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Research article

Localized Orthogonal Decomposition for two-scale Helmholtz-typeproblems

  • In this paper, we present a Localized Orthogonal Decomposition (LOD) in Petrov-Galerkin formulation for a two-scale Helmholtz-type problem. The two-scale problem is, for instance, motivated from the homogenization of the Helmholtz equation with high contrast, studied together with a corresponding multiscale method in a previous paper of the authors. There, an unavoidable resolution condition on the mesh sizes in terms of the wave number has been observed, which is known as "pollution e ect" in the finite element literature. Following ideas of Gallistl and Peterseim, we use standard finite element functions for the trial space, whereas the test functions are enriched by solutions of subscsale problems (solved on a finer grid) on local patches. Provided that the oversampling parameter m, which indicates the size of the patches, is coupled logarithmically to the wave number, we obtain a quasi-optimal method under a reasonable resolution of a few degrees of freedom per wave length, thus overcoming the pollution effect. In the two-scale setting, the main challenges for the LOD lie in the coupling of the function spaces and in the periodic boundary conditions.

    Citation: Mario Ohlberger, Barbara Verfürth. Localized Orthogonal Decomposition for two-scale Helmholtz-typeproblems[J]. AIMS Mathematics, 2017, 2(3): 458-478. doi: 10.3934/Math.2017.2.458

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  • In this paper, we present a Localized Orthogonal Decomposition (LOD) in Petrov-Galerkin formulation for a two-scale Helmholtz-type problem. The two-scale problem is, for instance, motivated from the homogenization of the Helmholtz equation with high contrast, studied together with a corresponding multiscale method in a previous paper of the authors. There, an unavoidable resolution condition on the mesh sizes in terms of the wave number has been observed, which is known as "pollution e ect" in the finite element literature. Following ideas of Gallistl and Peterseim, we use standard finite element functions for the trial space, whereas the test functions are enriched by solutions of subscsale problems (solved on a finer grid) on local patches. Provided that the oversampling parameter m, which indicates the size of the patches, is coupled logarithmically to the wave number, we obtain a quasi-optimal method under a reasonable resolution of a few degrees of freedom per wave length, thus overcoming the pollution effect. In the two-scale setting, the main challenges for the LOD lie in the coupling of the function spaces and in the periodic boundary conditions.


    In combinatorics, the Catalan numbers are the numbers of Dyck words of length 2n or the numbers of different ways n+1 factors completely parenthesized or the numbers of non-isomorphic ordered trees with n+1 vertices or the numbers of monotonic lattice paths along the edges of a grid with n×n square cells, which do not pass above the diagonal or the numbers of noncrossing partitions of the set {1,...,n} and arise in many other counting problems with real-world applications [3,5,7,24,28]. The Catalan-Daehee numbers are defined by assigning 14t1 instead of t in the definition of Daehee numbers which play important role in connecting relationship between special numbers [10,16]. Moreover, the generating function of Catalan numbers can be represented by the fermionic p-adic integral on Zp of (14t)x2 and the generating function of Catalan-Daehee numbers can be represented by the p-adic Volkenborn integral on Zp of the same function (14t)x2 [16,17]. Various identities of Catalan-Daehee polynomials have been studied in [5,16,17,29].

    Many scholars in the field of mathematics have worked on degenerate versions of special polynomials and numbers which include the degenerate Stirling numbers of the first and second kinds, the degenerate Bernstein polynomials, the degenerate Bell numbers and polynomials, the degenerate gamma function, the degenerate gamma random variables, and so on [1,2,10,11,12,13,14,15,19,20,30,31]. We can find the motivation to study degenerate polynomials and numbers in the following real-world examples. Suppose the probability of a baseball player getting a hit in a match is p. We wonder if the probability that the player will succeed in the 11th trial after failing 9 times in 10 trials is still p. We can see cases where the probability is less than p because of the psychological burden that the player must succeed in the 11th trial [31].

    In the 1970s, Rota and his collaborators [22,23,24] began to construct a rigorous foundation for the classical umbral calculus, which consisted of a symbolic technique for the manipulation of numerical and polynomial sequences. The umbral calculus has received much attention from researchers because of its numerous applications in many fields of mathematics, physics, chemistry, and engineering [4,6,9,11,13,15,16,20,21,22,23,24,25,26,28]. For instance, the connection between Sheffer polynomials and Riordan array and the isomorphism between the Sheffer groups and the Riordan Groups are proved [25,26]. Recently, Kim-Kim [11] introduced the λ-Sheffer sequences and the degenerate Sheffer sequences by substituting λ-linear functionals and λ-differential operators, respectively, instead of linear functionals and differential operators.

