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Article

A Class of the Generalized Ramanujan Tau Numbers and Their Associated Partition Functions

by
Aleksandar Petojević
1,
Hari M. Srivastava
2,3,4,5,6,7,* and
Sonja Orlić
1
1
Faculty of Education, University of Novi Sad, Podgorička 4, 25000 Sombor, Serbia
2
Department of Mathematics and Statistics, University of Victoria, Victoria, BC V8W 3R4, Canada
3
Department of Medical Research, China Medical University Hospital, China Medical University, Taichung 40402, Taiwan
4
Center for Converging Humanities, Kyung Hee University, 26 Kyungheedae-ro, Dongdaemun-gu, Seoul 02447, Republic of Korea
5
Department of Applied Mathematics, Chung Yuan Christian University, Chung-Li, Taoyuan City 320314, Taiwan
6
Department of Mathematics and Informatics, Azerbaijan University, 71 Jeyhun Hajibeyli Street, AZ 1007 Baku, Azerbaijan
7
Section of Mathematics, International Telematic University Uninettuno, I-00186 Rome, Italy
*
Author to whom correspondence should be addressed.
Axioms 2025, 14(6), 451; https://doi.org/10.3390/axioms14060451
Submission received: 18 April 2025 / Revised: 2 June 2025 / Accepted: 3 June 2025 / Published: 7 June 2025
(This article belongs to the Section Mathematical Analysis)

Abstract

:
In this paper, the authors derive some believed-to-be new recursion and explicit formulas for the generalized Ramanujan numbers τ s ( n ) ( s N { 1 } ) , where, as usual, N is the set of positive integers. The authors consider the associated partition functions and derive connections of the Eisenstein series with the numbers τ s ( n ) . Several related corollaries and consequences of each of the presented results are also given. The paper concludes by presenting an open problem that is related to one of these results.

