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Research article

On hypergeometric Cauchy numbers of higher grade

  • Received: 26 February 2021 Accepted: 13 April 2021 Published: 19 April 2021
  • MSC : 11B75, 11B37, 11C20, 15A15, 33C05

  • In 1875, Glaisher gave several interesting determinant expressions of numbers, including Bernoulli, Cauchy, and Euler numbers. Cauchy numbers can be generalized to the hypergeometric Cauchy numbers. Recently, Barman et al. study more general numbers in terms of determinants, which involve Bernoulli, Euler and Lehmer's generalized Euler numbers. However, Cauchy numbers and their generalizations are not involved in these generalized numbers. In this paper, we study more general numbers in terms of determinants, which involve Cauchy numbers. The motivations and backgrounds of the definition are in an operator related to graph theory. We also give several expressions and identities by Trudi's and inversion formulae.

    Citation: Takao Komatsu, Ram Krishna Pandey. On hypergeometric Cauchy numbers of higher grade[J]. AIMS Mathematics, 2021, 6(7): 6630-6646. doi: 10.3934/math.2021390

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  • In 1875, Glaisher gave several interesting determinant expressions of numbers, including Bernoulli, Cauchy, and Euler numbers. Cauchy numbers can be generalized to the hypergeometric Cauchy numbers. Recently, Barman et al. study more general numbers in terms of determinants, which involve Bernoulli, Euler and Lehmer's generalized Euler numbers. However, Cauchy numbers and their generalizations are not involved in these generalized numbers. In this paper, we study more general numbers in terms of determinants, which involve Cauchy numbers. The motivations and backgrounds of the definition are in an operator related to graph theory. We also give several expressions and identities by Trudi's and inversion formulae.



    In 1935, D. H. Lehmer [20] introduced and investigated generalized Euler numbers Wn, defined by the generating function

    3et+eωt+eω2t=n=0Wntnn!, (1.1)

    where ω=1+32 and ω2=ˉω=132 are the cube roots of unity. Notice that Wn=0 unless n0(mod3). The sequence of these numbers is given by

    W3n}n0=1,1,19,1513,315523,136085041,105261234643,132705221399353,254604707462013571,

    and the sequence of these absolute values is recorded in [22,A002115]. In [15], the complementary numbers W(j)n (j=0,1,2) to Lehmer's Euler numbers are defined by the generating function

    n=0W(j)ntnn!=(1+l=1t3l(3l+j)!)1. (1.2)

    Notice that W(j)n=0 unless n0(mod3). When j=0, Wn=W(0)n are the original Lehmer's Euler numbers. When j=1, we also have

    n=0W(1)ntnn!=3tet+ω2eωt+ωeω2t. (1.3)

    Lehmer's Euler numbers and their complementary numbers W(j)n can be considered analogous of the classical Euler numbers En and their complementary Euler numbers ˆEn ([11,19]). For, their generating functions are given by

    n=0Entnn!=1cosht=2et+et=(l=0t2l(2l)!)1 (1.4)

    and

    n=0ˆEntnn!=tsinht=2tetet=(l=0t2l(2l+1)!)1, (1.5)

    respectively. Still similar numbers are the well-known classical Bernoulli numbers defined by

    n=0Bntnn!=tet1=(l=0tl(l+1)!)1. (1.6)

    Recently, Barman et al. ([3]) introduce more general numbers, so-called hypergeometric Lehmer-Euler numbers W(j)N,n,r (j=0,1) of grade r, defined by

    n=0W(j)N,n,rtnn!=(1Fr(1;rN+j+1r,rN+j+2r,,rN+j+rr;(tr)r))1=(1+n=1(rN+j)!(rN+rn+j)!trn)1(N0),

    where 1Fr(a;b1,,br;z) is the hypergeometric function, defined by

    1Fr(a;b1,,br;z)=n=0(a)(n)(b1)(n)(br)(n)znn!.

    and (x)(n)=x(x+1)(x+n1) (n1) is the rising factorial with (x)(0)=1. A determinant expression is given by

    W(j)N,n,r=(1)n(rn)!|(rN+j)!(rN+j+r)!10(rN+j)!(rN+j+2r)!(rN+j)!(rN+j+r)!10(rN+j)!(rN+rn+jr)!(rN+j)!(rN+rn+j2r)!(rN+j)!(rN+j+r)!1(rN+j)!(rN+rn+j)!(rN+j)!(rN+rn+jr)!(rN+j)!(rN+j+2r)!(rN+j)!(rN+j+r)!|. (1.7)

