddπv(cda+fix)πwcvalπ. (17)

    As J2n+1(x):=J2n+1(1,1,x,1,1,1), we derive

    J2n+1(x)=πDP2n+1xdesπ (18)
    =σDP2n+1xexcπ. (19)

    Eq. (18) is due to Flajolet-Françon[12].

    Theorem 2.5. We have

    J2n+1(p,q,x,u,v,w)=n/2k=0a2n+1,2k(p,q)(xw)2k(u2+v2x2)n2k, (20)

    where

    a2n+1,2k(p,q):=πDP2n+1,2kp(2-13)πq(31-2)π, (21)

    and

    DP2n+1,2k:={πDP2n+1,dd(π)=0,valπ=desπ=2k}.

    Moreover, for all 0kn/2, the following divisibility holds

    (p+q)2k|a2n+1,2k(p,q). (22)

    In particular, we obtain the following expansion of J2n+1(x) from (20).

    Corollary 1. For all n1, we have

    J2n+1(x)=n2k=0|DP2n+1,2k|x2k(1+x2)n2k. (23)

    Remark 1. Using context-free grammar Ma-Ma-Yeh-Zhou gave another interpretation of γ-coefficients in increasing trees, see [20,Eq. (14)] and [20,Corollary 20], it would be interesting to find a direct bijection between DP2n+1,2k and the γ-coefficients in [20].

    The second goal of this paper is to explore the coefficients in the Taylor series expansion of Jacobi elliptic functions cn(z,x) by generalizing the continued fractions of (7).

    Definition 2.6. For σSn, any entry σ(i) (i[n]) can be classified according to their cyclic ordinal type into four cases:

    ● a cyclic peak if i=σ1(x)<x and x>σ(x);

    ● a cyclic valley if i=σ1(x)>x and x<σ(x);

    ● a double excedance(resp. fixed point) if i=σ1(x)<x and x<σ(x)(resp. x=σ(x));

    ● a double drop if i=σ1(x)>x and x>σ(x).

    Let cpkσ (resp. cvalσ, cdaσ, cddσ, fixσ) be the number of cyclic peaks (resp. valleys, double excedances, double drops, fixed points) in σ.

    Definition 2.7. For σSn with convention 0–, a double ascent σ(i) of σ (i[n]) is said to be a foremaximum if σ(i) is a left-to-right maximum of σ, i.e., σ(j)<σ(i) for all 1j<i. Denote the number of foremaxima of σ by fmaxσ.

    For instance, lda(42157368)=3, but da(42157368)=2 and fmax(42157368)=2.

    Definition 2.8. A permutation π is said to be a left doubled permutation iff for all 0i(n2)/2, elements (i.e. values) 2i+1 and 2i+2 in π are of the same left ordinal type. The set of left doubled permutation is denoted by LDPn. A permutation π is said to be a cyclic doubled Permutation iff for all 0i(n2)/2, elements (i.e. values) 2i+1 and 2i+2 in π are of the same cyclic ordinal type. The set of cyclic doubled permutation is denoted by CDPn.

    Let J2n(p,q,x,u,v,,w,y) be the polynomials defined by the continued fraction expansion

    n0(1)nJ2n(p,q,x,u,v,w,y)z2n=11+y2z2[1]2p,q[2]2p,qx2w2z41+((qu[2]p,q+p2y)2+x2v2[2]2p,q)z2[3]2p,q[4]2p,qx2w2z4. (24)

    Theorem 2.9. We have

    J2n(p,q,x,u,v,w,y)=πLDP2np(2-31)πq(31-2)πxdesπuldaπfmaxπvlddπwlvalπyfmaxπ (25)
    =σCDP2npnestπqcrosπxexcπucddπvcdaπwcvalπyfixπ. (26)

    Since J2n(x)=J2n(1,1,x,1,1,1), we derive

    J2n(x)=πLDP2nxdesπ (27)
    =σCDP2nxexcπ. (28)

    Eq. (27) is due to Flajolet-Françon [12].

    When u=0 and t=v=1 we can write

    J2n(p,q,1,0,1,w,y):=k,j0b2n,2k,2j(p,q)w2ky2j, (29)

    where b2n,2k,2j(p,q) is a polynomial in p and q with non negative integral coefficients. Let CDP2n,2k,2j denote the subset of all the permutations σCDP2n with exactly 2k cyclic valleys, 2j fixed points, and without double drops, and let LDP2n,2k,2j denote the subset of all permutations σLDP2n with exactly 2k valleys and 2j double ascents, which are all foremaxima. We derive the following combinatorial interpretation of b2n,2k,2j(p,q) from Theorem 2.9.