    With these points in mind, in this paper, we first define the degenerate Catalan-Daehee numbers and polynomials and degenerate Catalan-Daehee polynomials of order r(1) as one of the generalizations of the degenerate Catalan-Daehee polynomials. It is difficult to study identities related to degenerate Catalan-Daehee polynomials and special polynomials using the p-adic integral on Zp or other properties. Thus, we explore various interesting identities related to the degenerate Catalan-Daehee polynomials of order r and special polynomials and numbers by using degenerate Sheffer sequences. At the same time we derive the inversion formulas of these identities. Some of them include the degenerate and other special polynomials and numbers such as the degenerate falling factorials, the falling factorials, the degenerate Bernoulli polynomials and numbers of order r, the degenerate Euler polynomials and numbers of order r, the degenerate Daehee polynomials of order r, the degenerate Bell polynomials, etc.

    Now, we give some definitions and properties needed in this paper.

    For any nonzero λR, the degenerate exponential function is defined by

    exλ(t)=(1+λt)xλ,eλ(t)=(1+λt)1λ,  (|xλ|1)(see[1017]). (1.1)

    By Taylor expansion, we get

    exλ(t)=n=0(x)n,λtnn!,(see [1017]), (1.2)

    where (x)0,λ=1, (x)n,λ=x(xλ)(x2λ)(x(n1)λ), (n1).

    The degenerate Bernoulli polynomials and degenerate Euler polynomials of order r, respectively, are given by the generating function

    (teλ(t)1)rexλ(t)=n=0B(r)n,λ(x)tnn!, (see [1,1113]), (1.3)

    and

    (2eλ(t)+1)rexλ(t)=n=0E(r)n,λ(x)tnn!,(see[1,11,13]). (1.4)

    We note that B(r)n,λ=B(r)n,λ(0) and E(r)n,λ=E(r)n,λ(0) (n0), which are called the degenerate Bernoulli and degenerate Euler numbers of order r, respectively.

    The degenerate Bernoulli polynomials of the second kind of order r are defined by the generating function

    (tlogλ(1+t))r(1+t)x=n=0b(r)n,λ(x)tnn!,(see [8,11]). (1.5)

    When x=0, b(r)n,λ=b(r)n,λ(0), which are called the degenerate Bernoulli numbers of the second kind of order r.

    The degenerate Daehee polynomials of order r are defined by the generating function

    (logλ(1+t)t)r(1+t)x=n=0D(r)n,λ(x)tnn!,(see [6,11]), (1.6)

    where logλ(1+t)=1λ((1+t)λ1) and logλ(eλ(t))=eλ(logλ(t))=t.

    When x=0, D(r)n,λ=D(r)n,λ(0), which are called the degenerate Daehee numbers of order r.

    The Bell polynomials are defined by the generating function

    ex(et1)=n=0Beln(x)tnn!,(see  [3,15,19,20]).

    Kim-Kim introduced the degenerate Bell polynomials given by the generating function

    exλ(eλ(t)1)=l=0Bell,λ(x)tll!,(see  [13]). (1.7)

    When x=1, Bel(r)n,λ=Bel(r)n,λ(1) are called the degenerate Bell numbers.

    For n0, it is well known that the Stirling numbers of the first and second kind, respectively are given by

    (x)n=nl=0S1(n,l)xl  and  1k!(log(1+t))k=n=kS1(n,k)tnn!,(see  [1,14]),

    and

    xn=nl=0S2(n,l)(x)l  and  1k!(et1)k=n=kS2(n,k)tnn!,(see  [1,14]),

    where (x)0=1,(x)n=x(x1)(xn+1), (n1).

    Moreover, the degenerate Stirling numbers of the first and second kind, respectively are given by

    (x)n=nl=0S1,λ(n,l)(x)l,λ  and 1k!(logλ(1+t))k=n=kS1,λ(n,k)tnn!,(k0),(see  [12,14]), (1.8)

    and

    (x)n,λ=nl=0S2,λ(n,l)(x)l  and 1k!(eλ(t)1)k=n=kS2,λ(n,k)tnn!,(k0),(see  [12,14]). (1.9)

    For k0, as an extension of the notion of the degenerate Stirling numbers of the second kind, Kim et al. introduced Jindalrae-Stirling numbers of the second kind by

    1k!(eλ(eλ(t)1)1)k=n=kS(2)j,λ(n,k)tnn!,(see  [18]). (1.10)

    From (1.9) and (1.10), we note that

    S(2)j,λ(n,k)=nm=kS2,λ(n,m)S2,λ(m,k). (1.11)

    Let C be the complex number field and let F be the set of all power series in the variable t over C with

    F={f(t)=k=0aktkk! | akC}.

    Let P=C[x] and P be the vector space all linear functional on P:

    Pn={ P(x)C[x] | degP(x)n},  (n0).

    Then Pn is an (n+1)-dimensional vector space over C.

    Recently, Kim-Kim [11] considered λ-linear functional and λ-differential operator as follows:

    For f(t)=k=0aktkk!F and a fixed nonzero real number λ, each λ gives rise to the linear functional f(t)|λ on P, called λ-linear functional given by f(t), which is defined by

    f(t)|(x)n,λλ=an,forall n0,(see  [11]). (1.12)

    In particular tk|(x)n,λλ=n!δn,k, for all n,k0, where δn,k is the Kronecker's symbol.

