R(p,q)-deformed combinatorics: full characterization and illustration
Mahouton Norbert Hounkonnou, Fridolin Melong

TL;DR
This paper develops a comprehensive R(p,q)-deformed combinatorics framework, extending classical combinatorial concepts and applying it to deformed quantum algebra, enriching the mathematical tools for discrete probability and quantum algebra applications.
Contribution
It provides a full characterization of R(p,q)-deformed combinatorics, including new formulas and properties, and illustrates its application to generalized q-Quesne deformed quantum algebra.
Findings
Derived R(p,q)-deformed factorials and binomial coefficients
Established R(p,q)-Stirling numbers and Bell numbers
Applied formalism to q-Quesne deformed quantum algebra
Abstract
This paper addresses a theory of R(p,q)-deformed combinatorics in discrete probability. It mainly focuses on R(p,q)-deformed factorials, binomial coefficients, Vandermonde's formula, Cauchy's formula, binomial and negative binomial formulae, factorial and binomial moments, and Stirling numbers. Moreover, the R(p,q)-Stirling numbers of the second kind and the R(p,q)-Bell numbers for graphs are also derived. Related relevant properties are investigated and discussed. Finally, as a concrete illustration, the developed formalism is displayed for the well known generalized q-Quesne deformed quantum algebra to construct the corresponding deformed combinatorics, as a particular case.
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Taxonomy
TopicsAdvanced Combinatorial Mathematics · Advanced Mathematical Identities · Random Matrices and Applications
ICMPA-MPA/2019
deformed combinatorics: full characterization and illustration
Mahouton Norbert Hounkonnou*∗* and Fridolin Melong
International Chair in Mathematical Physics and Applications *(ICMPA-UNESCO Chair), * University of Abomey-Calavi, *072 B.P. 50 Cotonou, Republic of Benin
Abstract
This paper addresses a theory of -deformed combinatorics in discrete probability. It mainly focuses on -deformed factorials, binomial coefficients, Vandermonde’s formula, Cauchy’s formula, binomial and negative binomial formulae, factorial and binomial moments, and Stirling numbers. Moreover, the Stirling numbers of the second kind and the Bell numbers for graphs are also derived. Related relevant properties are investigated and discussed. Finally, as a concrete illustration, the developed formalism is displayed for the well known generalized Quesne deformed quantum algebra to construct the corresponding deformed combinatorics, as a particular case.
Keywords. Combinatorics, combinatorics, deformed quantum algebras, calculus.
Contents
1 Introduction
Combinatorial theory is a major branch of mathematics, which has applications in many fields such as computer science (languages, graphs, intelligent computing), natural and social sciences, biomedicine, molecular biology, operational research, engineering, and business[24, 25, 28]. Combinatorial theory and discrete mathematical methods play an important role, and occupy a central position in the theory of discrete probability. The most prominent of these methods are the combinatorial enumerative methods and the basic methods of finite difference computation. A considerable number of stochastic experiments or phenomena in discrete probability theory can be described by the stochastic models of distributions [10].
Chung and Kang developed a new combinatorics called combinatorics and investigated the significance of permutations and combinations[5]. The idea of analogs can be traced back to Euler in the 1700’s who studied series, especially specializations of theta functions. Meanwhile, in [7], Ch. A. Charalambides examined basic combinatorics and hypergeometric series. The power, factorial, binomial coefficient of a real number and two Vandermonde’s (factorial convolution) formulae were derived. The analogs of the Cauchy’s formulas were also investigated in [1].
Furthermore, the Stirling numbers of the first and second kinds, which are the coefficients of the expansions of factorials into powers, and of powers into factorials, respectively, were presented. Moreover, the Stirling numbers of the second kind and their generalizations were studied by several authors, (see for instance [21, 22, 23] and references theiren). The Stirling numbers of the second kind and Bell numbers for graphs were also analyzed in [2]. Corcino and Barientos [12] established many properties for analogs of Stirling numbers. The vertical and horizontal recursion relations and the generating function were also computed. Besides, two parameters Stirling numbers, which are generating functions for the joint distribution of pair statistics, were described in [29]. In addition, a theory of analogs of binomial coefficients was elaborated. Some properties and identities like the triangular, vertical, and horizontal recursion relations, the generating function, the orthogonality and inverse relations were derived in [11].