    When N=0 and r=3, W(j)n=W(j)0,n,3 are the Lehmer's generalized Euler numbers (j=0) in (1.1) and their complementary numbers (j=1) in (1.3). When N=0 and r=2, En=W(j)0,n,2 are the classical Euler numbers (j=0) in (1.4) and their complementary numbers (j=1) in (1.5). A famous determinant expression of Euler numbers discovered by Glaisher in 1875 ([6,p.52])

    E2n=(1)n(2n)!|121014!12101(2n2)!1(2n4)!1211(2n)!1(2n2)!14!12| (1.8)

    and an expression of the complementary numbers ([11,19])

    ˆE2n=(1)n(2n)!|13!1015!13!101(2n1)!1(2n3)!13!11(2n+1)!1(2n1)!15!13!|. (1.9)

    When r=1 and j=0, BN,n=W(0)N,n,1 are the hypergeometric Bernoulli numbers. When N=r=1 and j=0 in (1.7), Bn=W(0)1,n,1 are the classical Bernoulli numbers in (1.6). The determinant expression for the classical Bernoulli numbers was discovered by Glaisher ([6,p.53]).

    Bn=(1)nn!|121013!12101n!1(n1)!1211(n+1)!1n!13!12|. (1.10)

    However, the classical Cauchy numbers and their generalized numbers are not involved in the numbers W(j)N,n,r. Hypergeometric Cauchy numbers cN,n ([9]) are defined by

    12F1(1,N;N+1;t)=(1)N1tN/Nlog(1+t)N1n=1(1)n1tn/n=n=0cN,ntnn!, (1.11)

    where 2F1(a,b;c;z) is the hypergeometric function defined by

    2F1(a,b;c;z)=n=0(a)(n)(a)(b)(c)(n)znn!.

    When N=1, cn=c1,n are the classical Cauchy numbers defined by

    tlog(1+t)=n=0cntnn!. (1.12)

    The determinant expression of hypergeometric Cauchy numbers is given by

    cN,n=n!|NN+110NN+2NN+110NN+n1NN+n2NN+11NN+nNN+n1NN+2NN+1| (1.13)

    ([2,18]). The determinant expression for the classical Cauchy numbers was discovered by Glaisher ([6,p.50]). Other generalized Cauchy numbers, having similar properties, are Leaping Cauchy numbers [13] and Shifted Cauchy numbers [16].

    A generalized version for Bernoulli and Euler numbers has been established in [17], where the elements contain factorials, as seen in (1.8), (1.9), (1.10) and (1.7). However, expressions for Cauchy and their generalized numbers cannot be included because they do not contain the factorial elements, as seen in (1.13). Universal Bernoulli numbers were studied in [1] and [8], and particularly, some universal Kummer congruences were established in [1] and [8].

    In this paper, we introduce the hypergeometric Cauchy numbers of higher grade that are introduced as generalizations of both hypergeometric Cauchy numbers and the classical Cauchy numbers. We give several expressions and identities.

    For N1 and n0, define hypergeometric Cauchy numbers V(j)N,n,r (j=0,1) of grade r by

    n=0V(j)N,n,rtnn!=(2F1(1,N+jr;N+1+jr;(t)r))1, (2.1)

    where 2F1(a,b;c;z) is the Gauss hypergeometric function, defined by

    2F1(a,b;c;z)=n=0(a)(n)(b)(n)(c)(n)znn!.

    From the definition, V(j)N,n,r0(modr) unless n0(modr). When r=1 and j=0 in (2.1), cN,n=V(0)N,n,1 are the hypergeometric Cauchy numbers in (1.11). When N=1, r=1 and j=0 in (2.1), cn=V(0)1,n,1 are the classical Cauchy numbers in (1.12).

