“…J t can be stated or supposed surely that the type A is initiated and maintained if the breakdown occurs cold (dielectric) and cathode initiated a t ignition voltages > 400 V, that means without long-time heating (for instance > 0.1 psec) caused by prebreakdown currents, preceding niolten bridge stages (in contact breaking), gap bridging or contribution of anode processes [3,4,9,10,19,20,21,23,25], the wave impedance coupling between the current constriction of the microspot, the electrode parasitic circuit and the connected cables allows to exceed rapidly (< 1 nsec) the niininium arc current (see next sections), tiny ( N 30 nm) fieldeiiiitten or fiuldeinission sites are present on the cathode surface in a disperse spreading (for instance favoured by polished and cleaned surfaces, grain hori ndaries with gas contaiiiinat ions, oxide filn i i nhoniogeneit ies, segregation of wrt a i n alloying rrdiiiixtures and of hulk gases within tiny siirface sites [l-16, [19][20][21][22][23][24][25][26][27]), the external existence conditions of the discharge enforce a rapid directed or tindirected nioveiiient of the cathode root on a cold surface (for instance transverse magnetic field, nanocseond arc durations, low gas presiiires, micrometer gap widths,-one electrode moved) [l-271 and finally inlioiiiogeneities of the surface in a large area scale (coarse roughness) 2 2 p i are not present (for instance iiiacroscopic molten particles froiii preceding iiioltrn bridges or arc stages, dispersion of the electrode inaterial). Referring to point 1. i t iiiust be conipleted that in "vacuiini" [14] and for extreiiiely stiiall electrode distances in air [4,9,10] after a molten bridge ruptrire (contact breaking) a radial spot expansion and spot division from the contracted tvpe B to the disperse type A can occur after the spot has remained on the ignition site for a certain time.…”