“…198 On the other hand, Falicov and Stachowiak 199 have shown that the dHvA effect can still be satisfactorily described by considering quasiclassical electron wave packets that move on all possible closed orbits, that is, return back to a starting point using all possible paths in the MB network. In this approach, the initial wave of unit amplitude entering a MB junction is separated into a transmitted wave with amplitude υ and a reflected wave with amplitude ξ, such that 200,201 The conservation of particles leads to the phase difference of π/2 between the transmitted and reflected waves. While the absolute phases are not defined, it is conventionally assumed [199][200][201] that the reflected phase preserves the initial phase and the transmitted one changes by π/2.…”