    We can write (2.1) as

    2F1(1,N+jr;N+1+jr;(t)r)=n=0(1)n(rN+j)rN+rn+jtrn=1+n=1(1)n(rN+j)rN+rn+jtrn. (2.2)

    The definition (2.1) with (2.2) may be obvious or artificial for the readers with different backgrounds. However, our initial motivations were from Combinatorics, in particular, graph theory. In 1989, Cameron [5] considered the operator A defined on the set of sequences of non-negative integers as follows: for x={xn}n1 and z={zn}n1, set Ax=z, where

    1+n=1zntn=(1n=1xntn)1. (2.3)

    Cameron's operators deal with only nonnegative integers, but the operators can be used extensively for rational numbers. In the sense of Cameron's operator A, we have the following relation.

    A{(1)n1(rN+j)rN+rn+j}={V(j)N,rn,r(rn)!}

    This relation is interchangeable in the sense of determinants too. See Section 5 about Trudi's formula.

    We have the following recurrence relation.

    Proposition 1. For N0 and j=0,1, we have

    V(j)N,rn,r=n1k=0(1)nk1(rn)!(rN+j)(rN+rnrk+j)(rk)!V(j)N,rk,r(n1)

    with V(j)N,0,r=1.

    Proof. By (2.1), we get

    1=(1+l=1(1)l(rN+j)rN+rl+jtrl)(n=0V(j)N,rn,rtrn(rn)!)=n=0V(j)N,rn,rtrn(rn)!+n=1n1k=0(1)nk(rN+j)V(j)N,rk,r(rN+rnrk+j)(rk)!trn.

    Comparing the coefficient on both sides, we obtain

    V(j)N,rn,r(rn)!+n1k=0(1)nk(rN+j)V(j)N,rk,r(rN+rnrk+j)(rk)!=0(n1).

    We have an explicit expression of V(j)N,n,r.

    Theorem 1. Let j=0,1. For n1,

    V(j)N,rn,r=(rn)!nk=1(1)nki1++ik=ni1,,ik1(rN+j)k(rN+ri1+j)(rN+rik+j).

    Proof. The proof is done by induction on n. From Proposition 1 with n=1,

    V(j)N,r,r=r!(rN+j)rN+j+rV(j)N,0,r=r!(rN+j)rN+j+r.

    This matches the result when n=1. Assume that the result is valid up to n1. Then by Proposition 1

    V(j)N,rn,r(rn)!=n1l=0(1)nl1(rN+j)rN+rnrl+jV(j)N,rl,r(rl)!=n1l=1(1)nl1(rN+j)rN+rnrl+jlk=1(1)lki1++ik=li1,,ik1(rN+j)k(rN+ri1+j)(rN+rik+j)+(1)n1(rN+j)rN+rn+j=n1k=1(1)nk1n1l=k(rN+j)rN+rnrl+ji1++ik=li1,,ik1(rN+j)k(rN+ri1+j)(rN+rik+j)+(1)n1(rN+j)rN+rn+j=nk=2(1)nkn1l=k1rN+jrN+rnrl+ji1++ik1=li1,,ik11(rN+j)k1(rN+ri1+j)(rN+rik1+j)+(1)n1(rN+j)rN+rn+j=nk=2(1)nki1++ik=ni1,,ik1(rN+j)k(rN+ri1+j)(rN+rik+j)+(1)n1(rN+j)(rN+rn+j)(nl=ik)=nk=1(1)nki1++ik=ni1,,ik1(rN+j)k(rN+ri1+j)(rN+rik+j).

    There is an alternative form of V(j)N,n,r by using binomial coefficients. The proof is similar to that of Theorem 1 and is omitted.

    Theorem 2. For n1,

    V(j)N,rn,r=(rn)!nk=1(1)nk(n+1k+1)i1++ik=ni1,,ik0(rN+j)k(rN+ri1+j)(rN+rik+j).

    In this section, we shall show an expression of hypergeometric Cauchy numbers of higher grade in terms of determinants. This result is a generalization of those of the hypergeometric and the classical Cauchy numbers. For simplification of determinant expressions, we use the Jordan matrix

    J=(0000100001000010).

    J0 is the identity matrix and JT is the transpose matrix of J.

    Theorem 3. For n1,

    V(j)N,rn,r=(rn)!|JT+nk=1rN+jr(N+k)+jJk1|.

    Proof. For simplicity, put ˜VN,n=V(j)N,n,r/n!. Then, we shall prove that for any n1

    ˜VN,rn=|JT+nk=1rN+jr(N+k)+jJk1|. (3.1)

    When n=1, (3.1) is valid because by Theorem 1 we get

    ˜VN,r=rN+jrN+j+r.