Later in 2010, deformed quantum algebra was introduced by Hounkonnou and Bukweli [15] as a generalization of known deformed quantum algebras. The same authors also performed differentiation and integration, and deducted all relevant particular cases of and deformations [14]. This opens a novel route for developing the theory of analogs of special numbers and combinatorics.
This paper provides a general formalism, which enables an easier construction of a combinatorial theory from deformed quantum algebras existing in the literature by assigning concrete suitable expressions to the function and related specific meromorphic functions of the theory. Especially, analogs of factorials, binomial coefficients, Vandermonde’s formula, Cauchy’s formula, binomial formula and negative binomial formula, factorial moments, binomial moments, Stirling numbers and Bell numbers on a graph are investigated and discussed. Furthermore, the case of the generalized Quesne deformed combinatorics is derived to illustrate the presented formalism. From this new generalization, developing deformed combinatorial theories associated with other particular cases of deformed quantum algebras, known and spread in the literature, appears as a matter of triviality.
The paper is organized as follows. Section is devoted to basic notations, definitions and results related to quantum algebras and calculus, and to basic combinatorics. In Section the fundamentals of deformed combinatorics and the derivation of relevant properties are exposed. The generalized Quesne combinatorics is derived as a case study. Some concluding remarks are addressed in Section
2 Preliminaries
In this section, we briefly recall the main definitions, notations and known results used in the sequel. For more details, the reader can refer to [7, 8, 9, 10, 11], [14, 15] and [18, 19].
The coherent states introduced by Quesne[26] can be associated with the deformed algebra satisfying the relations
[TABLE]
where and the Quesne number is defined by:
[TABLE]
The Quesne algebra is a particular case of the Kalnins-Miller-Mukherjee algebra [20] with Furthermore, Hounkonnou and Ngompe Nkouankam [16] generalized the Quesne algebra with the generators satisfying the relations
[TABLE]
where Their generalized Quesne number is given as follows:
[TABLE]
Let now be a meromorphic function defined on by
[TABLE]
converging in the complex disc where are complex numbers, and is the radius of convergence of the series (2.3). Let us consider the set of holomorphic functions defined on .
In the sequel, when no possible confusion arises, and will designate two real numbers satisfying
Definition 2.1
[14]** Let and be two linear operators on . Then, for , we have
[TABLE]
[TABLE]
The derivative and the number are defined, respectively, by [6]:
[TABLE]
[TABLE]
while the derivative is given by [14]:
[TABLE]
Definition 2.2
[15]** The number and the factorials are defined, respectively, as follows:
[TABLE]
[TABLE]
and the binomial coefficient is given by:
[TABLE]
More details on deformed quantum algebras, differentiation and integration can be found in [14, 15]. To be complete, let us briefly recall some notions about known combinatorics pertaining to our development in the sequel.
Definition 2.3
The shifted factorial is given by
[TABLE]
The binomial coefficients are given by [11]:
[TABLE]
For real numbers and the analog of the Cauchy’s formula is given by [7]
[TABLE]
or, equivalently,
[TABLE]
Furthermore, the following orthogonality relations hold [8]:
[TABLE]
and
[TABLE]
where is the Kronecker delta, and are positive integers. The order of a factorial number is written as a polynomial of the number as follows [13]:
[TABLE]
or,
[TABLE]
where the coefficients and are called Stirling numbers of the first and second kinds, respectively.
Let and be positive integers. Then, the following relations also hold:
[TABLE]
and
[TABLE]
where is an integer and Finally, recall that the deformed probability distribution of a discrete random variable is given by Ch. A. Charalambides [7] as
[TABLE]
where the series is absolutely convergent, and {\bf E}\bigg{(}\bigg{[}\begin{array}[]{c}X\\ m\end{array}\bigg{]}_{q}\bigg{)} stands for the expectation value of \bigg{[}\begin{array}[]{c}X\\ m\end{array}\bigg{]}_{q}.