    For λ=0, we observe that the linear functional f(t)|0 agrees with the one in f(t)|xn=ak, (k0).

    For each λR and each nonnegative integer k, they also defined the differential operator on P by

    (tk)λ(x)n,λ={(n)k(x)nk,λ,    if   kn,0if   kn,(see[11]). (1.13)

    and for any power series f(t)=k=0aktkk!F, (f(t))λ(x)n,λ=nk=0(nk)ak(x)nk,λ,   (n0).

    The order o(f(t)) of a power series f(t)(0) is the smallest integer k for which the coefficient of tk does not vanish. The series f(t) is called invertible if o(f(t))=0 and such series has a multiplicative inverse 1/f(t) of f(t). f(t) is called a delta series if o(f(t))=1 and it has a compositional inverse ¯f(t) of f(t) with ¯f(f(t))=f(¯f(t))=t.

    Let f(t) and g(t) be a delta series and an invertible series, respectively. Then there exists a unique sequence sn,λ(x) such that the orthogonality condition holds

    g(t)(f(t))k|sn,λ(x)λ=n!δn,k,(n,k0),(see  [11]). (1.14)

    The sequence sn,λ(x) is called the λ-Sheffer sequence for (g(t),f(t)), which is denoted by sn,λ(x)(g(t),f(t))λ.

    The sequence sn,λ(x)  (g(t),f(t))λ if and only if

    1g(¯f(t))exλ(¯f(t)) = k=0sk,λ(x)k!tk,(n,k0),(see  [11]). (1.15)

    Assume that for each λR of the set of nonzero real numbers, sn,λ(x) is λ-Sheffer for (gλ(t),fλ(t)). Assume also that limλ0fλ(t)=f(t) and limλ0gλ(t)=g(t), for some delta series f(t) and an invertible series g(t). Then limλ0¯fλ(t)=¯f(t), where is the compositional inverse of f(t) with ¯f(f(t))=f(¯f(t))=t. Let limλ0sk,λ(x)=sk(x). In this case, Kim-Kim called that the family {sn,λ(x)}λR{0} of λ-Sheffer sequences sn,λ is the degenerate (Sheffer) sequences for the Sheffer polynomial sn(x).

    Let sn,λ(x)(g(t),f(t))λ and rn,λ(x)(h(t),g(t))λ, (n0). Then

    sn,λ(x)=nk=0zn,krk,λ(x),(n0),  where   zn,k=1k!h(¯f(t))g(¯f(t))(l(¯f(t)))k|(x)n,λλ,(n,k0),(see  [11]). (1.16)

    In this section, we define the degenerate Catalan-Daehee polynomials of order r, and derive several identities between the degenerate Catalan-Daehee polynomials of order r and some other polynomials arising from degenerate Sheffer sequences.

    As is known, the Catalan numbers Cn are given by the generating function

    114t2t=21+14t=n=0Cntn,(see  [5,16,17]).

    The Catalan numbers C(r)n of order r, as a generalization of Catalan numbers, are given by the generating function

    (114t2t)r=(21+14t)r=n=0C(r)ntn,(see  [16,17]).

    Kim-Kim introduced the Catalan-Daehee polynomials which are given by the generating function

    12log(14t)14t1(14t)x2=n=0Cn(x)tn=n=0n!Cn(x)tnn!,(see  [16,17]). (2.1)

    When x=0, Cn:=Cn(0), which are called Catalan-Daehee numbers.

    From (1.6) and (2.1), we note that

    n=0Cn(x)tn=12log(14t)14t1(14t)x2=n=0n!Dn,12(x2)(4)ntnn!.

    We introduce the degenerate Catalan-Daehee polynomials Cn,λ(x) which are given by the generating function

    (12logλ(14t)eλ(12logλ(14t))1)exλ(12logλ(14t))=n=0n!Cn,λ(x)tnn!. (2.2)

    When x=0, Cn,λ:=Cn,λ(0), which are called degenerate Catalan Daehee numbers.

    When λ0, we note that Cn,λ(x)=Cn(x).

    As a generalization of the degenerate Catalan-Daehee polynomials, we also introduce degenerate Catalan-Daehee polynomials C(r)n,λ(x) of order r are given by the generating function

    (12logλ(14t)eλ(12logλ(14t))1)rexλ(12logλ(14t))=n=0n!C(r)n,λ(x)tnn!. (2.3)

    When x=0, C(r)n,λ:=C(r)n,λ(0), which are called degenerate Catalan Daehee numbers of order r.

