First, a bit of background - Sylvester's sequence is defined recursively as $$e_{n+1}=\prod_{j=0}^{n-1}e_j=e_n^2-e_n+1, \space\space\space e_0=2$$ and, miraculously, there exists a number $E\approx 1.26$ that satisfies $$e_n=\lfloor E^{2^{n+1}}+1/2\rfloor$$ Wolfram gives a series representation for the constant $E$ (also called "Vardi's constant"), a proof of which I have been unable to find (or derive): $$E=\frac{\sqrt 6}{2}\exp\Bigg[\sum_{j=1}^\infty \frac{1}{2^{j+1}}\ln\bigg(1+\frac{1}{(2e_j-1)^2}\bigg)\Bigg]$$ or, reduced to a product, $$E=\frac{\sqrt 6}{2}\prod_{j=1}^\infty \bigg(1+\frac{1}{(2e_j-1)^2}\bigg)^{2^{-j-1}}$$ Reduced further, this is equal to $$E=\frac{\sqrt 6}{2}\prod_{j=1}^\infty \bigg(\frac{4e_{j+1}-4}{4e_{j+1}-3}\bigg)^{2^{-j-1}}$$ How might one derive this property? I haven't been able to make much progress with its derivation.
2026-03-29 16:20:16.1774801216
Sylvester's sequence - series representation of Vardi's constant
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The difference is that the exponent of my generating function based on the constant $L$ is $2^{n}$ instead of $2^{n+1}$, as in the case of Vardi's $E$.
$$(e_n-1)^2 \lt e_{n+1} \lt e_n^2$$
for Sylvester's sequence:
$2, 3, 7, 43, 1807, 3263443, 10650056950807, 113423713055421844361000443, \dots$
(sequence A000058 in the OEIS).
e.g.
$$(e_0-1)^2 = (2-1)^2=1 \lt e_1=3 \lt e_0^2 = 2^2=4$$
$$(e_1-1)^2 = (3-1)^2=4 \lt e_2=7 \lt e_1^2 = 3^2=9$$
$$(e_2-1)^2 = (7-1)^2=36 \lt e_3=43 \lt e_2^2 = 7^2=49$$
$$\cdots$$
$$L_0={e_0^{\frac{1}{2^0}}}$$
$$L_1={e_1^{\frac{1}{2^1}}}$$
$$L_2={e_2^{\frac{1}{2^2}}}$$
$$\cdots$$
$$L_5={e_5^{\frac{1}{2^5}}}=1.597910225682488561085083110$$
Where $L$ will be: $$\lim_{n \to \infty} L_n \ .$$ As in the case of the classical results of Mills, we do no know if it is a rational number or whether a closed-form formula could be obtained.
So you will require more precision as $n$ grows higher. With $L_5$ we will be able to calculate accurately $\{e_0,e_1,e_2,e_3,e_4,e_5\}$
The generating function initially would be as follows (it will require a correction I will explain later):
$$e_n = \lfloor L^{2^n} \rfloor$$
e.g. (still without correction):
$$e_5 = \lfloor L^{2^5} \rfloor = 3263443$$
$$e_4 = \lfloor L^{2^4} \rfloor = \color{red}{1806}$$
$$e_3 = \lfloor L^{2^3} \rfloor = \color{red}{42}$$
$$e_2 = \lfloor L^{2^2} \rfloor = \color{red}{6}$$
$$e_1 = \lfloor L^{2^1} \rfloor = \color{red}{2}$$
$$e_0 = \lfloor L^{2^0} \rfloor = \color{red}{1}$$
As you can observe still $e_0 \dots e_4$ are not accurate, but if we add $1/2$ the correction is good enough to make the result of the floor function match the sequence (as you can see the same correction is done in the OP's generating function for Vardi's constant $E$).
$$e_n=\lfloor L^{2^{n}}+1/2\rfloor$$
And now:
$$e_5 = \lfloor L^{2^5} +1/2\rfloor = 3263443$$
$$e_4 = \lfloor L^{2^4} +1/2 \rfloor = 1807$$
$$e_3 = \lfloor L^{2^3} +1/2 \rfloor = 43$$
$$e_2 = \lfloor L^{2^2} +1/2 \rfloor = 7$$
$$e_1 = \lfloor L^{2^11/2} +1/2 \rfloor = 3$$
$$e_0 = \lfloor L^{2^0} +1/2 \rfloor = 2$$
My guess is that the correction is required because, due to the properties of the sequence, we are embedding the sequence into quadratics intervals $(e_n-1)^2 \lt e_{n+1} \lt e_n^2$ instead of intervals of the shape $e_n^2 \lt e_{n+1} \lt (e_n+1)^2$ (which is the same case as Mills' constant but for intervals based on powers of three instead of powers of two. In the case of Mills' constant the correction is not required). I know this point do require a formal explanation but I would dare to say that it is related with the definition of the quadratic intervals.
This is basically an overview and lacks a lot of details, but the point is that due to the characteristics of the sequence we can bound it into quadratic intervals. Due to this, there is a monotone increasing sequence that we can embed into a constant, such that a quadratic exponent applied to it (plus the floor function corrected by $+1/2$) is able to recover the embedded sequence. So I think it is safe to say that this has been done by Vardi as well in a similar way. About the calculations of Wolfram, I think they are done by Wolfram's engine backwards, once you have defined properly the generating function and the constant. It can be seen that the precision of $E$ depends on the iteration $e_n$ so as $n$ grows higher we need more precision of $E$ (and same for my example $L$) to recover accurately the element $e_n$ of the sequence.