    Corollary 2. We have

    b2n,2k,2j(p,q)=σCDP2n,2k,2jpnestσqcrosσ=σLDP2n,2k,2jp(2-31)σq(31-2)σ. (30)

    In particular, when j=0, we obtain

    b2n,2k,0(p,q)=σDD2n,2k,0pnestσqcrosσ=σDD2n,2k,0p(2-31)σq(31-2)σ, (31)

    where DD2n:={πCDP2n,fixπ=0}.

    Recall (see [22]) that a coderangement is a permutation without foremaximum. Let DD2n be the subset of LDP2n consisting of coderangements, that is, DDn={σLDP2n:fmaxσ=0}. Thus, DD2n,2k,0 is the subset of derangements σDD2n with exactly 2k cyclic valleys, and without double drops, and DD2n,2k,0 is the subset of coderangements σDDn with exactly 2k valleys and without double ascents. The following is our main result about the polynomial

    DD2n(p,q,x,u,v,w):=J2n(p,q,x,u,v,w,0).

    Theorem 2.10. We have

    DD2n(p,q,x,u,v,w)=(n)/2k=0b2n,2k,0(p,q)(xw)2k(q2u2+x2v2)n2k. (32)

    A pair of integers (i,j) is an inversion of σSn if i<j and σ(i)>σ(j). Let invσ be the inverion number of σ.

    As inv=exc+2nest+cros (cf. [16,Eq. (2.41)]), taking (p,q,x,u,v,w)=(q,1,x,1,1,1) (resp. (p,q,x,u,v,w)=(q2,q,xq,1,1,1)) in Eq. (32), we obtain the following corollary.

    Corollary 3. For all positive integers n and for each statistic stat{nest,inv},

    πDD2nqstatπxexcπ=n/2k=0(πDD2n,2k,0qstatπ)x2k(1+x2)n2k. (33)

    For any permutation σSn, we denote by cycσ the number of its cycles. We give the following expansion.

    Theorem 2.11. We have

    σDD2nqcycπxexcπ=n/2k=0(πDD2n,2k,0qcycπ)x2k(1+x2)n2k. (34)

    The rest of this paper is organized as follows. In Section 3, we recall some definitions and preliminaries of combinatorial theory of continued fractions. In Sections 4–7 we shall prove Theorem 2.4, Theorem 2.5, Theorem 2.9, Theorem 2.10 and Theorem 2.11, respectively. In Section 8, we refine the enumeration results on alternating permutations, which are related to the combinatorial interpretations of Jacobi elliptic functions.

    A Motzkin path of length n in the plan N×N is a sequence of points (s0,,sn), where s0=(0,0), sisi1=(1,0),(1,±1) and sn=(n,0). Each step (si1,si) is called East (resp. North-East, South-East) if sisi1=(1,0) (resp. sisi1=(1,1), sisi1=(1,1)). The height of the step (si1,si) denoted by hi is the ordinate of si1.

    A 2-Motzkin path is a Motzkin path consists of two types of horizontal steps, either blue or red. The set of 2-Motzkin path of length n1 is denoted by CMn. Denoting the North-East step (resp. East blue step, East red step, South-East step) by a (resp. b, b, c), see Figure 1 for a 2-Motzkin path. If we weight each East blue (resp. East red, North-East, South-East) step of height i by bi (resp. bi, ai and ci), and define the weight of γ by the product of its step weights denoted by w(γ). Then,

    n=0γCMnw(γ)zn=11(b0+b0)za0c1z21(b1+b1)za1c2z2. (35)
    Figure 1.  The doubled path γ.

    A 2-Motzkin path is a doubled path if the step at odd position is always followed by a step of the same type. See Figure 1 for a doubled path γ, whose wieght is w(γ)=a0a1b2b2c2c1a0a1c2c1b0b0.

    Grouping steps 2 by 2 in a doubled path of length 2n yields a 2-Motzkin path of length n, by (35) we obtain the following lemma.