1. Introduction and the Main Recursion Formulas

We define the generalized Ramanujan tau sequence { τ s ( n ) } n = 1 as follows:
n = 1 ( 1 z n ) s : = n = 1 τ s ( n ) z n 1 ( z C ; | z | < 1 ; z 0 ; s N { 1 } ) ,
where, as usual, N denotes the set of positive integers. Euler’s statement and Jacobi’s statement [1] (p. 429) imply that
n = 1 ( 1 z n ) = n = ( 1 ) n z ( 3 n 2 + n ) / 2 = n = 0 ( 1 ) n ( n + 1 ) 2 z a n = n = 1 τ 1 ( n ) z n 1
and
n = 1 ( 1 z n ) 3 = n = 0 ( 1 ) r ( 2 n + 1 ) z n ( n + 1 ) / 2 = n = 1 τ 3 ( n ) z n 1 ,
where { a j } j = 0 is a sequence of generalized pentagonal numbers (see, for details, [2] (A001318); see also [3]). In a special case, τ 24 ( n ) = τ ( n ) is a sequence of the Ramanujan tau numbers [2] (A000594). Ramanujan [4] (p. 14) gave the following recursion formula for τ ( n ) :
( n 1 ) τ ( n ) = 1 m α n ( 1 ) m + 1 ( 2 m + 1 ) n 1 9 2 m ( m + 1 ) · τ n m 2 ( m + 1 ) ,
where
α n : = 1 2 8 n + 1 1 .
The recursion formula contains no other known functions. We define the partition function p ( n ) as the following generating function (see [2] (A000041)):
n = 1 ( 1 z n ) 1 = n = 0 p ( n ) z n .
The function applies in cases when
τ 1 ( n + 1 ) = p ( n ) ( n N { 0 } ) .
The familiar recursion formula for the generalized Ramanujan tau numbers τ s ( n ) ( s = 1 , , 24 ) is based upon the Euler transformation and contains the following known divisor function:
σ m ( n ) : = d | n d m σ ( n ) : = σ 1 ( n ) .
From the work of Petojević [5] (p. 46, Eq. (11)) and the Online Encyclopedia of Integer Sequences [2] (A010815, A002107, A010816, …, A000594), we recall the following limit formula:
τ s ( n ) = s n 1 k = 1 n 1 σ ( k ) τ s ( n k ) .
Remark 1.
The method that is described in the proof of [5] (p. 46, Lemma 3) readily demonstrates that Formula (4) is valid for all natural numbers s.
The authors are not aware of the existence of any correct recursion formula for the numbers τ s ( n ) ( s = 1 , , 23 ) , which do not contain any known functions. However, the recursion formula
( n 1 ) τ ( n ) = 1 | m | β n n 1 25 2 m ( 3 m + 1 ) τ n m 2 ( 3 m + 1 ) ,
where
β n = 1 6 24 n + 1 + 1 ,
which was given by Lehmer in [6] (p. 487) and [4] (p. 14), contradicts some well-known facts. For example, from Lehmer’s formula for n = 11 one obtains β 11 2.88 , which implies that m { ± 1 , ± 2 } . Finally, we find that τ ( 11 ) = 722,292 , while the exact value is τ ( 11 ) = 534,612 (see Example 1; see also [7,8,9,10] for some recent developments pertaining to this connection).
Various interesting number sequences and other entities, which are related to the above-defined generalized Ramanujan sequence { τ s ( n ) } n 1 , have indeed continued to be studied widely and extensively in the recent literature on the subject (see, for example, ref. [11,12,13,14,15,16]). Motivated essentially by the aforementioned recent developments, we first prove recursion formulas for the generalized Ramanujan tau numbers { τ s ( n ) } n 1 associated with Equation (6), which do not have a known function.
Theorem 1.
Let s , n N . Then τ s ( 1 ) = 1 and
( n 1 ) τ s ( n ) = 1 m d n ( 1 ) m + 1 n 1 ( s + 1 ) m ( 3 m + 1 ) 2 τ s n m ( 3 m + 1 ) 2 + 1 m b n ( 1 ) m + 1 n 1 ( s + 1 ) m ( 3 m 1 ) 2 τ s n m ( 3 m 1 ) 2 ,
where
d n = 24 n 23 1 6 and b n = 24 n 23 + 1 6 .
Proof. 
First of all, Equation (1) produces the following formula:
d d z ln n = 1 τ s ( n ) z n = d d z ln z + ln n = 0 ( 1 ) n ( n + 1 ) 2 z a n s .
Applying the Cauchy rule for multiplying power series, we get
n = 1 ( n 1 ) τ s ( n ) z n = m = 1 k = 1 m ( 1 ) ( m k + 1 ) ( m k + 2 ) 2 ( s a m k + 1 k + 1 ) τ s ( k ) z a m k + 1 + k .
Hence, for m = n + j a j 1 and k = n a j , we have z n = z a m k + 1 + k , so that
( n 1 ) τ s ( n ) = 1 a j n 1 ( 1 ) j ( j + 1 ) 2 ( s + 1 ) a j n + 1 τ s ( n a j ) .
Therefore, the recursion formula asserted by Theorem 1 follows the following equality:
a n = 1 2 m ( 3 m + 1 ) n = 2 m ; m N 1 2 m ( 3 m 1 ) n = 2 m 1 ; m N .
Remark 2.
The values of d n and b n , given by Equation (5), do not depend on the choice of the number s. Petojević et al. [17] proved Theorem 1 for s = 24 . Also, for s = 1 , Theorem 1 holds true (see [18]).
Example 1.
We now calculate τ ( 11 ) by using Ramanujan’s Formula (3) and Theorem 1:
τ ( 11 ) = 3 τ ( 10 ) + 85 τ ( 8 ) 308 τ ( 5 ) + 720 τ ( 1 ) 10 = 534612
and
τ ( 11 ) = 15 τ ( 10 ) 40 τ ( 9 ) + 115 τ ( 6 ) + 165 τ ( 4 ) 10 = 534612 .