    Assume that (3.1) is valid up to n1. Notice that by Proposition 1, we have

    ˜VN,rn=n1k=0(1)nk1(rN+j)rN+rnrk+j˜VN,rk.

    Thus, by expanding the right-hand side of (3.1) along the first row, it is equal to

    rN+jrN+j+r˜VN,rnr|rN+jrN+j+2r10rN+jrN+j+3rrN+jrN+j+r10rN+jrN+rn+jrrN+jrN+rn+j3rrN+jrN+j+r1rN+jrN+rn+jrN+jrN+rn+j2rrN+jrN+j+2rrN+jrN+j+r|=rN+jrN+j+r˜VN,rnrrN+jrN+j+2r˜VN,rn2r++(1)n|rN+jrN+rn+jr1rN+jrN+rn+jrN+jrN+j+r|=n1k=0(1)nk1(rN+j)rN+rnrk+j˜VN,rk=˜VN,rn.

    Remark. When r=1 and j=0, the determinant expression in Theorem 3 is reduced to that in (1.13) for the hypergeometric Cauchy numbers cN,n=V(0)N,n,1. When N=1, r=1 and j=0, we have a determinant expression of the Cauchy numbers cn=V(0)1,n,1 ([6,p.50]).

    As applications or variations to generalize the hypergeometric numbers V(j)N,n,r of higher grade, we shall introduce two kinds of incomplete hypergeometric Cauchy numbers of higher grade. Similar but slightly different kinds of incomplete numbers are considered in [10,12,14,17]. In addition, similar techniques can be found in [24] and later cited in [7]. For j=0,1 and nm1, define the restricted hypergeometric Cauchy numbers V(j)N,n,r,m of grade r by

    n=0V(j)N,n,r,mtnn!=(1+ml=1(1)l(rN+j)rN+rl+jtrl)1 (4.1)

    and the associated hypergeometric Cauchy numbers V(j)N,n,r,m of grade r by

    n=0V(j)N,n,r,mtnn!=(1+l=m(1)l(rN+j)rN+rl+jtrl)1. (4.2)

    When m in (4.1) and m=1 in (4.2), V(j)N,n,r=V(j)N,n,r,=V(j)N,n,r,1 are the original hypergeometric Cauchy numbers of grade r, defined in (2.1) with (2.2). Hence, both incomplete numbers are reduced to the hypergeometric Cauchy numbers too.

    Notice that V(j)N,n,r,m=V(j)N,n,r,m=0 unless n0(modr).

    The restricted and associated hypergeometric Cauchy numbers satisfy the following recurrence relations.

    Proposition 2. For j=0,1, we have

    V(j)N,rn,r,m=n1k=max{nm,0}(1)nk1(rn)!(rN+j)(rN+rnrk+j)(rk)!V(j)N,rk,r,m(n1)

    with V(j)N,0,r,m=1, and

    V(j)N,rn,r,m=nmk=0(1)nk1(rn)!(rN+j)(rN+rnrk+j)(rk)!V(j)N,rk,r,m(nm)

    with V(j)N,0,r,m=1 and V(j)N,r,r,m==V(j)N,r(m1),r,m=0.

    Proof. First, we shall prove the relation for the restricted hypergeometric Cauchy numbers. By the definition (4.1), we get

    1=(1+ml=1(1)l(rN+j)trlrN+rl+j)(n=0V(j)N,rn,r,mtrn(rn)!)=n=0V(j)N,rn,r,mtrn(rn)!+n=1n1k=max{nm,0}(1)nk(rN+j)V(j)N,rk,r,m(rN+rnrk+j)(rk)!trn.

    Comparing the coefficient on both sides, we obtain the first identity.

    Next, we prove the relation for the associated hypergeometric Cauchy numbers. By the definition (4.2), we get

    1=(1+l=m(1)l(rN+j)!trlrN+rl+j)(n=0V(j)N,rn,r,mtrn(rn)!)=n=0V(j)N,rn,r,mtrn(rn)!+n=mnmk=0(1)nk(rN+j)V(j)N,rk,r,m(rN+rnrk+j)(rk)!trn.

    Comparing the coefficient on both sides, we obtain the desired result.

    The restricted and associated hypergeometric Cauchy numbers have the following expressions in terms of determinants. From the expression of Theorem 3, all the elements change to 0 in more diagonal directed bands.

