Optical and electrical characterization of pulse-modulated argon atmospheric-pressure inductively coupled microplasma jets
The critical parameters determining the generation of the pulse-modulated argon atmospheric-pressure inductively coupled plasma (AP-ICP) microjet were studied by varying the power, P , pulse-modulation frequency, f , and duty ratio, DR. The temporal changes in the net output power, P net , monitored...
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Veröffentlicht in: | Journal of applied physics 2010-10, Vol.108 (8), p.083302-083302-5 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | The critical parameters determining the generation of the pulse-modulated argon atmospheric-pressure inductively coupled plasma (AP-ICP) microjet were studied by varying the power,
P
, pulse-modulation frequency,
f
, and duty ratio, DR. The temporal changes in the net output power,
P
net
, monitored between the very high frequency power supply and matching network by an rf sampler, and
ArI
4
s
′
[
1
/
2
]
1
O
-
4
p
′
[
1
/
2
]
0
emission from the antenna were measured to elucidate the behavior of this plasma. The AP-ICP microjet, which produces high-density
(
0.9
-
1.1
×
10
15
cm
−
3
)
nonequilibrium plasma, consists of an alumina discharge tube with the inner diameter of 0.8 mm. The generation diagram of the pulse-modulated plasma was created by having
f
as the horizontal axis and DR as the vertical axis while varying
P
up to 50 W. At
f
≤
10
kHz
, the plasma was generated at above the linear lines of
f
and DR, which indicated the existence of the critical power-off period of approximately
80
μ
s
. At
f
>
10
kHz
, the pulse-modulated plasma was produced above constant DR and almost independent of
f
. The time-averaged power,
P
¯
, which is the product of
P
and DR, had to be more than 8-10 W to sustain the pulse-modulated plasma. From the measurement of the temporal changes in the net power and ArI emission, the dynamic behavior of the pulse-modulated plasma was revealed as follows. The prebreakdown period was present for
∼
5
μ
s
after the power was turned on. Once the plasma was generated, the impedance was changed and the reflected power gradually decreased. A strong emission peak was observed immediately after the breakdown, followed by the gradual increase up to the steady state. Finally, the intense afterpeak was observed at
0.8
μ
s
after the power was turned off. |
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ISSN: | 0021-8979 1089-7550 |
DOI: | 10.1063/1.3499272 |