3 deformed combinatorics
Our aim is to present fundamentals of a generalization of the combinatorial theory from the deformed quantum algebra introduced in [15] as a generalization of known deformed quantum algebras. We consider with depending on the parameters and
3.1 deformed factorials and binomial coefficients
Definition 3.1
Let be a real number. Then, the deformed factorial of of order is defined by :
[TABLE]
where and
The relation (3.1) will also be called the order factorial of the deformed number. From the above definition, we derive the following basic property for the deformed factorial:
[TABLE]
Lemma 3.2
Let and be real numbers such that Then, the deformed factorial of of negative order is given as follows:
[TABLE]
[TABLE]
Proof: It uses the relation (3.2).
For the equation (3.3) yields
[TABLE]
Definition 3.3
The deformed binomial coefficient is defined by:
[TABLE]
We assume there exist with depending on the parameters and which link the deformed numbers and as follows:
[TABLE]
Then, the following relations hold:
[TABLE]
and
[TABLE]
and being real numbers.
Proposition 3.4
Let be a natural number and a positive integer. Then,
[TABLE]
[TABLE]
and
[TABLE]
Proof: Using the relation (3.5), we get
[TABLE]
Furthermore,
[TABLE]
Finally, using the relation (3.4), we obtain (3.10).
Remark 3.5
The formula (3.10) may be expressed as
[TABLE]
For we recover the Jagannathan-Srinivassa binomial coefficient as:
[TABLE]
The generalized Quesne binomial coefficient can be obtained by putting as:
[TABLE]
Theorem 3.6
Let and be real numbers such that and be a positive integer. Then, the deformed binomial coefficients satisfy the following recursion relation:
[TABLE]
or, equivalently,
[TABLE]
with the initial conditon \bigg{[}\begin{array}[]{c}x\\ 0\end{array}\bigg{]}_{\mathcal{R}(p,q)}:=1.
Proof: Since using the relations (3.6), the factorial of x satisfies the recursion relation:
[TABLE]
with condition From the expression (3.4), the relation (3.14) is deduced. Furthermore, the expression (3.1) satisfies
[TABLE]
Dividing the members of the above equation by , we obtain (3.15), and the proof is achieved.
Corollary 3.7
Let and be real numbers. Then, the following relation holds:
[TABLE]
Proof: It is straightforward by computation.
Taking we recuperate a simpler relation under the form
[TABLE]
where
Remark 3.8
- (1)
Note that the results obtained by Hounkonnou and Bukweli in **[14]** can be retrieved by taking 2. (2)
The generalized Quesne formulae are given as follows, with real numbers and such that and
- (i)
[TABLE]
- (ii)
[TABLE]
- (iii)
[TABLE]
- (iv)
[TABLE]
[TABLE]
and
[TABLE]
3.2 deformed Vandermonde’s and Cauchy’s formulae
The deformed Vandermonde’s formula, also called deformed factorial convolution, is contained in the theorem below, where, for the expression simplification, we set and and are real numbers with
Theorem 3.9
The deformed Vandermonde’s formula is given by:
[TABLE]
or, equivalently,
[TABLE]
where is a positive integer.
Proof: For we consider the following expression:
[TABLE]
For we have Using the recursion relation (3.14) and
[TABLE]
we obtain
[TABLE]
Therefore, for the sum satisfies the first-order recursion relation
[TABLE]
with Recursively, it follows that Therefore, we get (3.16). Finally, interchanging by and replacing by the expression (3.16) is rewritten in the form (3.17).
Remark 3.10
Note that the deformed Vandermonde’s formula can be retrieved by taking
[TABLE]
or, in an alternative form,
[TABLE]
where
From the Vandermonde’s formula (3.16), we can deduce the following remarkable deformed identities.