    It easy to see that the compositional inverse of f(t)=14(1eλ(2t)) such that f(¯f(t))=¯f(f(t))=t is

    ¯f(t)=12logλ(14t). (2.4)

    From(1.15), (2.2), (2.3) and (2.4) we have

    n!Cn,λ(x)(eλ(t)1t,14(1eλ(2t)))λ, (2.5)

    and

    n!C(r)n,λ(x)((eλ(t)1t)r,14(1eλ(2t))λ. (2.6)

    Theorem 1. For nN{0}, we have

    C(r)n,λ(x)=1n!nk=0((nm)(1)m22mkS1,λ(m,k)(nm)!C(r)nm,λ)(x)k,λ.

    Proof. From (1.2), (1.15) and (2.6), we consider the following two Sheffer sequence as follows:

    n!C(r)n,λ(x)((eλ(t)1t)r,14(1eλ(2t)))λand (x)n,λ(1,t)λ. (2.7)

    From (1.16) and (2.7), we have

    n!C(r)n,λ(x)=nk=0zn,k(1)k,λ. (2.8)

    From (1.8) and (2.3), we obtain

    zn,k=1k!(12logλ(14t)eλ(12logλ(14t))1)r(12logλ(14t))k|(x)n,λλ=12k(12logλ(14t)eλ(12logλ(14t))1)r|(logλ(1+(4t))kk!)λ(x)n,λλ=12knm=k(nm)(4)mS1,λ(m,k)(12logλ(14t)eλ(12logλ(14t))1)r|(x)nm,λλ=nm=k(nm)(1)m22mkS1,λ(m,k)(nm)!C(r)nm,λ. (2.9)

    Therefore, from (2.8) and (2.9), we have the desired result.

    The next theorem gives the inversion formula of Theorem 1.

    Theorem 2. For nN{0} and rN, we have

    (1)n,λ=nk=0k!r!4k(1)k(nl=k2l(nl)(nl+r)rS2,λ(l,k)S2,λ(nl+r,r))C(r)k,λ(x).

    Proof. From (2.7), we consider the following two degenerate Sheffer sequences

    (x)n,λ(1,t)λand n!C(r)n,λ(x)((eλ(t)1t)r,14(1eλ(2t)))λ. (2.10)

    From (1.16) and (2.10), we have

    (1)n,λ=nk=0~zn,kC(r)k,λ(x). (2.11)

    First, by (1.9), we observe that

    (eλ(t)1t)r=r!tr(eλ(t)1)rr!=r!m=0(m+r)rS2,λ(m+r,r)tmn!. (2.12)

    Then, from (1.2), (1.9), (1.16) and (2.12) we have

    ~zn,k=1k!(eλ(t)1t)r(14(1eλ(2t)))k|(x)n,λλ=14k(1)knl=k2lS2,λ(l,k)(nl)(eλ(t)1t)r|(x)nl,λλ=r!4k(1)knl=k2lS2,λ(l,k)(nl)(nl+r)rS2,λ(nl+r,r). (2.13)

    Therefore, from (2.11) and (2.13), we have what we want.

    Theorem 3. For nN{0}, we have

    C(r)n,λ(x)=1n!nk=0(nl=knm=ln!m!(1)m22mlS1,λ(m,l)S2,λ(l,k)C(r)nm,λ)(x)k.

    Proof. We note that

    (x)n(1,eλ(t)1)λ (2.14)

    because of exλ(log(1+t))=(1+t)x=n=0(x)ntnn!.

    From (2.6) and (2.14), we consider the following two degenerate Sheffer sequences.

    n!C(r)n,λ(x)((eλ(t)1t)r,14(1eλ(2t)))λand (x)n(1,eλ(t)1)λ. (2.15)

    From (1.8), (1.9), (1.16) and (2.15), we observe that

    n!C(r)n,λ(x)=nk=0zn,k(x)k, (2.16)

    and

    (eλ(12logλ(14t))1)kk!=l=kS2,λ(l,k)(12logλ(14t))ll!=m=ll=k(1)m22mlS1,λ(m,l)S2,λ(l,k)tmm!. (2.17)

    From (1.16) and (2.17), we obtain

    zn,k=1k!(12logλ(14t)eλ(12logλ(14t))1)r(eλ(12logλ(14t))1)k|(x)n,λλ=nm=lnl=k(1)m22mlS1,λ(m,l)S2,λ(l,k)(nm)(12logλ(14t)eλ(12logλ(14t))1)r|(x)nm,λλ=nm=lnl=k(1)m22mlS1,λ(m,l)S2,λ(l,k)(nm)(nm)!C(r)nm,λ=nl=knm=ln!m!(1)m22mlS1,λ(m,l)S2,λ(l,k)C(r)nm,λ. (2.18)

    From (2.16) and (2.18), we get the desired result.

    The next theorem is the inversion formula of Theorem 3.

    Theorem 4. For nN{0} and rN, we have

    (x)n=nk=0k!(nl=knm=l(nm)(1)k2l2kS1,λ(m,l)S2,λ(l,k)b(r)nm,λ)C(r)k,λ(x),

    where b(r)n,λ are the Bernoulli numbers of the second kind of order r.