    Lemma 3.1. If DM2n is the set of doubled paths of length 2n, then

    n=0γDM2nw(γ)zn=11(b02+b02)za0a1c2c1z21(b22+b22)za2a3c4c3z2. (36)

    Definition 3.2. A Laguerre history (restricted Laguerre history) of length n is a couple (γ,(p1,,pn)), where γ is a Motzkin path of length n and (p1,,pn) is a sequence satisfying 0pihi (resp. 0pihi1 if (si1,si) is East red and South east). Denote by LHn (resp. LHn) the set of Laguerre histories (resp. restricted Laguerre histories) of length n. Similarly, a doubled Laguerre history (restricted doubled Laguerre history) of length n is a couple (γ,(p1,,pn)), where γ is a doubled path of length n and (p1,,pn) is a sequence satisfying 0pihi (resp. 0pihi1 if (si1,si) is East red and South east). Denote by DHn (resp. DHn) the set of doubled Laguerre histories (resp. doubled restricted Laguerre histories) of length n.

    Clarke-Steingrímsson-Zeng [4] gave a direct bijection Φ on permutations converting statistic des into exc on permutations, and linking the restricted Françon-Viennot's bijection to Foata-Zeilberger bijection. As a variation of Φ, Shin and Zeng [23] constructed a bijection Ψ on permutations to derive a cycle version of linear statistics on permutations. Recently, Yan-Zhou-Lin [29] constructed a bijection ψYZL from Sn+1 to LHn. Han-Mao-Zeng [16] showed that Yan-Zhou-Lin's bijection ψYZL is a composition of Françon-Viennot's bijection and Shin-Zeng's bijection Ψ, see [16,Theorem 2.5]. Further, Han-Mao-Zeng also give another bijection Ψ on permutations converting statistic des into exc on permutations, see [16,Corollary 2.2].

    Lemma 4.1 (Han-Mao-Zeng). For σSn, we have

    (Val,Pk{n},Dd,Da)σ=(Cval,Cpeak,CdaFix,Cdd)Ψ(σ) (37)

    and

    ((2-13)i,(31-2)i)σ=(nesti,crosi)Ψ(σ)fori[n]. (38)

    Let

    wexσ=#{i[n1]:iσ(i)=σ(i)1}(=excσ).

    As exc=wex=cval+cda+fix, des=val+dd, by Lemma 4.1 and Definition 2.3, we obtain the following result.

    Theorem 4.2. Let ~Ψ be the restriction of Ψ on DP2n+1. Then ~Ψ is a bijection from DP2n+1 to DP2n+1. Moreover, for σDP2n+1, we have

    (2-13,31-2,des,da,dd,val)σ=(nest,cros,exc,cdd,cda+fix,cval)~Ψ(σ). (39)

    Proof of Theorem 2.4. For i[2n+1], define (31-2)kσ, (2-31)kσ and (2-13)kσ for σDP2n+1 by

    (31-2)kσ=#{i:i+1<j and σ(i+1)<σ(j)=k<σ(i)},(2-31)kσ=#{i:j<i1 and σ(i)<σ(j)=k<σ(i1)},(2-13)kσ=#{i:j<i1 and σ(i1)<σ(j)=k<σ(i)}.

    We use Françon-Viennot's bijection ΨFV:DP2n+1DH2n. For any σDP2n+1, the doubled Laguerre history (s0,,s2n,p1,,p2n) is constructed as follows. Let s0=(0,0) and for i=1,,2n,

    ● the step (si1,si) is North-East if i is a valley,

    ● the step (si1,si) is South-East if i is a peak,

    ● the step (si1,si) is East blue if i is a double ascent,

    ● the step (si1,si) is East red if i is a double descent.

    While pi=(2-13)iσ for i=1,,2n.

    According to definition of hi, (31-2)1σ+(2-13)1σ=0=h1. For i>1, if i is a valley, we have

    (31-2)iσ+(2-13)iσ={(31-2)i1σ+(2-13)i1σ1if i1 is a peak,(31-2)i1σ+(2-13)i1σ+1if i1 is a valley,(31-2)i1σ+(2-13)i1σif i1 is a double ascent,(31-2)i1σ+(2-13)i1σif i1 is a double descent.

    By inductions we have

    (31-2)iσ+(2-13)iσ=hiif i is a valley.