Lemma 3.11
Let and be real numbers such that Then, the following relations hold.
[TABLE]
[TABLE]
and
[TABLE]
Proof: Replacing by in (3.16), we obtain
[TABLE]
Multiplying both sides of this relation by and using we get
[TABLE]
and according to (3.3), we deduce the required formula
[TABLE]
Putting now in (3.22), and using, respectively,
[TABLE]
and
[TABLE]
we get (3.23). Similarly, by substituting by we obtain (3.24).
Remark 3.12
Taking we retrieve the identities as particular cases:
[TABLE]
[TABLE]
and
[TABLE]
Considering two real numbers and leads to the following results:
Theorem 3.13
The deformed Cauchy’s formula is given by:
[TABLE]
or, equivalently,
[TABLE]
Proof: From (3.4) and the deformed Vandermonde’s formula, we get the result.
We obtain the deformed Cauchy’s formulae (2.6) and (2.7) by taking
Theorem 3.14
The negative deformed Vandermonde’s formula is given by:
[TABLE]
or
[TABLE]
where is a positive integer.
Proof: For we consider the following expression:
[TABLE]
For we have
[TABLE]
Using the relation (3.14) and
[TABLE]
takes the following form
[TABLE]
Therefore, for the sum satisfies the first-order recursion relation
[TABLE]
with Recursively, it comes that Following the steps used to prove (3.30), we obtain (3.31), and the proof is achieved.
We recover the negative Vandermonde’s formulae by taking as follows:
[TABLE]
and, alternatively,
[TABLE]
where
Lemma 3.15
[TABLE]
and
[TABLE]
Proof: For a positive integer, the deformed factorial of of order is written as:
[TABLE]
and
[TABLE]
In the same vein, the deformed binomial coefficient of is given by:
[TABLE]
Moreover,
[TABLE]
and
[TABLE]
The relation (3.30) may be written as follows:
[TABLE]
where
[TABLE]
Taking into acount the fact that
[TABLE]
the relation (3.36) is reduced to (3.34). Similarly, we obtain (3.35).
Setting and provides the analogs of the formulae (3.34) and (3.35) as:
[TABLE]
and
[TABLE]
Remark 3.16
By taking and a positive integer, we deduct, as particular cases, the generalized Quesne deformed Vandermonde and Cauchy’s formulae given, respectively, by:
[TABLE]
and
[TABLE]
while their negative counterparts are provided by
[TABLE]
and
[TABLE]
respectively.
3.3 deformed binomial and negative binomial formulae
In this section, we examine in detail the deformed binomial. Here also, and are real numbers with is a positive integer. Then,
Theorem 3.17
[TABLE]
Proof: The result follows from induction on
Taking we recover the binomial formula (2.4), while gives the binomial formula (2.5).
Theorem 3.18
[TABLE]
where
Proof: We have
[TABLE]
Setting and from [7], we obtain
[TABLE]
The proof is achieved.
The negative binomial coefficient can be obtained, by setting in the form:
[TABLE]
A novel negative binomial formula can be deduced as follows:
Lemma 3.19
For
[TABLE]
or, in an equivalent way,
[TABLE]
Proof: Since
[TABLE]
and using [7], we obtain
[TABLE]
From (3.13) and
[TABLE]
we get (3.49). Replacing by by and by leads to (3.50), and the proof is achieved.
Remark 3.20
The negative binomial formula can be obtained by taking
[TABLE]
which can also be translated into the form:
[TABLE]
Theorem 3.21
The following orthogonality relations hold:
[TABLE]
and
[TABLE]
where is the Kronecker delta, and are positive integers.
Proof: Since
[TABLE]
then, the relation (3.54) may be expressed as:
[TABLE]
From the expression
[TABLE]
we get (3.55). Therefore, the result holds.