    Proof. From (2.15), we consider the following two degenerate Sheffer sequences.

    (x)n(1,t)λand n!C(r)n,λ(x)((eλ(t)1t)r,14(1eλ(2t)))λ. (2.19)

    From (1.16) and (2.19), we have

    (x)n=nk=0~zn,kk!C(r)k,λ(x). (2.20)

    From (1.5), (1.8), (1.9) and (1.16), we get

    ~zn,k=1k!(tlogλ(1+t))r14k(1eλ(2logλ(1+t)))k|(x)n,λλ=(1)k4knl=kS2,λ(l,k)2l(tlogλ(1+t))r|((logλ(1+t))ll!)λ(x)n,λλ=(1)k4knl=kS2,λ(l,k)2lnm=lS1,λ(m,l)(nm)(tlogλ(1+t))r|(x)nm,λλ=nl=knm=l(nm)(1)k2l2kS1,λ(m,l)S2,λ(l,k)b(r)nm,λ. (2.21)

    Combining (2.20) and (2.21), we prove the theorem.

    Theorem 5. For nN{0}, we have

    (1) when r1=r2, C(r1)n,λ(x)=1n!nk=0(1)m22nkS1,λ(n,k)B(r2)k,λ(x),

    (2) when r1r2, C(r1)n,λ(x)=nk=0nl=k(nl)(1)l22lk(nl)!S1,λ(l,k)C(r1r2)nk,λB(r2)k,λ(x),

    where B(r)k,λ(x) are the Bernoulli polynomials of order r.

    Proof. From (1.3), (1.15) and (2.6), we consider two degenerate Sheffer sequences as follows:

    n!C(r1)n,λ(x)((eλ(t)1t)r1,14(1eλ(2t)))λand B(r2)n,λ(x)((eλ(t)1t)r2,t)λ. (2.22)

    From (1.16) and (2.22), we have

    n!C(r1)n,λ(x)=nk=0zn,kB(r2)k,λ(x), (2.23)

    From (1.8) and (1.16), we have

    when r1=r2,

    zn,k=1k!12k(logλ(14t))k|(x)n,λλ=12kS1,λ(n,k)(4)n=(1)m22nkS1,λ(n,k), (2.24)

    when r1>r2,

    zn,k=1k!(eλ(12logλ(14t))112logλ(14t))r2r112k(logλ(14t))k|(x)n,λλ=12knl=kS1,λ(l,k)(4)l(nl)(12logλ(14t)eλ(12logλ(14t))1)r1r2|(x)nl,λλ=nl=k(1)l22lk(nl)S1,λ(l,k)(nl)!C(r1r2)nk,λ, (2.25)

    and when r1<r2,

    zn,k=1k!(eλ(12logλ(14t))112logλ(14t))r2r112k(logλ(14t))k|(x)n,λλ=nl=k(1)l22lk(nl)S1,λ(l,k)(12logλ(14t)eλ(12logλ(14t))1)r1r2|(x)nl,λλ=nl=k(1)l22lk(nl)S1,λ(l,k)(nl)!C(r1r2)nk,λ. (2.26)

    Therefore, from (2.23), (2.24), (2.25) and (2.26), we have the desired result.

    The following theorem gives the inversion formula of Theorem 5.

    Theorem 6. For nN{0}, we have

    (1) when r1=r2, B(r2)n,λ(x)=nk=0k!((1)k2n2kS2,λ(n,k))C(r1)k,λ(x),

    (2) when r1r2, B(r2)n,λ(x)=nk=0(1)kk!(nl=k(nl)2l2kS2,λ(l,k)B(r2r1)nl,λ)C(r1)k,λ(x).

    Proof. From (2.22), we consider the two degenerate Sheffer sequences as follows:

    B(r2)n,λ(x)((eλ(t)1t)r2,t)λand n!C(r1)n,λ(x)((eλ(t)1t)r1,14(1eλ(2t)))λ. (2.27)

    From (1.16) and (2.27), we have

    B(r2)n,λ(x)=nk=0~zn,kk!C(r1)k,λ(x). (2.28)

    And from (1.3), (1.5) and (1.16), we get

    when r1=r2,

    ~zn,k=1k!(1)k4k(eλ(2t)1)k|(x)n,λλ=(1)k22kl=kS2,λ(l,k)2ltll!|(x)n,λλ=(1)k2n2kS2,λ(n,k), (2.29)

    when r1>r2,

    ~zn,k=1k!(eλ(t)1t)r1r214k(1eλ(2t))k|(x)n,λλ=(1)k22knl=kS2,λ(l,k)2l(nl)(teλ(t)1)r2r1|(x)nl,λλ=(1)knl=k2l2k(nl)S2,λ(l,k)B(r2r1)nl,λ, (2.30)

    and when r1<r2,

    ~zn,k=1k!(teλ(t)1)r2r114k(1eλ(2t))k|(x)n,λλ=(1)knl=k2l2k(nl)S2,λ(l,k)B(r2r1)nl,λ. (2.31)

    From (2.28), (2.29), (2.30) and (2.31), we arrive at the desired result.