    Theorem 4. For integers n and m with nm1, we have

    V(j)N,rn,r,m=(rn)!|JT+mk=1rN+jr(N+k)+jJk1|

    and

    V(j)N,rn,r,m=(rn)!|JT+nk=mrN+jr(N+k)+jJk1|.

    Proof. First, we shall prove the first expression for the restricted hypergeometric Cauchy numbers. For simplicity, put ˜VN,rn,m=V(j)N,rn,r,m/(rn)! and prove that for nm1

    ˜VN,rn,m=|JT+mk=1rN+jr(N+k)+jJk1|. (4.3)

    When n=m, we have ˜VN,rm,m=˜VN,rm, and the result reduces to Theorem 3. Assume that (4.3) is valid up to n1. If n2m, then the determinant on the right-hand side of (4.3) is equal to

    ˜VN,rnr,m(rN+j)rN+j+r˜VN,rn2r,m(rN+j)rN+j+2r++(1)m1|rN+jrN+rm+j100rN+jrN+r+j1rN+jrN+rm+j1rN+jrN+rm+jrN+jrN+r+j|=˜VN,rnr,m(rN+j)rN+r+j˜VN,rn2r,m(rN+j)rN+2r+j++(1)m1˜VN,rnrm,m(rN+j)rN+rm+j=˜VN,rn,m.

    If m<n2m, then the determinant on the right-hand side of (4.3) is equal to

    ˜V(j)N,rnr,m(rN+j)rN+r+j˜V(j)N,rn2r,m(rN+j)rN+2r+j++(1)mn1|rN+jrN+rnrm+j10rN+jrN+rm+jrN+jrN+2rmrn+j010rN+jrN+rm+jrN+jrN+r+j|=˜VN,rnr,m(rN+j)rN+r+j˜VN,rn2r,m(rN+j)rN+2r+j++(1)nm1˜VN,rm,m(rN+j)rN+rnrm+j=˜VN,rnr,m(rN+j)rN+r+j˜VN,rn2r,m(rN+j)rN+2r+j++(1)m1˜VN,rnrm,m(rN+j)rN+rm+j=˜VN,rn,m.

    Next, we prove the second expression for the associated hypergeometric Cauchy numbers. For simplicity, put ˜VN,rn,m=VN,rn,r,m/(rn)! and we prove that

    ˜VN,rn,m=|JT+nk=mrN+jr(N+k)+jJk1|. (4.4)

    If mn2m, the determinant on the right-hand side of (4.4) is equal to

    (1)nm|00rN+jrN+rm+jrN+jrN+rn+j1000100m1|=(1)nm(1)m+1rN+jrN+rn+j|1000001|=(1)n+1rN+jrN+rn+j.

    Since only the term for k=0 does not vanish in the second relation of Proposition 2, we have

    ˜VN,rn,m=(1)n+1rN+jrN+rn+j.

    If n2m, the determinant on the right-hand side of (4.4) is equal to

    (1)m1|rN+jrN+rm+jrN+jrN+rn+j1000rN+jrN+rm+jrN+jr(N+nm)+jrN+jr(N+m)+jn2m+10100m1|=(1)m1˜V(j)N,rnrm,m(rN+j)rN+rm+j+(1)m|rN+jrN+rm+r+jrN+jrN+rn+j1000rN+jrN+rm+jrN+jr(N+nm1)+jrN+jr(N+m)+jn2m0100m1|==(1)m1˜V(j)N,rnrm,m(rN+j)rN+rm+j+(1)m˜V(j)N,r(nm1),m(rN+j)rN+r(m+1)+j++(1)nm+1˜V(j)N,rm,m(rN+j)rN+r(nm)+j+(1)nm+1(1)mrN+jrN+rn+j=nmk=m(1)nk˜VN,rk,m(rN+j)r(N+nk)+j=˜VN,rn,m.

    Here, we used the second relation of Proposition 2 again.

    There exist explicit expressions for both incomplete Cauchy numbers.

    Theorem 5. For n,m1,

    V(j)N,rn,r,m=(rn)!nk=1(1)nki1++ik=n1i1,,ikm(rN+j)k(rN+ri1+j)(rN+rik+j).

    For n,m1,

    V(j)N,rn,m=(rn)!nk=1(1)nki1++ik=ni1,,ikm(rN+j)k(rN+ri1+j)(rN+rik+j).