The deformed orthogonality relations (2.8) and (2.9) can be recovered by putting
Corollary 3.22
The inversion of the binomial formula is provided by:
[TABLE]
In particular,
[TABLE]
Proof: From the relation (3.10) and replacing by by by , by and by in (3.45), we get
[TABLE]
Multiplying the members of the above expression by (-1)^{\kappa}\,\epsilon_{1}^{{\kappa\choose 2}}\,\epsilon_{2}^{{\kappa\choose 2}}\bigg{[}\begin{array}[]{c}n\\ \kappa\end{array}\bigg{]}_{\mathcal{R}(p,q)}, it comes
[TABLE]
Summing the expression (3.63) for using (3.55) and
[TABLE]
we obtain (3.58). Replacing by in (3.58) and using
[TABLE]
yield (3.59).
Remark 3.23
Putting and we obtain the inversion of the binomial formula [7]:
[TABLE]
In particular,
[TABLE]
The inversion of the deformed binomial formulae (3.58) and (3.59) leads to the following results:
Lemma 3.24
[TABLE]
and
[TABLE]
Proof: Replacing by in equation (3.58), and using the expression
[TABLE]
we obtain (3.70). Also replacing by and by in (3.59), we get
[TABLE]
Using the relations (3.8), (3.10) and after computation, the result holds.
It is worth noticing the following relevant identities from binomial and negative binomial formulae, as exposed and proved below:
- •
Lemma 3.25
Let and be positive integers. Then, the following relations hold:
[TABLE]
[TABLE]
and
[TABLE]
Proof: From the binomial formula and
[TABLE]
we get
[TABLE]
where
[TABLE]
Using
[TABLE]
and
[TABLE]
we obtain
[TABLE]
giving (3.71). Setting and in (3.71), and using
[TABLE]
the relation (3.72) holds. Since
[TABLE]
and putting in (3.71), we get (3.73), what achieves the proof.
Remark 3.26
Note the following:
- (1)
*The relation (3.71) is a particular case of the *deformed Cauchy formula (3.28), with and 2. (2)
The particular case of deformation is achieved from the above formulae by taking as follows:
[TABLE]
[TABLE]
and
[TABLE]
- •
Lemma 3.27
Let and be positive integers. Then,
[TABLE]
Proof: From the relation
[TABLE]
where and from the negative binomial formula, we get
[TABLE]
where
[TABLE]
Setting and after computation, it follows
[TABLE]
yielding the result.
Remark 3.28
- (a)
This formula constitutes a particular version of the Cauchy formula (3.28), corresponding to negative integers and 2. (b)
*Putting we recover the deformed analog of this Lemma as: *
[TABLE]
- •
Lemma 3.29
For and positive integers, such that we have:
[TABLE]
Proof: Multiplying both the members of the negative binomial formula
[TABLE]
by and putting we obtain
[TABLE]
Similarly, we get
[TABLE]
and
[TABLE]
Using
[TABLE]
and the above relations, we arrive at the result.
Note that the deformed version can be recovered by taking
[TABLE]
Remark 3.30
It is worth noticing that
- (1)
The generalized Quesne deformed binomial and negative binomial formulae can straightforwardly be retrieved from the general formalism as particular cases as follows:
- (i)
[TABLE]
- (ii)
[TABLE]
- (iii)
[TABLE]
and
[TABLE]
- (iv)
[TABLE]
In particular,
[TABLE] 2. (2)
The associated deformed binomial formulae (3.80) and (3.81) can also be rewritten as follows:
[TABLE]
and
[TABLE]
Further, the following identities are retrieved from the above Lemmas:
[TABLE]
[TABLE]
[TABLE]
[TABLE]
[TABLE]
[TABLE]
or
[TABLE]
3.4 deformed Stirling numbers
Definition 3.31
Let and be real numbers such that Then, the noncentral deformed factorial of of order and of noncentrality parameter is defined by:
[TABLE]
where is a positive integer.
Taking in (3.84), we obtain the deformed factorial of of order Following the relation
[TABLE]
the equation (3.84) takes the form
[TABLE]
Further, we get a polynomial of the deformed number of degree as follows:
[TABLE]
or
[TABLE]
Equivalently,
[TABLE]
The coefficients and are the noncentral deformed Stirling numbers of the first and second kind, respectively.