    Theorem 7. For nN{0} and sN, we have

    C(r1)n,λ(x)=1n!nk=0(12k+1nl=kS1,λ(l,k)(4)l(nl)nlm=0m!C(r1)m,λ(nlm)×nlmj=ir2i=0(1)nlm2r2ij2(nlm)S2,λ(j,i)S1,λ(nlm,j))E(r2)k,λ(x),

    where E(r)n,λ(x) are the degenerate Euler polynomials of order r.

    Proof. From (1.4), (1.15) and (2.6), we consider the following two degenerate Sheffer sequences

    n!C(r1)n,λ(x)((eλ(t)1t)r1,14(1eλ(2t)))λand E(r2)n,λ(x)((eλ(t)+12)r2,t)λ. (2.32)

    From (1.16) and (2.32), we give

    n!C(r1)n,λ(x)=nk=0zn,kE(r2)k,λ(x). (2.33)

    Observe that

    (eλ(12log(14t))+1)r=(eλ(12log(14t))1+2)r=ri=0(ri)(eλ(12log(14t))1)i2ri=ri=0(ri)2rii!j=iS2,λ(j,i)(12)j(log(14t))jj!=ri=0(ri)2riji!j=iS2,λ(j,i)d=jS1,λ(d,j)(4)dtdd!=d=idj=iri=0(1)d2rij+2dS2,λ(j,i)S1,λ(d,j)tdd!. (2.34)

    From (1.2), (1.8), (1.16), (2.3) and (2.34), we obtain

    zn,k=1k!(eλ(12logλ(14t))+12)r2(12(logλ(14t))eλ(12logλ(14t))1)r1×12k(logλ(14t))k|(x)n,λλ=12k+1nl=kS1,λ(l,k)(4)l(nl)nlm=0m!C(r1)m,λ(nlm)×(eλ(12logλ(14t))+12)r2|(x)nlm,λλ=12k+1nl=kS1,λ(l,k)(4)l(nl)nlm=0m!C(r1)m,λ(nlm)×nlmj=ir2i=0(1)nlm2r2ij+2(nlm)S2,λ(j,i)S1,λ(nlm,j). (2.35)

    Therefore, from (2.33) and (2.35), we arrive at the desired result.

    Theorem 8. For nN{0} and sN, we have

    E(r2)n,λ(x)=nk=0k!(22k(1)knl=knlm=0(nl)(nlm)2l(1)nlm+1,λnlm+1×S2,λ(l,k)E(r2)m,λ)C(r1)k,λ(x),

    where E(r)n,λ(x) are the degenerate Euler polynomials of order r.

    Proof. From (1.4), (1.15) and (2.5), we consider two degenerate Sheffer sequences as follows:

    E(r2)n,λ(x)((eλ(t)+12)r2,t)λand n!C(r1)n,λ(x)((eλ(t)1t)r1,14(1eλ(2t)))λ. (2.36)

    From (1.16) and (2.36), we have

    E(r2)n,λ(x)=nk=0~zn,kk!C(r1)k,λ(x), (2.37)

    and from (1.2), (1.4), (1.9) and (1.16), we get

    ~zn,k=(2eλ(t)+1)r2(eλ(t)1t)r114k(1eλ(2t))kk!|(x)n,λλ.=22k(1)knl=kS2,λ(l,k)2l(nl)(eλ(t)1t)r1|(2eλ(t)+1)r2λ(x)nl,λλ=22k(1)knl=k(nl)2lS2,λ(l,k)nlm=0(nlm)E(r2)m,λ(eλ(t)1t)r1|(x)nlm,λλ=22k(1)knl=k(nl)2lS2,λ(l,k)nlm=0(nlm)E(r2)m,λ(1)nlm+1,λnlm+1. (2.38)

    From (2.37) and (2.38), we deduce the desired result.

    Theorem 9. For nN{0} and sN, we have

    C(r1)nm,λ(x)=1n!nk=0(nm=lml=k(nm)(1)m22ml(nm)!S1,λ(m,l)S2,λ(l,k)C(r1+r2)nm,λ)b(r2)k,λ(x),

    where b(r)n,λ(x) are degenerate Bernoulli polynomials of the second kind of order r.

