Prove series identity (Alternating reciprocal factorial sum)

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Discussion Overview

The discussion revolves around proving an identity involving an alternating series of reciprocal factorials. Participants explore various methods to establish the validity of the series identity, which connects to concepts in probability distributions, specifically the Gamma and Poisson distributions. The scope includes mathematical reasoning and combinatorial identities.

Discussion Character

  • Exploratory
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant presents an alternating series identity involving reciprocal factorials and seeks insights on proving it, noting its connection to the Gamma and Poisson distributions.
  • Another participant suggests using induction, proposing a two-step induction process on both k and n, starting with base cases.
  • A different participant transforms the equation to a summation involving binomial coefficients, suggesting this transformation might aid in the proof.
  • One participant expresses difficulty with the induction approach but finds the transformation promising and considers using properties of combinations to telescope the left-hand side of the equation.
  • A participant sketches a proof based on previous insights, manipulating the series and applying the relationship between binomial coefficients to show how terms cancel, leading to a telescoping effect.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the best approach to prove the identity, with multiple methods and perspectives being explored without resolution.

Contextual Notes

Some participants mention the need for additional base cases in the induction proof, indicating that the proof's requirements may depend on the specific steps taken. The discussion also highlights the complexity of the series and the transformations involved.

uart
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This alternating series indentity with ascending and descending reciprocal factorials has me stumped.
\frac{1}{k! \, n!} + \frac{-1}{(k+1)! \, (n-1)!} + \frac{1}{(k+2)! \, (n-2)!} \cdots \frac{(-1)^n}{(k+n)! \, (0)!} = \frac{1}{(k-1)! \, n! \, (k+n)}
Or more compactly,
\sum_{r=0}^{n} ( \frac{(-1)^r}{(k+r)! \, (n-r)!} ) = \frac{1}{(k-1)! \, n! \, (k+n)}

BTW. (Assume n,k integers, with n \ge 0 and k \ge 1.)

In this particular instance (for me), this series arises from a connection between the Gamma (Erlang) distribution and the Poisson distribution, where for certain parameters they represent the same probability scenario.
Specifically 1 - poisson\_cdf(k-1,\lambda) = gamma\_cdf(x,k,\lambda) at x=1. I know this is true, but if I try to prove it by doing a series expansion of each of those CDFs and equating coefficients, then I end up with the alternating series that has me stumped.

Has anyone seen that series before or know of any insights in how best to prove it?
 
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Identities of that kind often yield to induction. In this case you'd need two inductions, one on k and one on n.
I'd take the base case of k=1, n=0 and observe the identity's truth for that - both sides equalling 1.
Then I'd try proving that if the identity holds for k=k', n=n' then it holds for k=k',n=n'+1 and also for k=k'+1,n=n'. The result would follow by induction.

Sometimes the nature of the induction step proof requires us to have already proven more than one base case, eg not only k=1,n=0 but also k=1,n=1 and k=1,n=2. But if such a requirement exists it will become apparent when trying to prove one or other of the induction steps. In that case, you'd need to prove the additional base cases to complete the proof.
 
Equation to be proved is transformed to
(-)^k\sum_{r=0}^n \ _{n+k}C_{r+k} (-)^{r+k}=\ _{n+k-1}C_n
Terms under summation are interpreted as coefficients of ##x^{n-r}## in expansion of ##(x-1)^{n+k}##. I hope such a transformation could be helpful.
 
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Thanks all. Yes I did try induction first up, but I didn't get anywhere with it.

That's a great approach anuttarasammyak, looks very promising.

And using the combinations property that,
_nC_r = \, _{n-1}C_r + \, _{n-1}C_{r-1}
with the end condition that _nC_0 = \, _{n-1}C_0, I'm pretty sure I can make that whole LHS "telescope".
 
Just sketching out a proof based on anuttarasammyak's insights.
\frac{1}{k! \, n!} + \frac{-1}{(k+1)! \, (n-1)!} + \frac{1}{(k+2)! \, (n-2)!} \cdots \frac{(-1)^n}{(k+n)! \, (0)!} = \frac{1}{(k-1)! \, n! \, (k+n)}
Multiplying both sides by (k+n)! puts the proposed identity into the following form.
_{n+k}C_n -\, _{n+k}C_{n-1} +\, _{n+k}C_{n-2} - \cdots (-1)^n \,\, _{n+k}C_{n-n}= \, _{n+k-1}C_n
Using the relationship that, \, _nC_k = \, _{n-1}C_k + \, _{n-1}C_{k-1} (for n,k >=1), the LSH can be written as,
[ _{n+k-1}C_n + \, _{n+k-1}C_{n-1}] - [ _{n+k-1}C_{n-1} + \, _{n+k-1}C_{n-2}] + \cdots (-1)^{n-1} [ _{n+k-1}C_1 + \, _{n+k-1}C_0] + (-1)^n [ _{n+k}C_0 ]
Here the second binomial coefficient in each square bracketed term cancels with the first binomial coeff in the following bracketed term, so the series telescopes leaving just the very first coeff of, \, _{n+k-1}C_n, hence LHS = RHS.
 
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