“…In addition, as indicated in previous studies, the discharge with many thin filaments or micro-discharges can transfer to a glow discharge in APDBD plasmas provided that there are enough seed electrons to turn on the discharge under a low electric field [1,2]. Based on the preceding discussions, if we define the gas which can be ignited directly to form the RF APGD plasma as the plasma-inducing gas, e.g., helium or argon, while on the other hand, the gas which cannot be used to generate the RF APGD plasma directly at the present time, e.g., air, nitrogen, oxygen, etc., as the plasma-forming gas, in this paper, the induced gas discharge approach can be expressed as [33,34]: first, generating a glow discharge plasma operating in a a and/or c mode after breakdown with the plasma-inducing gas (e.g., helium or argon); second, transferring the discharge mode to the c mode (or a-c co-existing mode) if the plasma operates in a pure a mode after breakdown by increasing the RF power input; third, increasing the flow rate of the plasma-forming gas (e.g., air, nitrogen, oxygen, etc.) to generate the c mode discharge with the plasma-inducing-forming gas mixture; decreasing the plasma-inducing gas flow rate, and finally, a stable glow discharge plasma operating in the c mode is obtained when no plasma-inducing gas is added into the plasma-forming gas any more.…”