    Similarly, it is not difficult to prove by induction that (31-2)iσ+(2-13)iσ=hi if i is a peak, double ascent or double descent.

    Since σ(0)=σ(2n+2)=0, so 2n+1 must be a peak and valσ=pkσ1. Thus (s0,,s2n,p1,,p2n) is a doubled Laguerre history of length 2n and

    w(σ)=xERγ+NEγuEBγvERγwNEγ2ni=1ppiqhipi,

    where NEγ, EBγ, and ERγ are the number of North-East steps, East blue steps, and East red steps of γ. Therefore,

    J2n+1(p,q,x,u,v,w)=γDM2nxERγ+NEγuEBγvERγwNEγ2ni=1[hi+1]p,q, (40)

    where [n]p,q=(pnqn)/(pq). Given a doubled path γ, the weight of each step at height k is created by using the following rules:

    ak:=xw[k+1]p,q,bk:=u[k+1]p,q,bk:=xv[k+1]p,q,ck:=[k+1]p,q, (41)

    if the step is North-East, East blue, East red and South-East, respectively, and the weight of γ is defined to be the product of the step weights. Summing over all the doubled paths of length 2n with the rules (41), we have

    J2n+1(p,q,x,u,v,w)=γDM2nw(γ). (42)

    By Lemma 3.1, J2n+1(p,q,x,u,v,w) are the coefficients in the following continued fraction expansion,

    n0J2n+1(p,q,x,u,v,w)zn=11(u2+x2v2)[1]2p,qz[1]p,q[2]2p,q[3]p,qx2w2z21(u2+x2v2)[3]2p,qz[3]p,q[4]2p,q[5]p,qx2w2z2, (43)

    by transforming z to z2 and multiplying both sides by z, we obtain (16) immediately. This completes the proof of (16). This lead to (17) combining (39) and (16).

    Proof of Theorem 2.5. In view of (43), for 0kn/2, let a2n+1,2k(p,q,x,u,v) be the coefficient of w2k in A2n+1(p,q,x,u,v,w), i.e.,

    J2n+1(p,q,x,u,v,w)=n/2k=0a2n+1,2k(p,q,x,u,v)w2k. (44)

    Transforming z and w to z(u2+x2v2) and w(u2+x2v2)x in (43), respectively, we obtain

    n0n/2k=0a2n+1,2k(p,q,x,u,v)x2k(u2+x2v2)n2kw2kzn=11[1]2p,qz[1]p,q[2]2p,q[3]p,qw2z21[3]2p,qz[3]p,q[4]2p,q[5]2p,qw2z21[5]2p,qz[5]p,q[6]2p,q[7]p,qw2z2. (45)

    Since the right-hand side of the above identity is free of variables x, u, and v, the coefficient of w2kzn in the left-hand side is a polynomial in p and q with nonnegative integral coefficients. Denote the coefficient of (45) by

    P2n+1,2k(p,q):=a2n+1,2k(p,q,x,u,v)x2k(u2+x2v2)n2k.

    On the other hand, Take (p,q,x,u,v,w)=(p,q,1,1,0,w) in (44), then the continued fraction (43) becomes the right-hand side of (45) immediately. With the definition of a2n+1,2k in (21), we see that

    P2n+1,2k(p,q)=a2n+1,2k(p,q,1,1,0)=a2n+1,2k(p,q).

    With Eq. (44), this proves (20). Finally, since (p+q)2|[2n1]p,q[2n]2p,q[2n+1]p,q for all n1, each w2 appears with a factor (p+q)2 in the right-hand side of (45), and the polynomial P2n+1,2k(p,q) is divisible by (p+q)2k. This completes the proof. In the rest of this section, we will provide a combinatorial proof of Corollary 1 via the modified Foata-Strehl actions on permutations.

    Definition 5.1 (MFS-action). Let πSn with boundary condition π(0)=π(n+1)=0, for any a[n], the a-factorization of π reads π=w1w2aw3w4, where w2 (resp. w3) is the maximal contiguous subword immediately to the left (resp. right) of a whose letters are all larger than a. Following Foata and Strehl [14] we define the action φa by

    φa(π)=w1w3aw2w4.