2. An Explicit Formula for the Numbers τ s ( n )

In this section, we first state and prove the following result.
Theorem 2.
Let s , n N , k i { 0 , 1 , 2 , , s } for i = 1 , , n 1 . Then
τ s ( n ) = i = 1 n 1 i · k i = n 1 ( 1 ) i = 1 n 1 k i i = 1 n 1 s k i .
Proof. 
Let m = 1 , 2 , , n 1 . If, in the sum
s 0 z m · 0 s 1 z m · 1 + s 2 z m · 2 + ( 1 ) s 1 s s 1 z m · ( s 1 ) + ( 1 ) s s s z m · s ,
where we denote the coefficient z m · k i by
s k i : = s k i , m ,
then the product m = 1 n 1 ( 1 z m ) s is equal to the sum of terms of the following form:
( 1 ) k i , 1 s k i , 1 ( 1 ) k i , 2 s k i , 2 ( 1 ) k i , n 1 s k i , n 1 z 1 · k i , 1 + 2 · k i , 2 + + ( n 1 ) · k i , n 1 .
Since we calculate the coefficient with z n 1 , the following condition must be fulfilled:
1 · k i , 1 + 2 · k i , 2 + + ( n 1 ) · k i , n 1 = n 1 ,
so that
τ s ( n ) = 1 · k 1 + 2 · k 2 + + ( n 1 ) · k n 1 = n 1 ( 1 ) k 1 + k 2 + + k n 1 s k 1 s k 2 s k n 1 ,
which evidently proves the formula as claimed. □
Remark 3.
Goran-Dumitru and Merca [13] (Th.5.1, p. 77) proved Theorem 2 for s = 24 .
Example 2.
Making use of the formula proven in Theorem 2, and for s = 24 , we find that
τ ( 1 ) = ( 1 ) 0 24 0 = 1 , τ ( 2 ) = ( 1 ) 1 24 1 = 24 , τ ( 3 ) = ( 1 ) 2 24 2 + ( 1 ) 1 24 1 = 252 τ ( 4 ) = ( 1 ) 3 24 3 + ( 1 ) 1 24 1 ( 1 ) 1 24 1 + ( 1 ) 1 24 1 = 1472 τ ( 5 ) = ( 1 ) 4 24 4 + ( 1 ) 2 24 2 ( 1 ) 1 24 1 + ( 1 ) 2 24 2 + ( 1 ) 1 24 1 ( 1 ) 1 24 1 + ( 1 ) 1 24 1 = 4830 . τ ( 6 ) = ( 1 ) 5 24 5 + ( 1 ) 3 24 3 ( 1 ) 1 24 1 + ( 1 ) 2 24 2 ( 1 ) 1 24 1 + ( 1 ) 1 24 1 ( 1 ) 2 24 2 + ( 1 ) 1 24 1 ( 1 ) 1 24 1 + ( 1 ) 1 24 1 = 6048 .

