Ballistic Transmission of the Relativistic Quasielectrons …
165
Fig. 5 T vs. φ plot for the overbarrier passage of the quasielectrons; D = 8; E = 5; U = 1; β = 0.5
Fig. 6 The dependence of the transmission coefficient T on the quasielectron energy E for the
parameters: U = 4; φ = 1; β = 0.5; D = 1
In this dependence, it is particularly noteworthy that it has a pronounced tunneling
resonance character. This indicates that the structure considered in this paper is
a tunneling resonance structure. Most of the resonance peaks shown correspond
to Fabry–Perot resonances. Their energy position can be found from the above
expressions and is determined by formula (8).
The energy values for the Fabry–Perot resonances depend significantly on the
relation between the parameters U, D, and β, but do not depend on the parameter α.
165
Fig. 5 T vs. φ plot for the overbarrier passage of the quasielectrons; D = 8; E = 5; U = 1; β = 0.5
Fig. 6 The dependence of the transmission coefficient T on the quasielectron energy E for the
parameters: U = 4; φ = 1; β = 0.5; D = 1
In this dependence, it is particularly noteworthy that it has a pronounced tunneling
resonance character. This indicates that the structure considered in this paper is
a tunneling resonance structure. Most of the resonance peaks shown correspond
to Fabry–Perot resonances. Their energy position can be found from the above
expressions and is determined by formula (8).
The energy values for the Fabry–Perot resonances depend significantly on the
relation between the parameters U, D, and β, but do not depend on the parameter α.