    Proof. From (1.5), (1.15) and (2.6), we consider the following two degenerate Sheffer sequences

    n!C(r1)n,λ(x)((eλ(t)1t)r1,14(1eλ(2t)))λ and  b(r2)n,λ(x)((teλ(t)1)r2,eλ(t)1)λ. (2.39)

    From (1.16) and (2.39), we have

    n!C(r1)n,λ(x)=nk=0zn,kb(r2)k,λ(x). (2.40)

    From (1.8), (1.16) and (2.3), we derive

    zn,k=(12logλ(14t)eλ(12logλ(14t))1)r1(12logλ(14t)eλ(12logλ(14t))1)r2|(1k!(eλ(12logλ(14t))1)k)λ(x)n,λλ=nm=lml=k(1)m22mlS2,λ(l,k)S1,λ(m,l)(nm)(12logλ(14t)eλ(12logλ(14t))1)r1+r2|(x)nm,λλ=nm=lml=k(1)m22ml(nm)S1,λ(m,l)S2,λ(l,k)(nm)!C(r1+r2)nm,λ. (2.41)

    Therefore, from (2.40) and (2.41), we have the desired result.

    The next theorem is the inversion formula of Theorem 9.

    Theorem 10. For nN{0} and sN, we have

    b(r2)n,λ(x)=nk=0k!(nm=kml=k2l2k(nm)S1,λ(m,l)S2,λ(l,k)b(r1+r2)n,λ)C(r1)k,λ(x),

    where b(r)n,λ(x) are degenerate Bernoulli polynomials of the second kind of order r.

    Proof. From (1.8) and (1.9), we observe that

    (eλ(2logλ(1+t))1)kk!=l=kS2,λ(l,k)2l(logλ(1+t))ll!=l=kS2,λ(l,k)2lm=lS1,λ(m,l)tmm!=m=kml=k2lS1,λ(m,l)S2,λ(l,k)tmm!. (2.42)

    From (2.39), we consider the following two degenerate Sheffer sequences

    b(r2)n,λ(x)((teλ(t)1)r2,eλ(t)1)λand n!C(r1)n,λ(x)((eλ(t)1t)r1,14(1eλ(2t)))λ. (2.43)

    We have

    b(r2)n,λ(x)=nk=0~zn,kk!C(r1)k,λ(x). (2.44)

    From (1.5), (1.8), (1.9), (1.16) and (2.42),

    ~zn,k=1k!(tlogλ(1+t))r1+r214k(1eλ(2logλ(1+t)))k|(x)n,λλ.=22knm=kml=k2lS1,λ(m,l)S2,λ(l,k)(nm)(tlogλ(1+t))r1+r2|(x)nm,λλ=nm=kml=k2l2k(nm)S1,λ(m,l)S2,λ(l,k)b(r1+r2)n,λ. (2.45)

    Thus, from (2.44) and (2.45), we get the desired result.

    Theorem 11. For nN{0} and sN, we have

    C(r1)n,λ(x)=1n!nk=0nl=k2lS1,λ(n,l)S2,λ(l,k)D(r2)n,λ(x),

    where D(r)n,λ(x) are degenerate Daehee polynomials of order r.

    Proof. From (1.6), (1.15) and (2.6), we consider the following two degenerate Sheffer sequences

    n!C(r1)n,λ(x)((eλ(t)1t)r1,14(1eλ(2t)))λand D(r2)n,λ(x)((eλ(t)1t)r2,eλ(t)1)λ. (2.46)

    From (1.16) and (2.44), we have

    n!C(r1)n,λ(x)=nk=0zn,kD(r2)k,λ(x), (2.47)

    and from (1.8), (1.9) and (1.16), we get

    zn,k=1k!(eλ(12logλ(14t))1)k|(x)n,λλ=nm=kml=k2lS1,λ(m,l)S2,λ(l,k)1m!tm|(x)n,λλ=nl=k2lS1,λ(n,l)S2,λ(l,k). (2.48)

    From (2.47) and (2.48), we have the desired result.

    The next theorem represents the inversion formula of Theorem 11.

    Theorem 12. For nN{0} and sN, we have

    D(r2)n,λ(x)=nk=0k!(nl=k2l2k(1)kk!S1,λ(n,l)S2,λ(l,k))C(r1)k,λ(x),

    where D(r)n,λ(x) are degenerate Daehee polynomials of order r.

    Proof. By (2.46), we consider the following two degenerate Sheffer sequences

    D(r2)n,λ(x)((eλ(t)1t)r2,eλ(t)1)λand n!C(r1)n,λ(x)((eλ(t)1t)r1,14(1eλ(2t)))λ, (2.49)

    and from (1.16) and (2.49), we get

    D(r2)n,λ(x)=nk=0~zn,kk!C(r1)k,λ(x). (2.50)

    From (1.8), (1.9), (1.16) and (2.42), we have

    ~zn,k=1k!14k(1eλ(2logλ(1+t)))k|(x)n,λλ=(1)k4knm=kml=k2lS1,λ(m,l)S2,λ(l,k)1m!tm|(x)n,λλ=(1)knl=k2l2kS1,λ(n,l)S2,λ(l,k). (2.51)

    From (2.50) and (2.51), we obtain the desired result.