3. The s -Partition Function p s ( n )

We begin this section by introducing the following notations:
1 · k 1 + 2 · k 2 + + n · k n = n , s , n N , k i { 0 , 1 , 2 , , s } ( i = 1 , , n ) .
In what follows, we use the following notations and conventions:
  • p s ( n ) : the number of partitions of n that satisfy Equation (7) (Table 1).
  • i p s ( n ) : the number of partitions of n that do not satisfy Equation (7) (impossible partitions).
  • c ( n ) : the number of partitions of n that do not contain 1 as a part [2] (A002865).
  • w ( n ) : the nth number [2] (A092885).
  • x + x + + x m t i m e s : = m x .
  • · : the floor function of a real number, which is the largest integer not exceeding that real number.
Theorem 3.
Let n N . Then
p 24 ( n 1 ) p ( n 1 ) i = 1 n 1 25 p ( n 1 i · 25 ) .
Proof. 
In our proof of Theorem 3, we consider the following cases:
(1)
0 n 1 24 : p 24 ( n 1 ) = p ( n 1 ) = w ( n 1 ) .
(2)
25 n 1 49 : Based on the results presented in Table 2, we observe that the impossible partitions for n 1 = 29 are obtained by adding the number 1 to the impossible partitions for n 1 = 28 . The total number of such partitions is given by i p 24 ( 28 ) . In addition to these, we also consider the impossible partitions 25 1 + 2 + 2 and 25 1 + 4 , whose number is given by c ( 4 ) . Therefore, we find that
i p 24 ( 29 ) = i p 24 ( 28 ) + c ( 4 ) = 3 + 2 = 5 .
We now formulate the following generalization:
i p 24 ( n 1 ) = i p 24 ( n 2 ) + c ( n 1 25 ) = i p 24 ( n 3 ) + c ( n 2 25 ) + c ( n 1 25 ) = i p 24 ( n 4 ) + c ( n 3 25 ) + c ( n 2 25 ) + c ( n 1 25 ) k = 1 n 25 c ( n k 25 ) = p ( n 26 ) ,
so that
p 24 ( n 1 ) = p ( n 1 ) p ( n 26 ) = w ( n 1 ) .
(3)
50 n 1 74 : Analogously, we have i p 24 ( 50 ) = i p 24 ( 49 ) + number of partitions 25 1 + 25 , 25 1 + 23 + 2 , 25 1 + 22 + 3 , + number of partitions 25 2 . We then have
i p 24 ( 50 ) = i p 24 ( 49 ) + c 1 ( 25 ) + 1 = p ( 24 ) + c ( 25 ) + c ( 0 ) = p ( 25 ) + c ( 0 ) .
For n 1 = 51 , the impossible partition 25 2 + 1 is already included in the count of i p 24 ( 50 ) . Therefore, we can express the total number of impossible partitions for n 1 = 51 as follows:
i p 24 ( 51 ) = i p 24 ( 50 ) + c ( 26 ) + 0 = p ( 25 ) + c ( 26 ) + c ( 0 ) + c ( 1 ) = p ( 26 ) + p ( 1 ) .
This leads to the generalization given by
i p 24 ( n 1 ) = p ( n 26 ) + p ( n 51 ) ,
so that
p 24 ( n 1 ) = p ( n 1 ) p ( n 26 ) p ( n 51 ) = w ( n 1 ) .
(4)
75 n 1 99 : In this case, in addition to the partitions 25 1 and 25 2 , we also consider the partition 25 3 . Thus, clearly, we can write the total number of impossible partitions as i p 24 ( n 1 ) = p ( n 26 ) + p ( n 51 ) + p ( n 76 ) , so that
p 24 ( n 1 ) = p ( n 1 ) p ( n 26 ) p ( n 51 ) p ( n 76 ) = w ( n 1 ) p ( n 76 ) .
(5)
100 n 1 124 : For n 1 = 100 , the number of impossible partitions of the form
25 2 + 50 , 25 2 + 48 + 2 , 25 2 + 47 + 3 ,
is given by c ( 50 ) . Additionally, the number of impossible partitions of the following form
25 3 + 25 , 25 3 + 23 + 2 , 25 3 + 22 + 3 ,
is c ( 25 ) . We have the impossible partition 25 4 . This occurs when
