Published September 2016 | Version v1
Journal article

Electron density modulation in a pulsed dual-frequency (2/13.56 MHz) dual-antenna inductively coupled plasma discharge

  • 1. Plasma Research Laboratory, School of Physical Sciences, Dublin City University, Dublin 9 (Ireland)
  • 2. Department of Advanced Materials Science and Engineering, Sungkyunkwan University, Suwon, Gyeonggi-do 440-746 (Korea, Republic of)
  • 3. Department of Advanced Materials Science and Engineering, Sungkyunkwan University, Suwon, Gyeonggi-do 440-746, South Korea and SKKU Advanced Institute of Nanotechnology (SAINT), Sungkyunkwan University, Suwon, Gyeunggi-do 440-746 (Korea, Republic of)
  • 4. Plasma Research Laboratory, School of Physical Sciences, Dublin City University, Dublin 9, Ireland and Department of Advanced Materials Science and Engineering, Sungkyunkwan University, Suwon, Gyeonggi-do 440-746 (Korea, Republic of)

Description

The electron density, ne, modulation is measured experimentally using a resonance hairpin probe in a pulsed, dual-frequency (2/13.56 MHz), dual-antenna, inductively coupled plasma discharge produced in argon-C4F8 (90–10) gas mixtures. The 2 MHz power is pulsed at a frequency of 1 kHz, whereas 13.56 MHz power is applied in continuous wave mode. The discharge is operated at a range of conditions covering 3–50 mTorr, 100–600 W 13.56 MHz power level, 300–600 W 2 MHz peak power level, and duty ratio of 10%–90%. The experimental results reveal that the quasisteady state ne is greatly affected by the 2 MHz power levels and slightly affected by 13.56 MHz power levels. It is observed that the electron density increases by a factor of 2–2.5 on increasing 2 MHz power level from 300 to 600 W, whereas ne increases by only ∼20% for 13.56 MHz power levels of 100–600 W. The rise time and decay time constant of ne monotonically decrease with an increase in either 2 or 13.56 MHz power level. This effect is stronger at low values of 2 MHz power level. For all the operating conditions, it is observed that the ne overshoots at the beginning of the on-phase before relaxing to a quasisteady state value. The relative overshoot density (in percent) depends on 2 and 13.56 MHz power levels. On increasing gas pressure, the ne at first increases, reaching to a maximum value, and then decreases with a further increase in gas pressure. The decay time constant of ne increases monotonically with pressure, increasing rapidly up to 10 mTorr gas pressure and at a slower rate of rise to 50 mTorr. At a fixed 2/13.56 MHz power level and 10 mTorr gas pressure, the quasisteady state ne shows maximum for 30%–40% duty ratio and decreases with a further increase in duty ratio.

Additional details

Identifiers

Publishing Information

Journal Title
Journal of Vacuum Science and Technology. A, Vacuum, Surfaces and Films
Journal Volume
34
Journal Issue
5
Journal Page Range
p. 051302-051302.9
ISSN
0734-2101
CODEN
JVTAD6

INIS

Country of Publication
United States
Country of Input or Organization
International Atomic Energy Agency (IAEA)
INIS RN
48037405
Subject category
S46: INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY;
Descriptors DEI
ANTENNAS; ARGON; AUGMENTATION; ELECTRON DENSITY; KHZ RANGE 01-100; MHZ RANGE; MIXTURES; MODULATION; PEAK LOAD; PLASMA; PULSE RISE TIME; PULSES
Descriptors DEC
DISPERSIONS; ELECTRICAL EQUIPMENT; ELEMENTS; EQUIPMENT; FLUIDS; FREQUENCY RANGE; GASES; KHZ RANGE; NONMETALS; RARE GASES; TIMING PROPERTIES

Optional Information

Notes
(c) 2016 American Vacuum Society