Let $(c_n)$ be a sequence of positive numbers converging to $1$ as $n\to\infty$. That is, $c_n > 0$ for every $n$ and $\lim\limits_{n\to\infty}c_n=1$. Let $g_1=-c_1$ and define, for $n \geq 1$,$$g_{n+1}=\frac{-1}{c_n-g_n}.$$
Question: Does $\lim\limits_{n \to \infty} g_n$ exist?
Notice that in case $g_n$ converges to, say $g_\infty$, the limit is given by the negative root of the quadratic equation determined by the equation $g_\infty = \dfrac{-1}{1-g_{\infty}}$.
Notice also that each $g_{n+1}$ can be represented as the following finite continued fraction $$g_{n+1}=-\cfrac{1}{c_n+\cfrac{1}{c_{n-1}+\cfrac{1}{\ddots+\cfrac{1}{c_1-g_1}}}},$$ the shorthand for which is sometimes given by the notation $g_{n+1}=[c_n,c_{n-1},\cdots, c_1-g_1]$.
The question is: Does $\lim\limits_{n \to \infty} g_n$ exist?
Proof: On the one hand, since $\varlimsup\limits_{n → ∞} v_n = v$, there exists a subsequence $\{v_{n_k}\}$ such that $\lim\limits_{n → ∞} v_{n_k} = v$, then$$ \varliminf_{n → ∞} \frac{u_n}{v_n} = \lim_{m → ∞} \inf_{n \geqslant m} \frac{u_n}{v_n} \leqslant \lim_{m → ∞} \inf_{k \geqslant m} \frac{u_{n_k}}{v_{n_k}} = \varliminf_{k → ∞} \frac{u_{n_k}}{v_{n_k}} = \lim_{k → ∞} \frac{u_{n_k}}{v_{n_k}} = \frac{u}{v}. $$ On the other hand, for any $0 < ε < 1$, there exists $N \geqslant 1$ such that $u_n > (1 - ε)u$ for $n \geqslant N$. Thus for $m \geqslant N$,$$ \inf_{n \geqslant m} \frac{u_n}{v_n} \geqslant \inf_{n \geqslant m} \frac{(1 - ε)u}{v_n} = \frac{(1 - ε)u}{\sup\limits_{n \geqslant m} v_n}, $$ which implies$$ \varliminf_{n → ∞} \frac{u_n}{v_n} = \lim_{m → ∞} \inf_{n \geqslant m} \frac{u_n}{v_n} \geqslant (1 - ε)u \lim_{m → ∞} \frac{1}{\sup\limits_{n \geqslant m} v_n} = \frac{(1 - ε)u}{\lim\limits_{m → ∞} \sup\limits_{n \geqslant m} v_n} = (1 - ε) \frac{u}{v}, $$ and making $ε → 0^+$ yields $\varliminf\limits_{n → ∞} \dfrac{u_n}{v_n} \geqslant \dfrac{u}{v}$. Therefore, $\varliminf\limits_{n → ∞} \dfrac{u_n}{v_n} = \dfrac{u}{v}$.
Now return to the question. Define $a_n = -g_n$, then $a_{n + 1} = \dfrac{1}{a_n + c_n}$ and $a_1 = c_1$. In fact, a more general proposition can be proved.
Proof: First, it is easy to see that $a_n > 0$ for each $n$. Since there exists $N \geqslant 1$ such that$$ \frac{b}{2} < b_n < 2b, \quad \frac{c}{2} < c_n < 2c, \quad \forall n > N $$ then for $n > N$,$$ a_n < \frac{b_n}{c_n} < \frac{4b}{c} \Longrightarrow a_n > \frac{b_n}{\dfrac{4b}{c} + c_n} > \frac{b}{\dfrac{8b}{c} + 4c}, $$ which implies that$$ l := \varliminf_{n → ∞} a_n \geqslant \frac{b}{\dfrac{8b}{c} + 4c} > 0, \quad L := \varlimsup_{n → ∞} a_n \leqslant \frac{4b}{c} < +∞. $$
Now, making $n → ∞$ in $a_{n + 1} = \dfrac{b_n}{a_n + c_n}$ yields$$ l = \varliminf_{n → ∞} a_{n + 1} = \frac{\lim\limits_{n → ∞} b_n}{\varlimsup\limits_{n → ∞} a_n + \lim\limits_{n → ∞} c_n} = \frac{b}{L + c}, $$ and analogously $L = \dfrac{b}{l + c}$, thus$$ l = \frac{b}{c + \dfrac{b}{c + l}} \Longrightarrow l^2 + cl - b = 0 \Longrightarrow l = \frac{1}{2} (-c + \sqrt{c^2 + 4b}), $$ and analogously$$ L^2 + cL - b = 0 \Longrightarrow L = \frac{1}{2} (-c + \sqrt{c^2 + 4b}). $$ Therefore, $l = L$, which implies that $\lim\limits_{n → ∞} a_n$ exists and is finite.