i p 24 ( n 1 ) = p ( n 26 ) + p ( n 51 ) + p ( n 76 ) + 1 ,
which leads to the following expression for p 24 ( n 1 ) :
p 24 ( n 1 ) = p ( n 1 ) p ( n 26 ) p ( n 51 ) p ( n 76 ) 1 .
For n 1 = 101 , the impossible partition 25 4 + 1 is already included in the count of i p 24 ( 100 ) . Therefore, we can express the total number of impossible partitions for n 1 = 101 as follows:
p 24 ( n 1 ) = p ( n 1 ) p ( n 26 ) p ( n 51 ) p ( n 76 ) 1 0 .
For n 1 = 102 , the expression for p 24 ( n 1 ) is given by
p 24 ( n 1 ) = p ( n 1 ) p ( n 26 ) p ( n 51 ) p ( n 76 ) 1 0 1 .
For n 1 = 103 , we adjust the formula as follows:
p 24 ( n 1 ) = p ( n 1 ) p ( n 26 ) p ( n 51 ) p ( n 76 ) 1 0 1 1 .
In general, we can express p 24 ( n 1 ) as follows:
p 24 ( n 1 ) = p ( n 1 ) p ( n 26 ) p ( n 51 ) p ( n 76 ) p ( n 101 ) = w ( n 1 ) p ( n 76 ) p ( n 101 ) .
(6)
125 n 1 149 : For n 1 = 125 , the number of impossible partitions of the form
25 2 + 75 , 25 2 + 73 + 2 , 25 2 + 72 + 3 , , 25 2 + 25 3 , , 25 3 + 50 , 25 3 + 48 + 2 , 25 7 + 47 + 3 , , 25 3 + 25 2 , , 25 4 + 25 , 25 4 + 23 + 2 , 25 4 + 22 + 3 , , 25 5
are given by c ( 75 ) , c ( 50 ) , c ( 25 ) , and 1, respectively. However, we note that the partition 25 2 + 25 3 has been counted twice. This occurs when
i p 24 ( n 1 ) = p ( n 26 ) + p ( n 51 ) + p ( n 76 ) + p ( n 101 ) + 1 1 ,
which leads to the following expression for p 24 ( n 1 ) :
p 24 ( n 1 ) = p ( n 1 ) p ( n 26 ) p ( n 51 ) p ( n 76 ) p ( n 101 ) 1 + 1 .
For n 1 = 126 , we obtain the following expression for p 24 ( n 1 ) :
p 24 ( n 1 ) = p ( n 1 ) p ( n 26 ) p ( n 51 ) p ( n 76 ) p ( n 101 ) 1 0 + 1 + 0 .
For n 1 = 127 , the expression for p 24 ( n 1 ) is given by
p 24 ( n 1 ) = p ( n 1 ) p ( n 26 ) p ( n 51 ) p ( n 76 ) p ( n 101 ) 1 0 1 + 1 + 0 + 1 .
For n 1 = 128 , we have
p 24 ( n 1 ) = p ( n 1 ) p ( n 26 ) p ( n 51 ) p ( n 76 ) p ( n 101 ) 1 0 1 1 + 1 + 0 + 1 + 1 .
For n 1 = 129 , we observe that certain partitions are double-counted. Specifically, the partitions of the following form:
25 2 + 25 3 + 2 + 2 and 25 2 + 25 3 + 4
are counted more than once. In order to correct this, we adjust the formula as follows:
p 24 ( n 1 ) = p ( n 1 ) p ( n 26 ) p ( n 51 ) p ( n 76 ) p ( n 101 ) p ( n 126 ) + 1 + 0 + 1 + 1 + 2 .
In this procedure, we mark the number of impossible partitions that are repeated for the number n 1 with r 24 ( n 1 ) —that is,
r 24 ( 125 ) = 1 , r 24 ( 126 ) = 1 , r 24 ( 127 ) = 2 , r 24 ( 128 ) = 3 , and r 24 ( 129 ) = 5 .
Thus, in general, we can express p 24 ( n 1 ) as follows:
p 24 ( n 1 ) = p ( n 1 ) p ( n 26 ) p ( n 51 ) p ( n 76 ) p ( n 101 ) p ( n 126 ) + r 24 ( n 1 ) = p ( n 1 ) p ( n 26 ) p ( n 51 ) p ( n 76 ) p ( n 101 ) p ( n 126 ) + p ( n 126 ) = p ( n 1 ) p ( n 26 ) p ( n 51 ) p ( n 76 ) p ( n 101 ) = w ( n 1 ) p ( n 76 ) p ( n 101 ) .
If we continue this procedure, we get
p 24 ( n 1 ) = p ( n 1 ) i = 1 n 1 25 p ( n 1 i · 25 ) + r 24 ( n 1 ) .
Remark 4.
For s , n N , what is the value of p s ( n 1 ) ? For s = 24 , 150 n 1 , and 24 s N ( n N ) , the problem remains open.