    Note that if a is a double ascent (resp. double descent), then w2= (resp. w3=), and if a is a peak then w2=w3=. For instance, if a=3 and π=28531746S7, then w1=2,w2=85,w3= and w4=1746. Thus φa(π)=23851746. Clearly, φa is an involution acting on Sn and it is not hard to see that φa and φb commute for all a,b[n]. Brändén [3] modified the map φa to be

    φa(π):={φa(π),if a is not a valley of π;π,if a is a valley of π.

    See Figure 2 for illustration, where exchanging w2 and w3 in the a-factorisation is equivalent to move a from a double ascent to a double descent or vice versa. Note that the boundary condition does matter. Take the permutation 569173428 in Figure 2 as an example. If π(0)=10 instead, then 5 becomes a valley and will be fixed by φ5.

    Figure 2.  MFS-actions on 569174328 (recall π(0)=π(10)=0).

    It is clear that φa's are involutions and commute. For any subset S[n] we can then define the map φS:DP2n+1DP2n+1 by

    φS(π)=aSφ2a1(π)φ2a(π).

    Note that φ2n+1(π)=π and the concatenation of φ2a1(π)φ2a(π) is closed for πDP2n+1. Hence the group Zn2 acts on DP2n+1 via the functions φS, S[n]. This action will be called the Modified Foata–Strehl action (MFS-action for short).

    Proof of Theorem 1. For any permutation πDP2n+1, let Orb(π)={g(π):gZn2} be the orbit of π under the MFS-action. The MFS-action divides the set DP2n+1 into disjoint orbits. Moreover, for πDP2n+1, 2a1 and 2a are double descents (resp. double ascents) of π if and only if 2a1 and 2a are double ascents (resp. double descents) of φ2a1(π)φ2a(π). Double descents (resp. double ascents) 2a1 and 2a of π remains a double descent (resp. double ascent) of φ2b1(π)φ2b(π) for any ba. Hence, there is a unique permutation in each orbit which has no double descent. Let ˉπ be this unique element in Orb(π), then daˉπ=2n+1pkˉπvalˉπ and desˉπ=pkˉπ1=valˉπ. And for any other πOrb(π), it can be obtained from ˉπ by repeatedly applying φ2a1 and φ2a for some double ascents 2a1 and 2a of ˉπ. Once φ2a1φ2a is used, des2 increases by 1 and da2 decreases by 1. Thus

    σOrbπxdesσ2=xdesˉπ2(1+x)daˉπ2=xdesˉπ2(1+x)ndesˉπ.

    By summing over all the orbits that compose together to form DP2n+1, we obtain

    πDP2n+1xdes2π=n2k=0|DP2n+1,2k|xk(1+x)n2k,

    by transforming x to x2, (23) is derived immediately.

    We need the following result[16,Lemma 2.1].

    Lemma 6.1 (Shin-Zeng). For σSn, we have

    (Lval,Lpk,LdaFmax,Fmax,Ldd)σ (46)
    =(Cval,Cpeak,Cda,Fix,Cdd)(Φ(σ)) (47)
    =(Cval,Cpeak,Cda,Fix,Cdd)(Φ(σ))1, (48)

    and

    ((2-31)i,(31-2)i)σ=(nesti,crosi)(Φ(σ))1fori[n]. (49)

    As exc=cval+cda, des=lpk+ldd=lval+ldd, by Lemma 6.1 and Definition 2.8, we obtain the following result.

    Theorem 6.2. Let ˜Φ be the restriction of Φ on LDP2n. Then ˜Φ is a bijection from LDP2n to CDP2n. Moreover, for σLDP2n, we have

    (2-31,31-2,des,ldafmax,ldd,lval,fmax)σ=(nest,cros,exc,cdd,cda,cval,fix)(˜Φ(σ))1. (50)

    Proof of Theorem 2.9. Using Foata-Zeilberger's bijection ΨFZ:CDP2nDH2n, the restricted doubled Laguerre history (s0,,s2n,p1,,p2n) is constructed as follows. Define s0=(0,0) and

    ● the step (si1,si) is North-East if i is a cyclic valley,

    ● the step (si1,si) is South-East if i is a cyclic peak,

    ● the step (si1,si) is East blue if i is a double drop (or fixed point),

    ● the step (si1,si) is East red if i is a double excedance,

    while pi=nestiσ for i=1,,2n. Then, we have

    nestiσ+crosiσ={hi,if (si1,si) is North-East;hi1,if (si1,si) is South-East;hi,if (si1,si) is East blue;hi1,if (si1,si) is East red.