    Theorem 13. For nN{0} and sN, we have

    C(r)n,λ(x)=1n!nk=0(nm=kml=k(1)m22ml(nm)(nm)!S1,λ(m,l)S1,λ(l,k)C(r)nm,λ)Belk,λ(x),

    where Beln,λ(x) are degenerate Bell polynomials.

    Proof. From (1.8) and (2.3), we observe that

    logλ(1+12logλ(14t))kk!=l=kS1,λ(l,k)(12)l(logλ(14t))ll!=m=kml=k(1)m22mlS1,λ(l,k)S1,λ(m,l)tmm!. (2.52)

    From (1.7) and (1.15), we consider the following two degenerate Sheffer sequences as follows:

    n!C(r)n,λ(x)((eλ(t)1t)r,14(1eλ(2t)))λand Belk,λ(x)(1,logλ(1+t))λ. (2.53)

    From (1.16) and (2.53), we have

    n!C(r)n,λ(x)=nk=0zn,kBelk,λ(x). (2.54)

    From (1.16), (2.3) and (2.52), we get

    zn,k=1k!(12logλ(14t)eλ(12logλ(14t))1)r(logλ(1+12(logλ(14t)))k|(x)n,λλ=nm=kml=k(1)m22mlS1,λ(l,k)S1,λ(m,l)(nm)(12logλ(14t)eλ(12logλ(14t))1)r|(x)nm,λλ=nm=kml=k(1)m22ml(nm)(nm)!S1,λ(m,l)S1,λ(l,k)C(r)nm,λ. (2.55)

    Thus, from (2.54) and (2.55), we have the desired result.

    The next theorem is the inversion formula of Theorem 13.

    Theorem 14. For nN{0} and sN, we have

    Beln,λ(x)=nk=0k!r!(nm=kml=knmd=0d+rj=r(nm)(nmd)(1)k2l2k(d+r)r×S2,λ(m,l)S2,λ(l,k)S2,λ(d+r,j)S2,λ(j,r)B(r)nmd,λ)C(r)k,λ(x),

    where Beln,λ(x) are degenerate Bell polynomials.

    Proof. From (2.53), we consider two degenerate Sheffer sequences as follows:

    Belk,λ(x)(1,logλ(1+t))λand  n!C(r)n,λ(x)((eλ(t)1t)r,14(1eλ(2t)))λ. (2.56)

    From (1.16) and (2.56), we have

    Beln,λ(x)=nk=0~zn,kk!C(r)k,λ(x). (2.57)

    First, from (1.2), (1.9) and (1.10), we have two identities as follows:

    (eλ(2(eλ(t)1))1)kk!=(1)kl=kS2,λ(l,k)2l(eλ(t)1)ll!=m=kml=kS2,λ(l,k)2lS2,λ(m,k)tmm!, (2.58)

    and

    (eλ(eλ(t)1)t)r=r!tr1r!(eλ(eλ(t)1)1)r=r!1trd=rSJ,λ(d,r)tdd!=r!d=0SJ,λ(d+r,r)td(d+r)!=r!l=0(d+r)rSJ,λ(d+r,r)tdd!, (2.59)

    where SJ,λ(n,r) are the Jindalrae-Stirling numbers of the second kind [18].

    From (1.11), (1.16), (2.58) and (2.59), we observe that

    ~zn,k=1k!(eλ(eλ(t)1)1eλ(t)1)r14k(1eλ(2(eλ(t)1)))k|(x)n,λλ=nm=kml=k(1)k2l2k(nm)S2,λ(m,l)S2,λ(l,k)×(teλ(t)1)r|((eλ(eλ(t)1)1t)r)λ(x)nm,λλ=nm=kml=k(1)k2l2k(nm)S2,λ(m,l)S2,λ(l,k)r!nmd=0(d+r)r×d+rj=rS2,λ(d+r,j)S2,λ(j,r)(nmd)B(r)nmd,λ. (2.60)

    From (2.57) and (2.60), we get the desired result.

    In this paper, we introduced the degenerate Catalan-Daehee numbers and polynomials of order r (r1). It was shown that the degenerate Catalan-Daehee polynomials of order r were expressed based on the degenerate falling factorials, the falling factorials, the degenerate Bernoulli polynomials of order r, the Euler polynomials (of order r), the degenerate Bernoulli polynomials of the second kind of order r, the degenerate Deahee polynomials of order r, and the degenerate Bell polynomials. We also obtained inverse formula for each of them.

    It is difficult to single out where and why these formulas play an important role, but we do not doubt that they will be helpful to researchers in need of these identities. Further research would be related with the degenerate versions of some special combinatorial numbers and polynomials and then contribution in mathematics and physics applications.

    The author would like to thank the referees for the detailed and valuable comments that helped improve the original manuscript in its present form.

    This work was supported by research fund of Kwangwoon University in 2021.

    The authors declare no conflict of interest.

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    沈阳化工大学材料科学与工程学院 沈阳 110142

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