Abstract
In the paper, the authors present some symmetric identities involving the Stirling polynomials and higher order Bernoulli polynomials under all permutations in the finite symmetric group of degree n. These identities extend and generalize some known results.
    Keywords:
                                                                    symmetric identity;                    Stirling polynomial;                    Stirling number of the second kind;                    finite symmetric group;                    permutation;                    higher order Bernoulli polynomial        MSC:
                Primary 20C30; Secondary 05A19, 11B68, 11B73
            1. Introduction
The Stirling numbers arise in a variety of analytic and combinatorial problems. They were introduced in the eighteenth century by James Stirling. There are two kinds of the Stirling numbers: the Stirling numbers of the first and second kind. Some combinatorial identities for the Stirling numbers of these two kinds are studied and collected in [,,,,,,,] and closely related references.
The Stirling numbers of second kind  are the numbers of ways to partition a set of n elements into k nonempty subsets. It can be computed by
      
      
        
      
      
      
      
    
      and can be generated by
      
      
        
      
      
      
      
    
The Stirling polynomials  can be generated [,,,,,] by
      
      
        
      
      
      
      
    
      and the first five Stirling polynomials  for  are
      
      
        
      
      
      
      
    
The Stirling polynomials  generalize several important sequences of numbers, including the Stirling numbers of the second kind  and the Bernoulli numbers , appearing in combinatorics, number theory, and analysis.
In the case  for  in Equation (1), we can derive
      
      
        
      
      
      
      
    
	  Equating coefficients on the very ends of the above identity arrives at
      
      
        
      
      
      
      
    
      for .
It is common knowledge [] that the Bernoulli numbers  are generated by
      
      
        
      
      
      
      
    
	  By considering the case  in Equation (1) and the definition in Equation (3) for the Bernoulli numbers , we have
      
      
        
      
      
      
      
    
	  Comparing the coefficients on both sides of this equation results in
      
      
        
      
      
      
      
    
The higher order Bernoulli numbers  for  and  can be generated [,,] by
      
      
        
      
      
      
      
    
	  Combining this with Equation (1) yields the relation
      
      
        
      
      
      
      
    
In the paper [], some new symmetric identities for the q-Bernoulli polynomials are derived from the fermionic integral on . In [,], the method in the paper [] is extended to the q-Euler and q-Genocchi polynomials, respectively. In [], some symmetric identities involving the Stirling polynomials  are investigated. The symmetric identities of some special polynomials, such as higher order Bernoulli polynomials , higher order q-Euler polynomials, degenerate generalized Bernoulli polynomials, and degenerate higher order q-Euler polynomials, have been studied by several mathematicians in [,,,,,] and closely related references therein.
The purpose of this paper is to investigate some interesting symmetric identities involving the Stirling polynomials  under the finite symmetric group . By specializing these identities, we can obtain some new symmetric identities involving the Stirling polynomials .
2. Symmetric Identities of Stirling Polynomials
Now, we start out to state and prove our main results.
Theorem 1. 
Let  and . Then, the expression
      
        
      
      
      
      
    is invariant under any permutation , where ,
      
        
      
      
      
      
    and  for .
Proof.  
For convenience, we denote . Define
        
      
        
      
      
      
      
    
		It is clear that we can rewrite I as
        
      
        
      
      
      
      
    
		By applying Equations  (1)–(8), we can rearrange the equality in Equation (7) as
        
      
        
      
      
      
      
    
Combining the above three equalities leads to the expression
        
      
        
      
      
      
      
    
        which are invariant under any permutations . □
Corollary 1. 
Let  and . Then, the quantities
      
        
      
      
      
      
    are invariant under any permutation .
Replacing x by  for  in Theorem 1 and employing Equation (2) result in the following corollary.
Corollary 2. 
Let  and . Then the expressions
      
        
      
      
      
      
    are invariant under any permutations .
Finally, combining Corollary 2 with Equation (4) leads to the following corollary.
Corollary 3. 
Let  and . Then the expressions
      
        
      
      
      
      
    are invariant under any permutations .
From Theorem 1 to Corollary 3, if taking , then we have the following corollaries.
Corollary 4. 
Let  be any positive integers, n be any non-negative integer. Then the expressions
      
        
      
      
      
      
    and
      
        
      
      
      
      
    are invariant under any permutations of .
Corollary 5. 
For  and ,the expressions
      
        
      
      
      
      
    are invariant under any permutations of .
Corollary 6. 
For  and , the expressions
      
        
      
      
      
      
    are invariant under any permutations of .
3. Symmetric Identities via Higher Order Bernoulli Polynomials
Recall from [] that higher order Bernoulli polynomials  can be generated by
      
      
        
      
      
      
      
    
	  Now, we start out to investigate symmetric identities for the Stirling polynomials  under the finite symmetric group  via higher order Bernoulli polynomials .
Theorem 2. 
Let  and . Then the quantities
      
        
      
      
      
      
    are invariant under any permutations , where  is defined by Equation (6).
Proof.  
Define  as
        
      
        
      
      
      
      
    
		Then we can rewrite  as
        
      
        
      
      
      
      
    
		Applying Equations (1) and (9) to the equality in Equation (10) gives
        
      
        
      
      
      
      
    
Similarly, we can rewrite  as
        
      
        
      
      
      
      
    
Inductively, for any , we can rearrange  as
        
      
        
      
      
      
      
    
From Theorem 2, we can derive the following interesting results in a simple way.
Corollary 7. 
Let  and . Then the expressions
      
        
      
      
      
      
    are invariant under all permutations .
Replacing x by  for  in Theorem 2 and using the equality in Equation (2) arrive at the following corollary.
Corollary 8. 
Let  and . Then the expressions
      
        
      
      
      
      
    are invariant under all permutations .
Finally, combining Corollary 8 with Equation (4) leads to the following corollary.
Corollary 9. 
For  and  such that , the quantities
      
        
      
      
      
      
    are invariant under all permutations .
Corollary 10. 
For  and , the quantities
      
        
      
      
      
      
    are invariant under all permutations .
Corollary 11. 
For  and , the quantities
      
        
      
      
      
      
    are invariant under all permutations .
Corollary 12. 
For  such that  and , the quantities
      
        
      
      
      
      
    are invariant under all permutations .
Corollary 13. 
For  such that  and , the quantities
      
        
      
      
      
      
    are invariant under all permutations .
Remark 1. 
In view of Corollaries 10–13, by specializing  or , we can obtain many interesting symmetric identities for Stirling polynomials .
Author Contributions
The authors contributed equally to this work. The authors read and approved the final manuscript.
Funding
The first author was supported by the National Research Foundation of Korea (NRF) with Grant Numbers NRF-2016R1A5A1008055 and NRF-2018R1D1A1B07041846.
Acknowledgments
The authors are thankful to the anonymous referees for their careful corrections to and valuable comments on the original version of this paper.
Conflicts of Interest
The authors declare no conflict of interest.
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