REVIEW 1 major objections 4 minor 12 references
A note on new type degenerate Srirling numbers of the first kind
T0 review · 1 major / 4 minor · reviewed 2026-08-05 · deepseek-v4-flash
Pith's one-line read A one-parameter deformation of Stirling numbers of the first kind is shown to satisfy a finite-sum probabilistic identity that reduces to the classical random-variable formula when the parameter vanishes.
desk verdict The first-kind half is sound and the probabilistic identity is a clean Adell-Lekuona analog, but the second-kind definition (17) is inconsistent with the expansion and theorem that follow it. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The central object is the random sum S_k = U_1X_1 + ⋯ + U_kX_k and the identity E[e^{S_k}_λ(t)] = (1/((1/λ)log(1+λt)))^k log^k(1/(1−(1/λ)log(1+λt))). This identity links the generating function of the new first-kind numbers to an expectation, allowing the degenerate exponential to be expanded through the falling factorial (S_k)_{l,λ} and the logarithmic factor through ordinary Stirling numbers S1(m,k). That expansion is what produces the finite-sum probabilistic formula. For the second-kind family, the analogous engine is the expansion of (1/λ)(e^{λ(e^t−1)}−1) in powers of (e^t−1), which turns the defining series into a convolution of ordinary Stirling numbers of the second kind.
What would settle it
Expand Eq. (17) literally at k=1: the coefficient of t^1/1! on the left is (1/λ)·(d/dt)e_λ(e^t−1)|_{t=0}=1/λ, whereas Theorem 3.1 gives {1 1}^*_λ=1. Replacing the base with e^{λ(e^t−1)} makes the coefficient 1, matching the theorem and the ordinary λ→0 limit. Checking this first coefficient decides which definition the paper's result requires.
Extended reading notes
Core claim
Starting from the generating function for the unsigned new type degenerate Stirling numbers of the first kind, the paper proves Theorem 2.1: these numbers equal Σ_{m=k}^n λ^{n−m} binom(n,m) [m k]. The main result, Theorem 2.2, states that for n≥k≥1, [n k]^*_{−λ} = Σ_{m=k}^n λ^{m−k} binom(n,m) S1(m,k) E[(S_k)_{n−m,λ}], where S_k is the sum of k independent products of a uniform(0,1) and an exponential(1) random variable. The proof uses the identity E[e^{S_k}_λ(t)] = ((1/λ)log(1+λt))^{-k} log^k(1/(1−(1/λ)log(1+λt))), which converts the defining generating function into an expectation of a degenerate exponential. Letting λ→0 recovers the classical identity [n k] = binom(n,k) E[S_k^{n−k}]. The c
Load-bearing premise
The proof of the second-kind formula assumes that the defining generating function really uses e^{λ(e^t−1)} rather than the degenerate exponential e_λ(e^t−1) shown in the manuscript; if the printed expression is taken literally, the expansion in the proof is wrong.
Editorial extensions
If this is right
- Each new first-kind number is a polynomial in λ with integer coefficients, thanks to the finite sum in Theorem 2.1, and the paper's tables show that a wide range of values can be computed directly from ordinary Stirling numbers.
- Theorem 2.2 provides a finite-sum identity, so the expectation E[(S_k)_{n−m,λ}] can be replaced by the explicit k-fold integral displayed in Theorem 2.3, giving an integral representation for every new first-kind number.
- Both new families limit to the ordinary Stirling numbers as λ→0, so the construction is a genuine one-parameter extension rather than an unrelated sequence.
- The convolution structure in Theorems 2.1 and 3.1 means the new numbers are computable from binomial coefficients and classical Stirling numbers with no need to evaluate expectations numerically.
- The generating-function identities give a route to recurrences and further identities for the new families by standard manipulations of exponential generating functions.
Reading between the lines
- The printed definition (17), read literally with the degenerate exponential e_λ(e^t−1), does not support the expansion used to prove Theorem 3.1; the theorem goes through only if the intended base is e^{λ(e^t−1)}, and the λ→0 limit confirms that this is almost certainly the intended definition.
- The same probabilistic device could define degenerate analogues of Bell, Dowling, or derangement numbers by substituting e^{λ(e^t−1)}-type bases into their generating functions, with the same ordinary-Stirling expansion producing finite-sum formulas.
- Because S_k is a sum of k independent products of uniform and exponential variables, Theorem 2.2 suggests asymptotic and moment formulas for the new numbers as n grows, a direction the paper does not pursue.
- The explicit polynomial-in-λ formulas in Theorems 2.1 and 3.1 invite further study of divisibility properties or roots as λ varies, which is not addressed in the paper.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper defines a one-parameter family of 'new type degenerate' unsigned Stirling numbers of the first kind via the generating function (8), proves an explicit finite convolution formula (Theorem 2.1), and derives a finite-sum probabilistic representation (Theorem 2.2) in the style of Adell-Lekuona, with the parameter limit recovering the classical identity (5). It then introduces, by inversion, a 'new type degenerate' Stirling number of the second kind and claims an analogous convolution formula (Theorem 3.1). The first-kind results are derived cleanly; the second-kind section, as printed, contains a mismatch between the definition and the proof.
