Chemistry Reference
In-Depth Information
At φ
=
π and for H
1 it follows for the ion sheath voltage
ϕ s
k B ·
e
·¯
9
32 ·
ϕ sh =−¯
ϕ s
T e =
π 2
·
H 2
(3.258)
and for the sheath thickness
s max
s eff =
5
12 ·
z
=
s max
π
·
H
(3.259)
respectively.
Finally, we obtain with the Bohm current density an expression similar to the
Child-Langmuir law
2
1 / 2
e
m +
·
ϕ 3 / 2
s
s max
¯
j + =
e
·
n 0 ·
v Bohm =
C + ·
ε 0 ·
·
(3.260)
w ith C + =
200
/
243 (in the DC Child-Langmuir law C + =
4
/
9) and s max =
50
s child .
In the case of collisional sheath a corresponding formula to (3.243) is derived [36]
/
27
·
2
1 / 2
λ 1 / 2
+
e
m +
·
ϕ 3 / 2
s
¯
·
j + =
e
·
n 0 ·
v Bohm
1.68
·
ε 0 ·
·
.
(3.261)
s 5 / 2
max
3.6.3.2 Strongly Asymmetric Capacitively Coupled RF Plasma
In a capacitively coupled, unconfined, and for that reason asymmetrical RF discharge,
a negative self-bias voltage
appears at the powered electrode which is little less
than half the peak-to-peak RF voltage
(
ϕ sb )
. Assuming capacitive sheath model
and strong asymmetry, the idealized potentials over the RF cycle is represented in
Figure 3.29.
(
ϕ pp )
ϕ RF (
t
) =−
ϕ SB +
ϕ 0 ·
sin
(
ω
·
t
)
,
(3.262)
1
2 · (
ϕ pl (
t
) =
ϕ sf +
ϕ SB +
ϕ 0 ) ·
[1
+
sin
(
ω
·
t
)
]
(3.263)
with
ϕ 0 .
The negative self-bias potential results from the fact that no net DC current
can flow over one RF cycle due to the capacitive coupling, and that the sur-
face ratio between the powered and grounded electrode is significantly different
(
|
ϕ SB |≤
1
/
2
·
ϕ pp =
.
The electrons can follow the alternating electric field and leads to a moving
electron edge which modulates the positive space charge region, the sheath potential,
and the thickness, see Figures 3.28 and 3.29. Increasing RF voltage amplitudes mainly
affect the self-bias voltage and sheath properties at the powered electrode. It has only
little influence on the plasma potential in strongly asymmetric RF discharges. As the
result, the self-bias voltage at the powered electrode increases with the applied RF
A rf
A grounded )
 
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