4. Connection of the Eisenstein Series with the Numbers τ s ( n )

For each positive even integer m, the Eisenstein series E m ( q ) is defined as follows (see [19]; see also the several interesting recent developments reported in [20,21,22,23]):
E m ( q ) : = 1 2 m B m n = 1 σ m 1 ( n ) q n ( ( z ) > 0 ) ,
where q = e 2 π i z is the complex power-series variable and B m represents the Bernoulli numbers defined by the generating function
n = 0 B n x n n ! = x e x 1 .
The Eisenstein series are widely applied in the theory of modular forms. In this connection, it seems to be necessary to mention some more facts about modular forms.
Theorem 4.
Let s , n N . Then
n = 1 τ s ( n ) z n 1 = exp s n = 1 σ ( n ) n z n
or, equivalently,
n = 1 ( 1 z n ) s = exp s n = 1 σ ( n ) n z n .
Proof. 
Based on Equation (4), we have the following equalities:
n = 1 n τ s ( n ) z n = n = 1 τ s ( n ) z n s n = 1 z n k = 1 n 1 σ ( k ) τ s ( n k ) ,
so that
n = 1 n τ s ( n ) z n n = 1 τ s ( n ) z n = 1 s n = 1 z n k = 1 n 1 σ ( k ) τ s ( n k ) n = 1 τ s ( n ) z n
and that
n = 1 n τ s ( n ) z n n = 1 τ s ( n ) z n = 1 s n = 1 σ ( n ) z n ,
that is,
n = 1 n τ s ( n ) z n 1 n = 1 τ s ( n ) z n = 1 z s n = 1 σ ( n ) z n 1 ,
which readily yields
d d z ln n = 1 τ s ( n ) z n = 1 z s n = 1 σ ( n ) z n 1 .
Upon integrating both sides of this last equation, we find that
ln n = 1 τ s ( n ) z n = ln z s n = 1 σ ( n ) n z n ,
so that
ln n = 1 τ s ( n ) z n 1 = s n = 1 σ ( n ) n z n .
Hence, clearly, we conclude that
n = 1 τ s ( n ) z n 1 = exp s n = 1 σ ( n ) n z n .
Remark 5.
It is also possible to prove Theorem 4 based on the following identity:
ln ( 1 z n ) = 0 z n t n 1 1 t n d t ( | z | < 1 ) .
If we choose s = 24 , that is, τ 24 = τ ( n ) , and set m = 2 in Definition (8), we obtain the generating function for Ramanujan’s tau numbers using the Eisenstein series E 2 ( z ) . From Theorem 4, we then have
n = 1 τ ( n ) z n = z exp 24 n = 1 σ ( n ) n z n ,
so that
n = 1 τ ( n ) z n = exp 0 z E 2 ( t ) t d t .

