64th Annual Gaseous Electronics Conference
Volume 56, Number 15
Monday–Friday, November 14–18, 2011;
Salt Lake City, Utah
Session SF2: Microdischarges II
8:00 AM–9:00 AM,
Friday, November 18, 2011
Room: 255E
Chair: Steve Adams, AFRL
Abstract ID: BAPS.2011.GEC.SF2.2
Abstract: SF2.00002 : Spatially-resolved diagnostics of 1-GHz microdischarges*
8:30 AM–9:00 AM
Preview Abstract
Abstract
Author:
Jeffrey Hopwood
(Tufts University)
This talk addresses the internal structure of atmospheric pressure
microdischarges powered in the $f \sim $ 1 GHz frequency regime.
Microwave
power is focused into a sub-millimeter discharge gap using a
resonating
microstrip transmission line. The advantages of microwave
excitation over
low frequency operation include low power and discharge voltage
($<$1W, $<$
100 V), no ion sputtering ($f$ $>$ $f_{pi})$, and stable
steady-state cold plasma
generation.
Metastable argon density and the gas temperature were estimated
by the
optical absorption transition in Ar (1s$_{5}$-2p$_{8})$ at 801.4
nm using a
laser diode focused to $\sim $30 microns. The gas temperature was
estimated
from the Ar line broadening due to collisions. Able inversion of the
line-integrated density shows that the 200-micron wide central
core of the
microplasma is depleted of metastable atoms. Spatially-resolved
continuum
optical emission from electron recombination, however, shows that
the
microdischarge has a dense electron core.
Gas temperatures are difficult to accurately extract from optical
diagnostics due to the extreme depletion of commonly-used
spectroscopic
species from the microdischarge's central core (e.g., N$_{2}$,
OH\c{ }
Ar$^{m})$. In the case of the argon metastable line broadening,
the higher
density of Ar$^{m}$ in the peripheral regions masks the line
width within
the core. Numerical modeling interpolates the microplasma's core
temperature
based on measurements around the periphery. The model shows that
the core
temperature exceeds 1600 K, even though spatially-averaged nitrogen
rotational spectra suggest that the gas temperature is typically
only 400 K.
Diagnostics are important to the successful development of
microplasma
applications. The presentation concludes with an example of
low-temperature
microplasma deposition using acetylene at 1 atm, and a discussion
of scaling
single microplasmas to long linear arrays that are appropriate for
roll-to-roll plasma processing at atmospheric pressure.
*Supported by Department of Energy grant DE-SC0001923 and NSF-0755761
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2011.GEC.SF2.2