Remark 3.32
- (1)
For these deformed numbers are reduced to and which are nothing but the deformed Stirling numbers of the first and second kinds, respectively. 2. (2)
Taking we recover the deformed Stirling numbers of first and second kinds (2.10) and (2.11) .
Lemma 3.33
[TABLE]
and
[TABLE]
where is a positive interger, and stands for the deformed absolute noncentral deformed Stirling number of the first kind.
Proof: Since
[TABLE]
then,
[TABLE]
is also a polynomial of the deformed number of degree and after computation, for we get
[TABLE]
Furthermore,
[TABLE]
[TABLE]
Replacing now by and by and by in (3.85), the result follows.
Theorem 3.34
The deformed Stirling numbers of the first and second kinds verify the orthogonality relations:
[TABLE]
and
[TABLE]
Proof: From the relations (3.85) and (3.86), we write
[TABLE]
giving, after computation, (3.88). Similarly, we obtain (3.89).
The next statement is also valid.
Theorem 3.35
*For and the noncentral deformed Stirling numbers of the first and second kinds, and obey, respectively, the recursion relations *
[TABLE]
with initial conditions and and
[TABLE]
with initial conditions and
Proof:
- (1)
Let us consider the relation
[TABLE]
or
[TABLE]
From the relation (3.85) and the expansion of both members of the recursion relation (3.92) into powers of we get
[TABLE]
which gives (3.90). We use the relation (3.85) to get the initial conditions. 2. (2)
Similarly, consider
[TABLE]
and use the relation (3.86) to obtain
[TABLE]
Thus, we get the relation (3.91). The initial conditions follow from (3.87).
Theorem 3.36
For fixed , the generating function of noncentral deformed Stirling numbers of the second kind is given as follows:
[TABLE]
or, equivalently, in product form
[TABLE]
for
Proof: We assume that the series (3.94) converges. Multiplying the expression (3.91) by and summing the resulting relation for and we obtain
[TABLE]
which implies
[TABLE]
By induction and consideration that
[TABLE]
Remark 3.37
The generating function of the noncentral Stirling numbers of the second kind can be obtained as:
[TABLE]
where and
Lemma 3.38
For and the reciprocal noncentral deformed factorial is expanded into the reciprocal deformed powers as follows:
[TABLE]
while the reciprocal deformed powers is expanded into the reciprocal noncentral deformed factorial as below expressed:
[TABLE]
where
Proof: Setting in (3.94) and (3.95), we obtain
[TABLE]
and
[TABLE]
Thus,
[TABLE]
and after rearranging, we find (3.96). Moreover, let us fix in (3.96). Replacing by and by we get
[TABLE]
Multiplying the result by and summing for we find
[TABLE]
By the orthogonality relation (3.89), we have
[TABLE]
and the result follows.
Theorem 3.39
The noncentral deformed Stirling numbers of the first and second kinds are given, respectively, by
[TABLE]
and
[TABLE]
*where and *
Proof: From the relation (3.10) and replacing in the binomial formula (3.45), we get
[TABLE]
Multipliying (3.99) by and using
[TABLE]
we obtain
[TABLE]
Comparing the above relation with (3.85), we obtain (3.97). Furthermore,
[TABLE]
Using (3.59), we get
[TABLE]
and from (3.87), we obtain (3.98).
Remark 3.40
Taking we obtain the noncentral Stirling numbers of the first and second kinds as:
[TABLE]
and
[TABLE]
*where and *
Corollary 3.41
Let and be positive integers. Then, the following relations hold:
[TABLE]
and
[TABLE]
where is an integer and
Proof: Replacing by by by and in (3.97), we get
[TABLE]
Multiplying this result by
[TABLE]
and summing for all we obtain
[TABLE]
Similarly, in (3.98), we replace by by multiply the resulting expression by
[TABLE]
and sum it for all to get the result.
