Is the following limit finite …?

Suppose that the sequence is a Newton–Raphson method for calculating numerically the zeroes of a function. What would that function look like then? $$ x_{n+1}=x_{n}-{\frac {f(x_{n})}{f'(x_{n})}} \quad \Longleftrightarrow \quad a_{n+1}=a_n+\frac{1}{a_n} $$ Identify $\,a_n = x_n\,$ in the first place, and solve for the function: $$ \frac{f'(x)}{f(x)} = -x \quad \Longleftrightarrow \quad f(x) = C\,e^{-x^2/2} $$ Interpretation: the sequence is a Newton–Raphson iterative method : for finding the zeroes of a Gaussian. However, it is clear from the start that the numerical calculations are not going to find those zeroes, for the simple reason that there aren't any.

But suppose that we modify the problem a bit, as follows: find the zeroes of $\;f(x) = e^{-x^2/2} - e^{-N}\;$ with $N$ some large positive integer, then we have instead the sequence: $$ x_{n+1}=x_{n}+\frac{1}{x_n}\left[1-\frac{e^{-N}}{e^{-x_n^2/2}}\right] $$ And now the iterations stop when: $$ x_{n+1} = x_n \quad \Longleftrightarrow \quad e^{-x_n^2/2} = e^{-N} \quad \Longleftrightarrow \quad x_n = \sqrt{2N} $$ Here is a little (Delphi Pascal) program that does the job:

program Diego;
procedure main(N : integer); var x,y : double; t : integer; begin Writeln('sqrt(2N) =',sqrt(2\*N)); x := 1; y := 0; t := 0; Writeln(t:4,' : x =',x); while not (y=x) do begin y := x; t := t + 1; x := x + 1/x\*(1-exp(-N)/exp(-sqr(x)/2)); Writeln(t:4,' : x =',x); end; end;
begin main(8); end.
Output:
sqrt(2N) = 4.00000000000000E+0000
   0 : x = 1.00000000000000E+0000
   1 : x = 1.99944691562985E+0000
   2 : x = 2.49834687643857E+0000
   3 : x = 2.89556809260418E+0000
   4 : x = 3.23325795454623E+0000
   5 : x = 3.52322153181656E+0000
   6 : x = 3.75982762597611E+0000
   7 : x = 3.92105171808397E+0000
   8 : x = 3.98953172402065E+0000
   9 : x = 3.99979758749457E+0000
  10 : x = 3.99999992320208E+0000
  11 : x = 3.99999999999999E+0000
  12 : x = 4.00000000000000E+0000
  13 : x = 4.00000000000000E+0000
So far so good. Now, what will happen if the value of $N$ is increased indefinitely? Then the sequence will become longer and longer; in the end it will never stop. Moreover, the following will be true: $$ \lim_{N\to\infty} e^{-N} = 0 \quad \Longrightarrow \quad x_{n+1}=x_{n}+\frac{1}{x_n} $$ It is clearly seen, however, that the number of iterations in the finite case ($n = 13$) does not equal $N = 8$ . So I doubt if the conjectured limit is true. Still apart from the fact that subtraction of two (infinitely) large numbers is highly unstable numerically (i.e. "bad" limit).

Update. Further numerical experiments reveal that indeed our iterands $\,x_n\,$ as well as the OP's original $\,a_n\,$ are close to $\,\sqrt{2n}\,$ and the larger $\,n\,$ the better, it seems. Here is an example, with $\,\sqrt{2\times 8192} = 128$ :

8188 : x = 1.27991318734407E+0002 , a = 1.27993080007178E+0002
8189 : x = 1.27996559906482E+0002 , a = 1.28000892929564E+0002
8190 : x = 1.27999342587009E+0002 , a = 1.28008705375065E+0002
8191 : x = 1.27999973101217E+0002 , a = 1.28016517343767E+0002
8192 : x = 1.27999999953749E+0002 , a = 1.28024328835758E+0002 <==
8193 : x = 1.27999999999999E+0002 , a = 1.28032139851126E+0002
8194 : x = 1.28000000000000E+0002 , a = 1.28039950389958E+0002
8195 : x = 1.28000000000000E+0002 , a = 1.28047760452340E+0002
So it may be conjectured that for all $\,n$ : $$ x_n < \sqrt{2n} < a_n $$ With: $$ x_{n+1} = x_n + \frac{1}{x_n}\left[1 - \frac{e^{-n}}{e^{-x_n^2/2}}\right] \quad ; \quad a_{n+1} = a_n + \frac{1}{a_n} $$ I have not (yet) been able to prove that this conjecture is true.
Quick and dirty proof.
Assume for a moment that the sequence $\,a_n\,$ is a continuous and differentiable function $\,a(n)\,$ of $\,n\,$ as is suggested in the picture below.

Then consider the following sequence. Fasten your seatbelts! $$ a_{n+1} = a_n + \frac{1}{a_n} \\ \frac{a_{n+1} - a_n}{1} = \frac{1}{a_n} \\ \frac{a(n+dn) - a(n)}{dn} = \frac{1}{a(n)} \\ a'(n)\,a(n) = 1 \\ \frac{da^2(n)}{dn} = 2 \\ a^2(n) = 2n+C $$ [Scaling argument deleted. I see no way to get it consistent, let it be rigorous. See edits of this post] Now we would like to have $\,C=0$ ; and fortunately there is a boundary condition, for $\,n=2$ , that fits the bill : $\,C = a_2^2 - 2\cdot 2 = 0$ . So: $\;a_n = \sqrt{2n}$ .
The larger $n$ , the better all of the approximations. A much neater way to express the end-result is: $$ \large \boxed{\lim_{n\to\infty} \frac{a_n}{\sqrt{2n}} = 1} $$ BONUS. Lemma: $$ a_{n+1} = a_n + \frac{1}{a_n} \quad \Longrightarrow \quad a_{n-1}^2 - a_na_{n-1} + 1 = 0 \quad \Longrightarrow \quad a_{n-1} = \frac{a_n}{2} + \sqrt{\left(\frac{a_n}{2}\right)^2-1} $$ Now compute (the discretization of) the second derivative, assuming again that $\,a_n\,$ is large: $$ a''(n) = a_{n+1} - 2a_n + a_{n-1} = a_n + \frac{1}{a_n} - 2a_n + \frac{a_n}{2} + \frac{a_n}{2}\sqrt{1-\frac{1}{(a_n/2)^2}} \approx \\ \frac{1}{a_n} - \frac{a_n}{2} + \frac{a_n}{2} \left[1-\frac{1}{2}\frac{1}{(a_n/2)^2} - \frac{1}{8}\left(\frac{1}{(a_n/2)^2}\right)^2\right] = -\frac{1}{a_n^3} $$ Which means that the discrete function $\,a_n\,$ for large $\,n\,$ is actually very smooth , when seen as a continuous and differentiable $\,a(n)$ . This is an even stronger motivation for the above treatment.
It is noticed that the "true" derivatives exhibit the same structure as the discretizations: $$ \left(\sqrt{2x}\right)'' = \left(\frac{1}{\sqrt{2x}}\right)' = -\frac{1}{\left(\sqrt{2x}\right)^3} $$ There are no coincidences in mathematics.