    Proof. First, we shall prove the first expression for the restricted hypergeometric Cauchy numbers. When nm, the proof is similar to that of Proposition 1. Note that in the proof of Proposition 1,

    1nl=iknk+1n.

    Let nm+1. By the first relation of Proposition 2

    V(j)N,rn,r,m(rn)!=n1l=nm(1)nl1(rN+j)V(j)N,rl,r,m(rN+rnrl+j)(rl)!=n1l=nm(1)nl1(rN+j)rN+rnrl+jlk=1(1)lki1++ik=l1i1,,ikm(rN+j)k(rN+ri1+j)(rN+rik+j)=n1l=1(1)nk1(rN+j)rN+rnrl+jlk=1i1++ik=l1i1,,ikm(rN+j)k(rN+ri1+j)(rN+rik+j)+nm1l=1(1)nk(rN+j)rN+rnrl+jlk=1(1)ki1++ik=l1i1,,ikm(rN+j)k(rN+ri1+j)(rN+rik+j)=n1k=1(1)nk1n1l=krN+jrN+rnrl+ji1++ik=l1i1,,ikm(rN+j)k(rN+ri1+j)(rN+rik+j)+nm1k=1(1)nknm1l=krN+jrN+rnrl+ji1++ik=l1i1,,ikm(rN+j)k(rN+ri1+j)(rN+rik+j)=nk=2(1)nkn1l=k1rN+jrN+rnrl+ji1++ik1=l1i1,,ik1m(rN+j)k1(rN+ri1+j)(rN+rik1+j)+nmk=2(1)nk1nm1l=k1rN+jrN+rnrl+ji1++ik1=l1i1,,ik1m(rN+j)k1(rN+ri1+j)(rN+rik1+j)=nk=nm+1(1)nkn1l=k1rN+jrN+rnrl+ji1++ik1=l1i1,,ik1m(rN+j)k1(rN+ri1+j)(rN+rik1+j)+nmk=2(1)nkn1l=nmrN+jrN+rnrl+ji1++ik1=l1i1,,ik1m(rN+j)k1(rN+ri1+j)(rN+rik1+j).

    By putting ik=nl, in the first term by n1lk1nm, in the second term by n1lnm, we have

    1nl=ikm.

    Therefore,

    V(j)N,rn,r,m(rn)!=nk=nm+1(1)nki1++ik=n1i1,,ikm(rN+j)k(rN+ri1+j)(rN+rik+j)+nmk=2(1)nki1++ik=n1i1,,ikm(rN+j)k(rN+ri1+j)(rN+rik+j)=nk=1(1)nki1++ik=n1i1,,ikm(rN+j)k(rN+ri1+j)(rN+rik+j).

    Note that the expression vanishes for k=1 as n>m.

    Next, we prove the second expression for the associated hypergeometric Cauchy numbers. Since the set

    {(i1,,ik)|i1++ik=n,i1,,ikm}

    is empty for n=1,,m1, we have V(j)N,r,r,m==V(j)N,rmr,r,m=0. For n=m, by the second expression of Theorem 4

    V(j)N,rm,r,m=(rm)!|0101rN+jrN+rm+j00|=(rm)!(1)m1rN+jrN+rm+j=(1)m1(rN+j)rN+rm+j,

    which matches the result for n=m. Assume that the result is valid up to n1(m). Then by the second relation of Proposition 2

    VN,rn,r,m(rn)!=nml=0(1)nl1(rN+j)(rN+rnrl+j)(rl)!V(j)N,rl,r,m=(1)n1(rN+j)rN+rn+j+nml=1(1)nl1(rN+j)rN+rnrl+jlk=1(1)lki1++ik=li1,,ikm(rN+j)k(rN+ri1+j)(rN+rik+j)=(1)n1(rN+j)rN+rn+j+nmk=1(1)nk1nml=krN+jrN+rnrl+ji1++ik=li1,,ikm(rN+j)k(rN+ri1+j)(rN+rik+j)=(1)n1(rN+j)rN+rn+j+nm+1k=2(1)nknml=k1rN+jrN+rnrl+ji1++ik1=li1,,ik1m(rN+j)k1(rN+ri1+j)(rN+rik1+j)=(1)n1(rN+j)rN+rn+j+nm+1k=2(1)nki1++ik=ni1,,ikm(rN+j)k(rN+ri1+j)(rN+rik+j)(ik=nl)=nm+1k=1(1)nki1++ik=ni1,,ikm(rN+j)k(rN+ri1+j)(rN+rik+j)=nk=1(1)nki1++ik=ni1,,ikm(rN+j)k(rN+ri1+j)(rN+rik+j).