Note that we obtain the deformed formulae (2.12) and (2.13) by taking
Lemma 3.42
Let be a natural number. Then, the following relations hold:
[TABLE]
and
[TABLE]
where \zeta_{u,p,q}=\displaystyle\sum_{j=1}^{u}\epsilon^{(j-1)(x+1)}_{1}\Bigg{(}\mathcal{R}(p^{j},q^{j})\Bigg{)}^{-1} and
Proof: From the triangular recursion relation of the deformed Stirling numbers of the first kind (3.90), we set and obtain the first-order recursion relation
[TABLE]
with and By iteration, we get (3.105). Setting also leads to the recursion relation
[TABLE]
where
[TABLE]
which is solved to give the required expression.
Taking we recover
[TABLE]
and
[TABLE]
where
Remark 3.43
The particular case of the generalized Quesne quantum algebra is here worthy of attention as matter of illustration. Indeed, the signless (or absolute) noncentral generalized Quesne Stirling number of the first kind is given by
[TABLE]
or
[TABLE]
where is a positive interger. The related deformed Stirling numbers of the first and second kinds verify the orthogonality relations
[TABLE]
and
[TABLE]
*They obey, respectively, the following recursion relations: *
[TABLE]
with the initial conditions and and
[TABLE]
with the initial conditions s^{Q}_{p,q}(n,0,j)=\big{(}{q\over p}[j]^{Q}_{p,q}\big{)}^{n}, and For fix , they are generated by the function given by
[TABLE]
developed in the product form as:
[TABLE]
for Their reciprocal factorial is expanded into reciprocal generalized Quesne powers \big{(}[t]^{Q}_{p,q}\big{)}^{-n-1} as follows:
[TABLE]
while their reciprocal powers \big{(}[t]_{p,q}^{Q}\big{)}^{-\kappa-1} are spanned in the reciprocal noncentral generalized Quesne factorial as:
[TABLE]
*where Moreover, *
[TABLE]
and
[TABLE]
where and In particular,
[TABLE]
For positive integers and
[TABLE]
and
[TABLE]
where is an integer and Furthermore, given a natural number ,
[TABLE]
and
[TABLE]
where
3.5 deformed Bell numbers
Let us consider a simple finite graph with vertices, and independent blocks. is a set of vertices of The vertices are partitioned into independent blocks by We define the deformed weight as follows:
[TABLE]
where is the cardinality of the set The deformed Stirling number of the second kind for the graph is expressed by
[TABLE]
where S_{\mathcal{R}(p,q)}\big{(}\bf G,0\big{)}:=0, and denotes the independent partitions of Analogously, the deformed Bell number for the graph is defined by
[TABLE]
Theorem 3.44
Let be the dual path graph of Then, the deformed Stirling numbers of the second kind and the deformed Bell numbers for the graph are given, respectively, by
[TABLE]
and
[TABLE]
where
Proof: Let us consider the expression
[TABLE]
For the relation (3.109) is true. We assume that (3.109) is true for all and prove it for Consider
[TABLE]
where
[TABLE]
and
[TABLE]
Using Eq.(3.14) and after computation, we obtain
[TABLE]
Thus, the proof is achieved.
3.6 Application
We consider the dual path graph It has independent partitions into blocks given as follows:
[TABLE]
[TABLE]
The deformed weight is given by
[TABLE]
Hence,
[TABLE]
Similarly, we get W_{\mathcal{R}(p,q)}(\Gamma_{2})=\Big{(}{\epsilon_{2}\over\epsilon_{1}}\Big{)}^{7}, W_{\mathcal{R}(p,q)}(\Gamma_{3})=\Big{(}{\epsilon_{2}\over\epsilon_{1}}\Big{)}^{8} and W_{\mathcal{R}(p,q)}(\Gamma_{4})=\Big{(}{\epsilon_{2}\over\epsilon_{1}}\Big{)}^{9}. Finally,
[TABLE]
Remark 3.45
- (1)
Note that the Stirling number of the second kind and Bell number of the graph can easily be derived by taking as follows:
[TABLE]
and
[TABLE]
where 2. (2)
The generalized Quesne Stirling number of the second kind and the Bell number for the dual path graph are, respectively, given by
[TABLE]
and
[TABLE]
where
3.7 deformed factorial and binomial moments
For a study on factorial and binomial moments, see [7]. We deal here with the generalization. For that, we consider a nonnegative integer-valued discrete random variable and the probability distribution of
[TABLE]
[TABLE]
referred to the order factorial and order binomial moments, respectively, of the random variable In the particular case of we define the mean value, also called the expectation value, of by
[TABLE]
The variance of is then obtained as
[TABLE]
Since and then
[TABLE]
Theorem 3.46
The binomial moment is given as function of the binomial moment as follows:
[TABLE]
while the factorial moment is given in terms of the factorial moment by
[TABLE]
where and is the deformed Stirling number of the first kind.