5. Decomposition of the Numbers τ s ( n )

Brent [24] (Theorem 3.1) proved the following formula for computing Ramanujan’s τ ( n ) -function values:
τ ( n + 1 ) = 1 · k 1 + 2 · k 2 + + ( n 1 ) · k n = n ( 24 ) k 1 + k 2 + + k n σ ( 1 ) k 1 σ ( 2 ) k 2 σ ( n ) k n 1 k 1 k 1 ! 2 k 2 k 2 ! n k n k n ! .
In our next result (see Theorem 5 below), we will prove an analogous decomposition for τ s ( n ) where s N .
Theorem 5.
Let 1 < n N and s N . Then
τ s ( n ) = i = 1 n 1 i · k i = n 1 ( s ) i = 1 n 1 k i i = 1 n 1 σ ( i ) k i i k i k i ! k i N { 0 } .
Proof. 
We present an elementary proof based on Theorem 4 and the expansion of function e z . According to Theorem 4, we have the following equations:
n = 1 τ s ( n ) z n 1 = exp s n = 1 σ ( n ) n z n = exp s σ ( 1 ) 1 z 1 s σ ( 2 ) 2 z 2 s σ ( 3 ) 3 z 3 s σ ( 4 ) 4 z 4 .
Hence, clearly, the expansion of the function e z yields
n = 1 τ s ( n ) z n 1 = ( s σ ( 1 ) z 1 ) 0 1 0 0 ! + ( s σ ( 1 ) z 1 ) 1 1 1 1 ! + ( s σ ( 1 ) z 1 ) 2 1 2 2 ! + · ( s σ ( 2 ) z 2 ) 0 2 0 0 ! + ( s σ ( 2 ) z 2 ) 1 2 1 1 ! + ( s σ ( 2 ) z 2 ) 2 2 2 2 ! + · ( s σ ( 3 ) z 3 ) 0 3 0 0 ! + ( s σ ( 3 ) z 3 ) 1 3 1 1 ! + ( s σ ( 3 ) z 3 ) 2 3 2 2 ! + · ( s σ ( n 1 ) z n 1 ) 0 ( n 1 ) 0 0 ! + ( s σ ( n 1 ) z n 1 ) 1 ( n 1 ) 1 1 ! +
In order to compute the value for τ ( n ) , we need to calculate the coefficient of z n 1 on the right-hand side of this last equation. For this reason, we consider the following product:
1 + ( s σ ( 1 ) z 1 ) 1 1 1 1 ! + ( s σ ( 1 ) z 1 ) 2 1 2 2 ! + ( s σ ( 1 ) z 1 ) 3 1 3 3 ! + · 1 + ( s σ ( 2 ) z 2 ) 1 2 1 1 ! + ( s σ ( 2 ) z 2 ) 2 2 2 2 ! + + ( s σ ( 2 ) z 2 ) 3 2 3 3 ! · 1 + ( s σ ( 3 ) z 3 ) 1 3 1 1 ! + ( s σ ( 3 ) z 3 ) 2 3 2 2 ! + ( s σ ( 3 ) z 3 ) 3 3 3 3 ! + · 1 + ( s σ ( n 1 ) z n 1 ) 1 ( n 1 ) 1 1 ! + ( s σ ( n 1 ) z n 1 ) 2 ( n 1 ) 2 2 ! + ( s σ ( n 1 ) z n 1 ) 3 ( n 1 ) 3 3 ! + .
In the formation of the coefficient of z n 1 in the specified product, each factor contributes a single term from the sum of the type:
( s ) k i [ σ ( i ) ] k i z i k i i k i k i ! ( k i N { 0 } ) .
It is clear that the following condition must be satisfied:
1 · k 1 + 2 · k 2 + + ( n 1 ) · k n 1 = n 1 ,
so that
τ s ( n ) = 1 · k 1 + 2 · k 2 + + ( n 1 ) · k n 1 = n 1 ( s ) k 1 + k 2 + + k n 1 · [ σ ( 1 ) ] k 1 [ σ ( 2 ) ] k 2 [ σ ( n 1 ) ] k n 1 1 k 1 · k 1 ! · 2 k 2 · k 2 ! ( n 1 ) k n 1 · k n 1 ! .
Example 3.
We use the formula that was proven in Theorem 5. For s = 24 , we thus find that
τ ( 2 ) = ( 24 ) 1 [ σ ( 1 ) ] 1 1 1 · 1 ! = 24 ,
τ ( 3 ) = ( 24 ) 2 [ σ ( 1 ) ] 2 ] 1 2 · 2 ! + ( 24 ) 1 [ σ ( 2 ) ] 1 2 1 · 1 ! = 252 ,
τ ( 4 ) = ( 24 ) 3 [ σ ( 1 ) ] 3 1 3 · 3 ! + ( 24 ) 2 [ σ ( 1 ) ] 1 1 1 · 1 ! [ σ ( 2 ) ] 1 2 1 · 1 ! + ( 24 ) 1 [ σ ( 3 ) ] 1 3 1 · 1 ! = 1472 ,
and
τ ( 5 ) = ( 24 ) 4 [ σ ( 1 ) ] 4 1 4 · 4 ! + ( 24 ) 3 [ σ ( 1 ) ] 2 1 2 · 2 ! [ σ ( 2 ) ] 1 2 1 · 1 ! + ( 24 ) 2 [ σ ( 1 ) ] 1 1 1 · 1 ! [ σ ( 3 ) ] 1 3 1 · 1 ! + ( 24 ) 2 [ σ ( 2 ) ] 2 2 2 · 2 ! + ( 24 ) 1 [ σ ( 4 ) ] 1 4 1 · 1 ! = 4830 .
Remark 6.
Recently, Goran-Dumitru and Merca [13] established multiple decompositions of Ramanujan’s τ-function as sums over all partitions.