    Note that ik=nlm as lnm. As 1mn1, we have m(nm+2)>n, so the set

    {(i1,,ik)|i1++ik=n,i1,,ikm}

    is empty for nm+2kn.

    We shall use Trudi's formula to obtain different explicit expressions and inversion relations for the numbers V(j)N,n. Denote the multinomial coefficients by (t1++tnt1,,tn)=(t1++tn)!t1!tn!.

    Lemma 1. For a positive integer n, we have

    |a1a00a2a10an1a1a0anan1a2a1|=t1+2t2++ntn=n(t1++tnt1,,tn)(a0)nt1tnat11at22atnn.

    This relation is known as Trudi's formula [21,Vol.3, p.214], [23] and the case a0=1 of this formula is known as Brioschi's formula [4], [21,Vol.3, pp.208–209].

    In addition, there exists the following inversion formula (see, e.g., [17]), which is based upon the relation

    nk=0(1)nkαkD(nk)=0(n1)

    or Cameron's operator in (2.3).

    Lemma 2. For the sequence {αn}n0 defined by α0=1 and

    αn=|D(1)1D(2)1D(n)D(2)D(1)|, we have D(n)=|α11α21αnα2α1|.

    From Trudi's formula, it is possible to give the combinatorial expression

    αn=t1+2t2++ntn=n(t1++tnt1,,tn)(1)nt1tnD(1)t1D(2)t2D(n)tn.

    By applying these lemmas to Theorem 4, we obtain explicit expressions for the incomplete hypergeometric Cauchy numbers of higher grade defined in (4.1) and (4.2).

    Theorem 6. For nm1, we have

    V(j)N,rn,r,m=(rn)!t1+2t2++mtm=n(t1++tmt1,,tm)(1)nt1tm(rN+jrN+j+r)t1(rN+jrN+rm+j)tm

    and

    (j)N,rn,r,m=(rn)!mtm+(m+1)tm+1++ntn=n(tm+tm+1++tntm,tm+1,,tn)×(1)ntmtm+1tn(rN+jrN+rm+j)tm(rN+jrN+rm+j+r)tm+1(rN+jrN+rn+j)tn.

    As a special case of Theorem 6, we can obtain the expressions for the original hypergeometric Cauchy numbers.

    Corollary 1. For n1, we have

    V(j)N,rn,r=(rn)!t1+2t2++ntn=n(t1++tnt1,,tn)(1)nt1tn(rN+jrN+j+r)t1(rN+jrN+rn+j)tn.

    By applying the inversion relation in Lemma 2 to Theorem 3, we have the following.

    Theorem 7. Let j=0,1. For n1, we have

    rN+jrN+rn+j=|JT+nk=1V(j)N,kr,r(kr)!Jk1|.

    In this sense, we have the inversion relation of Corollary 1 too.

    Corollary 2. For n1, we have

    rN+jrN+rn+j=t1+2t2++ntn=n(t1++tnt1,,tn)(1)nt1tn(V(j)N,r,rr!)t1(V(j)N,rn,r(rn)!)tn.

    In this paper, we proposed one type of generalizations of the classical Cauchy numbers and hypergeometric Cauchy numbers. Many other generalizations are known, but the focus of this paper is on the determinant, which originated in Glaisher and others. Similar determinants have been dealt with by Brioshi, Trudi and others, but have long been forgotten. A similar generalization attempt, made by the first author of this paper with Barman in 2019, has proposed generalized numbers including the classical Bernoulli numbers, hypergeometric Bernoulli numbers, Euler numbers, hypergeometric Euler numbers, and so on. However, classical Cauchy numbers and hypergeometric Cauchy numbers cannot be included in the generalization by Barman et al., and this is achieved in this paper. The background and motivation for generalization is Cameron's operator, which is related to graph theory. There, only integers were targeted, but in this paper, we extended this to rational numbers and applied it.

    The authors thank the anonymous referees for useful comments which have helped us to improve the manuscript.



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