We studied pairing mechanism of the heavily electron doped FeSe (HEDIS) systems, which commonly have one incipient hole band -- a band top below the Fermi level by a finite energy distance $epsilon_b$ -- at $Gamma$ point and ordinary electron bands at $M$ points in Brillouin zone (BZ). We found that the system allows two degenerate superconducting solutions with the exactly same $T_c$ in clean limit: the incipient $s^{pm}_{he}$-gap ($Delta_h^{-} eq 0$, $Delta_e^{+} eq 0$) and $s_{ee}^{++}$-gap ($Delta_h =0$, $Delta_e^{+} eq 0$) solutions with different pairing cutoffs, $Lambda_{sf}$ (spin fluctuation energy) and $epsilon_b$, respectively. The $s_{ee}^{++}$-gap solution, in which the system dynamically renormalizes the original pairing cutoff $Lambda_{sf}$ to $Lambda_{phys}=epsilon_b$ ($< Lambda_{sf}$), therefore actively eliminates the incipient hole band from forming Cooper pairs, but without loss of $T_c$, becomes immune to the impurity pair-breaking. As a result, the HEDIS systems, by dynamically tuning the pairing cutoff and selecting the $s_{ee}^{++}$-pairing state, can always achieve the maximum $T_c$ -- the $T_c$ of the degenerate $s^{pm}_{he}$ solution in the ideal clean limit -- latent in the original pairing interactions, even in dirty limit.
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