“…In the last decade, the study of non-extensivity in plasmas and plasma sheaths has attracted significant attention. [30][31][32][33][34] Assuming a non-extensively distributed population of electrons, Debye shielding, floating potential, and sheath thickness in a two component collisionless unmagnetized plasma sheath with cold ions, has been studied by Sharifian et al [30] Borgohain et al [31,32] have studied the behaviour of the sheath in an electronegative plasma with q-non-extensive electron distribution. The sheath structure in the presence of non-extensive electrons for a constant and variable dust charge have been respectively studied by Driouch et al [33] and El Ghani et al [34] Given the assumption that a super-extensive statistical distribution describes the highly energetic population of electrons, it is straightforward to think that such a population of electrons is more likely to produce secondary electrons emission from the wall, in the sheath region, and hence, a SEE process must be included in a sheath model for a complete study.…”