Proof: Multiplying (3.103) by the probability distribution and summing for all we deduce (3.115) from (3.116). Moreover, from
[TABLE]
and the relation (3.116), we derive (3.117).
Remark 3.47
Putting we obtain the usual binomial moment as function of the binomial moment as:
[TABLE]
while the usual factorial moment is given in terms of the factorial moment by
[TABLE]
where and is the Stirling number of the first kind.
Theorem 3.48
The deformed probability distribution of a discrete random variable is given by the absolutely convergent series
[TABLE]
Proof: Replacing by and by in expression (3.115), multiplying it by
[TABLE]
and summing for all we obtain
[TABLE]
Note that the probability distribution (2.14) can be retrieved by taking
Remark 3.49
*The particular case of the generalized Quesne factorial and binomial moment, and probability distribution is detailed as follows: *
- (1)
Let be a nonnegative integer-valued discrete random variable and the probability distribution of Assume the convergence of the series:
[TABLE]
[TABLE]
*here designated by **order generalized Quesne factorial and *order generalized Quesne binomial moment, respectively, of the random variable In the particular case of we deduce the generalized Quesne mean value, also called the generalized Quesne expectation value, of by
[TABLE]
The associated variance of is then obtained as
[TABLE]
or, equivalently,
[TABLE] 2. (2)
*Its deformed binomial moment is given by *
[TABLE]
while the factorial moment is expressed in terms of the generalized Quesne factorial moment by
[TABLE]
where and is the generalized Quesne Stirling number of the first kind. 3. (3)
The probability distribution of a discrete random variable is given by
[TABLE]
4 Concluding remarks
In this paper, we have developed and illustrated the fundamentals of deformed combinatorics, with a special focus on factorials, binomial coefficients, Vandermonde’s and Cauchy’s formulae, binomial formula, Stirling numbers, and Bell numbers induced by the deformed quantum algebra. These results have also been derived and discussed in the particular case of the so-called generalized Quesne deformed quantum algebra. Relevant properties have been deduced and analyzed in this framework.
Acknowledgements
This work is supported by TWAS Research Grant RGA No.17 - 542 RG/ MATHS/AF/AC _G - FR3240300147. The ICMPA-UNESCO Chair is in partnership with the Association pour la Promotion Scientifique de l’Afrique (APSA), France, and Daniel Iagolnitzer Foundation (DIF), France, supporting the development of mathematical physics in Africa. MNH acknowledges his colleagues Nicholas M. J. Hall, Isabelle Dadou, Yves Morel, Catherine Jeandel, the staff of the UMR 5566 Laboratoire d’Etudes en Géophysique et Océanographique Spatiales (LEGOS) of the Faculté des Sciences et Ingénierie, Michael Toplis, Director of the Observatoire Midi-Pyrénées, and Nguyen Tien Zung of the Institut de Mathématiques de Toulouse for their hospitality during his stay, as visiting professor, at the Université Toulouse III Paul Sabatier, where this work has been completed. MNH is also grateful to Mrs Sophie Raynaud, Head of International Relations Office, and Prof. Fabrice Dumas, Vice-president in charge of International Relations, Université Toulouse III Paul Sabatier, for all their solicitude.
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