    Thus (s0,,s2n,p1,,p2n) is a restricted doubled Laguerre history of length 2n and

    w(σ)=xERγ+NEγuEBγvERγwNEγyEBγqNEγ+EBγ2ni=1ppiqhi1pi,

    where NEγ, EBγ, and ERγ are the number of North-East steps, East blue steps, and East red steps of γ and EBγ is the number of East blue steps whose height is equal to pi. Given a doubled path γ, the weight of each step at height k is created by using the following rules:

    ak:=xw[k+1]p,q,bk:=ypk+qu[k]p,q,bk:=xv[k]p,q,ck:=[k]p,q, (51)

    if the step is North-East, East blue, East red and South-East, respectively, and the weight of γ is defined to be the product of the step weights. Summing over all the doubled paths of length 2n with the rules (51), we have

    J2n(p,q,x,u,v,w,y)=γDM2nw(γ). (52)

    By Lemma 3.1, J2n(p,q,x,u,v,w,y) are the coefficients in the following continued fraction expansion,

    n0J2n(p,q,x,u,v,w,y)zn=11y2z[1]2p,q[2]2p,qx2w2z21((qu[2]p,q+p2y)2+x2v2[2]2p,q)z[3]2p,q[4]2p,qx2w2z2. (53)

    By transforming z to z2 in (53), we obtain (24) immediately. This completes the proof of (26). This lead to (25) combining (50) and (26).

    Proof of Theorem 2.10. The generating function of the right side of Eq. (32) is

    n0n/2k=0(πDD2n,2k,0pnestπqcrosπ)(xw)2k(q2u2+x2v2)n2kzn (54)
    =n0π~DD2npnestπqcrosπ(xwq2u2+x2v2)cvalπ((q2u2+x2v2)z)n, (55)

    where ~DD2n:=nk=0DD2n,2k,0. Using Theorem 2.9, we have

    J2n(p,q,1,0,1,w,0):=π~DD2npnestπqcrosπwcvalπ.

    Eq. (53) implies that

    1+n1π~DD2npnestπqcrosπwcvalπzn=11[1]2p,q[2]2p,qw2z21[2]2p,qz[3]2p,q[4]2p,qw2z21[4]2p,qz.

    Making the substitution z(q2u2+x2v2)z and wxw/(q2u2+x2v2) in the above equation, we obtain the continued fraction of (55) is

    11[1]2p,q[2]2p,qx2w2z21(q2u2[2]2p,q+x2v2[2]2p,q)z[3]2p,q[4]2p,qx2w2z21(q2u2[4]2p,q+x2v2[4]2p,q)z, (56)

    which is generating function of n0J2n(p,q,x,u,v,w,0)zn by (53). This completes the proof.

    We need the following lemma. Let

    Dn(q,t,u,v,w):=σDnqcycσxexcσucdaσvcddσwcvalσ. (57)

    Lemma 7.1. [23,Eq. (41)] We have

    1+n=1Dn(q,x,u,v,w)zn=110(xu+v)z1(q+0)xwz211(xu+v)z2(q+1)xwz212(xu+v)z3(q+2)xwz2. (58)

    Define Dcyc2n(β,x,u,v,w) to be the coefficients in the following continued fraction expansion

    1+n1(1)nDcyc2n(β,x,u,v,w)z2n=11+b0z2λ1x2w2z41+b1z2λ2x2w2z4, (59)

    where, for k0,

    bk=(2k)2(x2u2+v2),andλk+1=(2k+1)(2k+2)(β+2k)(β+2k+1).

    Lemma 7.2. We have

    Dcyc2n(β,x,u,v,w):=πDD2nβcycπxexcπucdaπvcddπwcvalπ. (60)

    Proof of Lemma 7.2. Comparing the definition of (57) and (60), observing the Eq. (58), we constuct a doubled path γ, the weight is created by using the following rules:

    bk+bk:=k(xu+v)andakck+1:=(k+1)(β+k)xw, (61)

    where ak (resp. bk, bk and ck) is the weight of North-East (resp. East blue, East red and South-East) step at height k. The weight of γ is defined to be the product of the step weights. Summing over all the doubled paths of length 2n with the rules (61), we have

    Dcyc2n(β,x,u,v,w)=γDM2nw(γ).