6. Concluding Remarks and Observations

In this concluding section, we introduce the following notation:
m z m { f ( z ) } : = f ( z ) ( m ) = : f ( m ) ( m N 0 ) .
Based on Theorem 4, here we demonstrate another possible decomposition of the Ramanujan τ -function. Let the function f : = f ( z ) be given as follows:
f = s n = 1 σ ( n ) n z n .
We then obtain
n = 1 τ s ( n ) z n 1 ( n 1 ) z = 0 = e f ( n 1 ) z = 0 ,
that is,
( n 1 ) ! τ s ( n ) = e f ( n 1 ) z = 0 .
Let us examine the derivatives of the function e f at point z = 0 . We thus find that
e f ( 1 ) z = 0 = e f f ( 1 ) z = 0 = f ( 1 ) z = 0 ,
e f ( 2 ) z = 0 = e f f ( 1 ) 2 + e f f ( 2 ) z = 0 = f ( 1 ) 2 + f ( 2 ) z = 0 ,
e f ( 3 ) z = 0 = e f f ( 1 ) 3 + 3 e f f ( 1 ) f ( 2 ) + e f f ( 3 ) z = 0 = f ( 1 ) 3 + 3 f ( 1 ) f ( 2 ) + f ( 3 ) z = 0
and
e f ( 4 ) z = 0 = e f f ( 1 ) 4 + 6 e f f ( 1 ) 2 f ( 2 ) + 3 e f f ( 2 ) 2 z = 0 + 4 e f f ( 1 ) f ( 3 ) + e f f ( 4 ) z = 0 = f ( 1 ) 4 + 6 f ( 1 ) 2 f ( 2 ) + 3 f ( 2 ) 2 + 4 f ( 1 ) f ( 3 ) + f ( 4 ) z = 0 .
Hence, finally, we choose to conjecture that
( n 1 ) ! τ s ( n ) = j b j f ( 1 ) a j , 1 f ( 2 ) a j , 2 f ( n 1 ) a j , n 1 z = 0 ,
where the sum taken over all admissible j and
1 · a j , 1 + 2 · a j , 2 + + ( n 1 ) · a j , n 1 = n 1 .
Remarkably, the computation of each of the coefficients
b j and a j , i ( i { 1 , 2 , 3 , , n 1 } ) ,
which are involved in our conjecture as given in (11), remains an open problem.

Author Contributions

Methodology, A.P.; validation, A.P., H.M.S. and S.O.; software, S.O.; formal analysis, A.P. and H.M.S.; investigation, A.P., H.M.S. and S.O.; writing–original draft preparation, A.P. and S.O.; writing–review and editing, A.P. and H.M.S.; Supervision, A.P. and H.M.S. All authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Data Availability Statement

Data are contained within the article.

Conflicts of Interest

The authors declare that they have no conflicts of interest.

References

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Table 1. The s-partition function p s ( n ) for s = 1 , 2 , 3 , 4 and n = 1 , 2 , , 8 .
Table 1. The s-partition function p s ( n ) for s = 1 , 2 , 3 , 4 and n = 1 , 2 , , 8 .
n12345678
p 1 ( n ) 11111111
p 2 ( n ) 122457913
p 3 ( n ) 1234691216
p 4 ( n ) 12356101318
Table 2. The impossible partition i p 24 ( n 1 ) for n 1 = 25 , 26 , 27 , 28 , 29 .
Table 2. The impossible partition i p 24 ( n 1 ) for n 1 = 25 , 26 , 27 , 28 , 29 .
n 1 Impossible Partitions ip 24 ( n 1 )
25 25 1 1
26 26 1 1
27 27 1 25 1 + 2 2
28 28 1 26 1 + 2 25 1 + 3 3
29 29 1 27 1 + 2 26 1 + 3 25 1 + 2 + 2 25 1 + 4 5
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Petojević, A.; Srivastava, H.M.; Orlić, S. A Class of the Generalized Ramanujan Tau Numbers and Their Associated Partition Functions. Axioms 2025, 14, 451. https://doi.org/10.3390/axioms14060451

AMA Style

Petojević A, Srivastava HM, Orlić S. A Class of the Generalized Ramanujan Tau Numbers and Their Associated Partition Functions. Axioms. 2025; 14(6):451. https://doi.org/10.3390/axioms14060451

Chicago/Turabian Style

Petojević, Aleksandar, Hari M. Srivastava, and Sonja Orlić. 2025. "A Class of the Generalized Ramanujan Tau Numbers and Their Associated Partition Functions" Axioms 14, no. 6: 451. https://doi.org/10.3390/axioms14060451

APA Style

Petojević, A., Srivastava, H. M., & Orlić, S. (2025). A Class of the Generalized Ramanujan Tau Numbers and Their Associated Partition Functions. Axioms, 14(6), 451. https://doi.org/10.3390/axioms14060451

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