Significance. The first-kind representation (15) is correct and gives a genuine degenerate analogue of the Adell-Lekuona identity, with a transparent derivation from a probabilistic calculation. If the typesetting error in (17) is corrected, Theorem 3.1 provides a natural inverse family and explicit convolution formula. The results are modest—the numbers are finite sums of classical Stirling numbers—but they are coherent and the probabilistic interpretation is a useful addition. The paper's proofs are elementary and checkable; no parameter fitting or circular reasoning is involved.
major comments (1)
- [Sec. 3, Eq. (17) through Theorem 3.1] As printed, Eq. (17) defines the second-kind numbers using e_λ(e^t−1) = (1+λ(e^t−1))^{1/λ}. This is inconsistent with the expansion in Eq. (18), which is valid for e^{λ(e^t−1)}. For example, for k=1 the coefficient of t^2/2! in the printed (17) is 2/λ−1, while Theorem 3.1 and the table give {2 1}^*_λ = 1+λ. The stated λ→0 limit also fails for the printed definition. Since Theorem 3.1 and its table depend entirely on Eq. (18), the theorem is unproved as stated. The intended definition is evidently ((e^{λ(e^t−1)}−1)/λ)^k/k!, which is the compositional inverse of the first-kind generating function; please correct (17) and the note following it.
minor comments (4)
- [Title and abstract] Typo in title: 'Srirling' should be 'Stirling'; the header also has an unwanted space in 'DEGENERA TE'.
- [Sec. 3, after Theorem 3.1] The sentence 'we illustrate the values of the unsigned new type degenerate Stirling numbers of the first kind' should refer to the second-kind numbers defined in (17).
- [Eq. (15) paragraph] 'By taking λ → 0 in (15) and using (9)' is ungrammatical; suggest 'Taking λ → 0 in (15) and using (9), we recover (5).'
- [Throughout] Minor typos: 'plynomial' should be 'polynomial', 'Furthemore' should be 'Furthermore', 'probabilty' should be 'probability'. Some displayed tables lack column headers, which would help readability.
Circularity Check
No significant circularity: the new-number identities are direct generating-function expansions; the self-citations are not load-bearing.
full rationale
The central results are obtained by direct coefficient extraction from the stated generating functions, not by fitting or by assuming the target. Theorem 2.1 (Eq. 10) expands (8) using the standard series for log(1−λt) and the definition of ordinary Stirling numbers of the first kind; Theorem 2.2 (Eqs. 11–15) computes the degenerate moment generating function of Sk explicitly, multiplies by the reciprocal factor, and compares coefficients; Theorem 3.1 (Eq. 18) expands the second-kind generating function using the ordinary Stirling expansion of (e^{λ(e^t−1)}−1)^k. These are algebraic derivations from the definitions. The citations to the authors' earlier papers [4,5,6,7,8,12] provide background definitions and standard identities; the definitions used here are restated in the paper and are independently verifiable, so they are not load-bearing self-citations. No parameter is fitted to reproduce a target, and no uniqueness claim is imported from the authors' prior work. The only notable issue is a non-circular correctness/typo concern: Eq. (17) prints e_λ(e^t−1), while the expansion in Eq. (18) is valid for the compositional inverse e^{λ(e^t−1)}; this is an algebraic inconsistency, not a circularity. Hence score 0.
Assumptions & free parameters
assumptions (4)
- standard math Classical Stirling number generating function identities in (2), (4), (10), and (18).
- standard math Degenerate exponential e_lambda(t) = (1+lambda t)^{1/lambda} and its product property e_{x+y} = e_x e_y.
- domain assumption Probabilistic model with U independent uniform on (0,1) and X independent exponential with rate 1, plus interchange of expectation and coefficient extraction.
- ad hoc to paper The definitions (7) and (17) determine well-defined formal power series and hence well-defined number sequences.
invented entities (2)
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Unsigned new type degenerate Stirling numbers of the first kind [n k]*_lambda
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New type degenerate Stirling numbers of the second kind {n k}^*_lambda
Cite this review
Pith. "Pith review of A note on new type degenerate Srirling numbers of the first kind." pith.science (2026). https://pith.science/paper/JWC6C6KK
@misc{pith2026250903415,
author = {Pith},
title = {Pith review of: A note on new type degenerate Srirling numbers of the first kind},
year = {2026},
howpublished = {\url{https://pith.science/paper/JWC6C6KK}},
note = {Machine review of arXiv:2509.03415}
}
read the original abstract
We introduce a new sequence of unsigned degenerate Stirling numbers of the first kind. Following the work of Adell-Lekuona, who represented unsigned Stirling numbers of the first kind as multiples of the expectations of specific random variables, we express our new numbers as finite sums of multiples of the expectations of certain random variables. We also provide a representation of these new numbers as finite sums involving the classical unsigned Stirling numbers of the first kind. As an inversion formula, we define a corresponding sequence of new type degenerate Stirling numbers of the second kind. We derive expressions for these numbers as finite sums that involve the Stirling numbers of the second kind.
Reference graph
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Reviewed August 5, 2026 · model on record in the stance chip above.
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