    By Lemma 3.1, Dcyc2n(β,x,u,v,w) are the coefficients in the following continued fraction expansion,

    1+n1Dcyc2n(β,x,u,v,w)zn=110(x2u2+v2)z2β(β+1)x2w2z2122(x2u2+v2)z3(β+2)4(β+3)x2w2z2, (62)

    which is equivalent to (59) by transforming z to (z)2.

    Proof of Thereom 2.11. Then the generating function of the right side of Eq. (34) is

    1+n1n/2k=0(πDD2n,2k,0qcycπ)x2k(1+x2)n2kzn (63)
    =1+n1π~DD2nqcycπ(x1+x2)cvalπ((1+x2)z)n. (64)

    Using Lemma 7.2, we have

    Dcyc2n(β,1,1,0,w):=π~DD2nβcycπwcvalπ.

    Eq. (62) implies that

    1+n1π~DD2nβcycπwcvalπzn=110z2β(β+1)w2z21221z3(β+2)4(β+3)w2z2. (65)

    Making the substitution z(1+x2)z and wx/(1+x2) in the above equation, we obtain the continued fraction of (64) is

    110(1+x2)z2β(β+1)x2z2122(1+x2)z3(β+2)4(β+3)x2z2, (66)

    which is generating function of 1+n1Dcyc2n(β,x,1,1,1)zn by (62). This completes the proof.

    A permutation σ=σ1σ2σnSn is alternating (resp. falling alternating) permutation if σ1<σ2, σ2>σ3, σ3<σ4, etc. (resp. σ1>σ2, σ2<σ3, σ3>σ4, etc.). Let An (resp. An) be the set of alternating (resp. falling alternating) permutations on [n]. Let evalπ (resp. oval) and opkπ (resp. epk) denote the number of even valleys (resp. odd valleys) and odd peaks of π (resp. even peaks).

    A Dyck path is a Motzkin path without horizontal step. So the length of a Dyck path must be even. Let Dyck2n denote the set of Dyck paths of length 2n. Then, it is well known (see [12]) that

    1+n1γDyck2nw(γ)z2n=11a0c1z21a1c2z21a2c3z2. (67)

    Recall Definition 3.2, let Dyck path diagram (resp. restricted Dyck path diagram) of length 2n be the Lagurre history (restriced Laguerre history) of length 2n without east steps. Denote by P2n (resp. P2n) the set of Dyck path diagram (restricted Dyck path diagram) of length 2n. There are several well-known bijections between A2n and P2n1 and P2n, see [22] and references therein.

    We also need a standard contraction formula for continued fractions, see [22,Eq. (44)].

    Lemma 8.1 (Contraction formula). There holds

    11c1z1c2z1c3z1c4z1=11c1zc1c2z21(c2+c3)zc3c4z21.

    Define the polynomials En(p,q,x,y) by the continued fraction expansions

    n=0(1)nE2n(p,q,x,y)z2n=11+[1]2p,qy2z21+[2]2p,qx2z21+[3]2p,qy2z21+[4]2p,qx2z2 (68)
    =1y2z2+y2((p+q)2x2+y2)z4+,

    and

    n=0(1)nE2n+1(p,q,x,y)z2n+1=xz1+[1]p,q[2]p,qy2z21+[2]p,q[3]p,qx2z21+[3]p,q[4]p,qy2z21+[4]p,q[5]p,qx2z2=xz(p+q)xy2z3+((p+q)2(p2+pq+q2)x3y2+(p+q)2xy4)z5+. (69)

    We have the following combinatorial interpretations for En(p,q,x,y).

    Theorem 8.2. For n0, we have

    E2n(p,q,x,y)=πA2np(2-31)πq(31-2)πxevalπ+opkπyovalπ+epkπ, (70)
    E2n+1(p,q,x,y)=πA2n+1p(2-13)πq(31-2)πxevalπ+opkπyovalπ+epkπ. (71)

    Proof. We prove the Eq. (70) and Eq. (71) by using Françon-Viennot's bijection ΨFV:A2n+1P2n and ΨFV:A2nP2n. For σA2n+1, the corresponding Dyck path diagram (s0,,s2n,ξ1,,ξ2n) is constructed as follows: Let s0=(0,0) and for i=1,,2n,

    ● the step (si1,si) is North-East if i is a valley,

    ● the step (si1,si) is South-East if i is a peak.

