In "Sharp threshold phenomena in statistical physics", H. Duminil-Copin, Japanese J. of Math. 14, 2019, a sharp transition of a boolean function is defined as follows:
A sequence of increasing boolean functions $(\mathbf{f_n})$ undergoes a sharp threshold at $(p_n)$ if there exists a $(\delta_n)$ tending to 0 such that $f_n(p_n - \delta_n) \to 0$ and $f_n(p_n + \delta_n) \to 1$.
An example is $p_n = 1/n$, for the indicator $f=\mathbb{1}_{\text{giant component}}$ of the random graph.
What if I write $p_n = n^{-c}$, for $c<1$ and $c>1$, and consider this the threshold point for $\mathbb{1}_{\text{giant component}}$? Have I followed the correct definition of a sharp threshold above? That is, if I show that the limit of the indicator $\mathbb{1}_{\text{giant component}}$ is either 0 or 1 for $c<1$ or $c>1$, have completed an equivalent task to the above definition?
How are these two formulations (the adding $\delta_n$ method and the use of a power $c$) of the threshold related? Perhaps, I can write $f(n^{-c}) = f(n^{-1} ± \Delta_n(c))$, and find the corresponding sequence $(\Delta_n(c))$, and therefore show the two limits above are 0 or 1?