On the Quantum Capacitance of Quantum Wire Field-Effect …
89
(vi) The model of Palik et al.
The 1D electron statistics under the condition of unity Fermi function at low
temperatures can be written following [41] as
n s =
2g v
π
S
B 21
E
F , n x , n y
(12)
Using (1) and (12) the C g can be expressed as
C g =
2g v e
2
π
S(θ 6 )
1 +
2g v e
2
πC ins
S(θ 6 )
−1
(13)
where, θ 6 =
∂
∂ E
F
B 21
E
F , n x , n y
.
2.3 The C g in QWFET of II–VI Materials
The 1D electron statistics under the condition of unity Fermi function at low
temperatures can be written following [41] as
n s =
g v
π
√
B 0
S
t 7
E
F , n x , n y
(14)
Using (1) and (14) the C g can be expressed as
C g =
g v e
2
π
√
B 0
S(θ 7 )
1 +
g v e
2
C ins π
√
B 0
S(θ 7 )
−1
(15)
where, θ 7 =
∂
∂ E
F
t 7
E
F , n x , n y
.
2.4 The ¯
C G in QWFET of IV–VI Materials
The 1D electron statistics under the condition of unity Fermi function at low
temperatures can be written following [41] as
n s =
2g v
π
S
B 32
E
F , n x , n y
(16)
Using (1) and (16) the C g can be expressed as