    While ξi=(31-2)iσ for i=1,,2n. We only prove Equation (70) and leave (71) to the interested reader.

    For any σ=σ1σ2σ2nA2n, let σ=σ1σ2σ2nσ2n+1 with σ2n+1=2n+1. Let ΨFV(σ):=ΨFV(σ). Since 1 is the valley then (31-2)1σ+(2-31)1σ=0=h1, and for i>1,

    (31-2)iσ+(2-31)iσ={(31-2)i1σ+(2-31)i1σ+1if i1 is a valley and i is a valley,(31-2)i1σ+(2-31)i1σ1if i1 is a peak and i is a peak,(31-2)i1σ+(2-31)i1σif i1 is a valley and i is a peak,(31-2)i1σ+(2-31)i1σif i1 is a peak and i is a valley,

    by induction we have

    (31-2)iσ+(2-31)iσ={hiif i is a valley,hi1if i is a peak.

    Therefore,

    w(σ)=xENEγ+OSEγyONEγ+ESEγqNEγ2ni=1phi1ξiqξi,

    where NEγ, SEγ, ENEγ, ONEγ, ESEγ and OSEγ are the number of North-East steps, South-East steps, North-East steps at even positions, North-East steps at odd positions, South-East steps at even positions, and South-East steps at odd positions. By inductions it is easy to see that the the height h2i (resp. h2i+1) of even step (s2i1,s2i)(1in) (resp. odd step (s2i,s2i+1)(0in1)) of Dyck path is odd (resp. even). For example, σ=645231 gives the path (ONE,ENE,OSE,ENE,OSE,ESE) and the weight (y,xp,xq,xp,xq,y). Let [n]p,q=(pnqn)/(pq), given a Dyck path γ, the weight of each step is created by using the following rules:

    a2k:=[2k+1]p,qy,a2k+1:=[2k+2]p,qx,c2k:=[2k]p,qx,c2k+1:=[2k+1]p,qy, (72)

    if the step is North-East at height 2k, North-East at height 2k+1, South-East at height 2k, and South-East at height 2k+1, respectively, and the weight of γ is defined to be the product of the step weights. Summing over all the doubled paths of length 2n with the rules (72), we have

    E2n(p,q,x,y)=γDyck2nw(γ). (73)

    By (67), J2n(p,q,x,y) are the coefficients in the following continued fraction expansion,

    n=0E2n(p,q,x,y)z2n=11[1]2p,qy2z21[2]2p,qx2z21[3]2p,qy2z21[4]2p,qx2z2. (74)

    By transforming z2 to z2 for the above equation, we obtain (68) immediately, This completes the proof of Eq. (70).

    Remark 2. By Lemma 8.1 it is easy to check that

    E2n(p,q,x,1)=J2n(p,q,x,1,1,1,1), (75)
    E2n+1(1,1,1,1)=J2n+1(1,1,1,1,1,1). (76)

    Given a Dyck path Dyck2n, a North-East step at positions (s2i1,s2i)(1in) is matched by some South-East step at (s2i,s2i+1)(0in1), i.e., the number of North-East even steps is equal to the number of South-East odd steps. From the Françon-Viennot's bijection, the number of even valleys is equal to the number of odd peaks for πA2n. Therefore, when p=q=1, (70) reduces to Flajolet's result [12,Theorem 4].

    2. When x=y=1, (70) and (71) reduce to Shin-Zeng's result [22,Theorem 4].

    3. Dumont [10,Propostion 7] obtained E2n(1,1,x,y) by enumerating cycle-alternating permutations with distinct weights for even and odd cycle peaks. Further refinements of E2n(p,q,x,y) were given in [25,Section 2.15] with combinatorial interpretations in terms of cycle-alternating permutations.

    The author thanks Prof. Jiang Zeng for his inspiring discussions and useful comments. Most of the present work was done during his PhD at Institut Camille Jordan, Université Claude Bernard Lyon 1 in 2018-2019.



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  • This article has been cited by:

    1. Bin Han, The γ-positive coefficients arising in segmented permutations, 2021, 344, 0012365X, 112336, 10.1016/j.disc.2021.112336
    2. Bin Han, Gamma-positivity of derangement polynomials and binomial Eulerian polynomials for colored permutations, 2021, 182, 00973165, 105459, 10.1016/j.jcta.2021.105459
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