-
F − mobility was calculated in the gas mixtures SF 6 –Xe, SF 6 –Ar and SF 6 –He from a Monte Carlo
code for ion transport simulation. The elastic momentum transfer cross sections were determined from
the semi-classical JWKB approximation while the inelastic ones (detachment and charge transfer) were
taken from the literature. The resulting collision cross section sets were validated from the good
agreement between the calculated F − mobilities in the individual gases and the measured ones.
Moreover, the longitudinal and transverse density normalized diffusion coefficients and the reaction
rate coefficients were calculated in these mixtures for the case where the share of SF 6 is 50%.
Finally, a comparison of our calculated F − mobilities in these mixtures obtained from the Monte
Carlo code and those obtained from linear Blanc's law showed good agreement in the case of SF 6 –Xe
at low field but strong disa...
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This paper presents the self-consistent modelling of argon micro-plasmas, produced by a microwave
source (2.45 GHz) at atmospheric pressure. The source is a microstrip-like transmission line, with a
50–200 µm final gap where the micro-plasmas are created. Simulations use a one-dimensional,
stationary code that solves the fluid-type transport equations for electrons, positive ions Ar + and
##IMG##
[ej.iop.org] {${\rm Ar}^+_2$} ,
and the electron mean energy; the rate balance equations for the main neutral species; Poisson's
equation for the space-charge electrostatic field; Maxwell's equations for the electromagnetic
excitation field; the gas energy balance equation for its temperature distribution; and the kinetic
electron Boltzmann equation considering several direct and stepwize electron collision processes.
The model uses a kinetic scheme that considers the atomic excited states Ar(4s) an...
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The formation and expansion dynamics of laser-produced plasmas was studied by means of the effect of
a second delayed laser pulse upon the ion kinetic energy of the plasma created by the first one. Two
types of measurements were carried out: ion kinetic energy distributions and overall ion time of
flight (t.o.f.). Ion energy distributions were obtained with an electrostatic energy analyser, which
allowed the observation of the energy distributions of each charge state separately while the ion
t.o.f. signal was measured with an ion probe. Laser power densities ranged from 2 × 10 8 to 2 × 10 9
W cm −2 with 532 nm photons, and studies were extended to Al, Cu and Co targets. The effects of the
second laser pulse on the plasma created by the first were very different depending on the
interpulse delay. At low delays (from 0 to 10 ns) the second pulse produced an increase of the
plasma average charge state and the maximum ion kinetic energy, while at higher...
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The influence of a small addition of argon (2–5%) on the parameters of a strongly non-uniform
microwave discharge (with the electrode microwave discharge as an example) in nitrogen at reduced
pressures was studied. Experiments showed that the small addition of Ar strongly affected the
discharge: it increased in size, and the power absorbed in the plasma and the emission intensities
of nitrogen bands reduced. A self-consistent 2D modeling of the discharge was carried out. The model
included the Maxwell, Poisson and Boltzmann equations and a set of balance equations for neutral
excited and charged plasma species. The processes involving vibrationally excited ground state
molecular nitrogen were taken into account by the well-known analytic expression for the vibrational
distribution of molecules in the diffusion approximation. The results of modeling and experiment
were in qualitative agreement. Additional information about the discharge allowed us to explain the
experimental resul...
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In this work, we compare measurements of electron density ( n e ), plasma potential ( ##IMG##
[ej.iop.org] {phiv} p ), electron temperature ( T e ), and electron
energy distribution function (EEDF or f ( E )) made with a dc biased RF probe and a Langmuir probe.
The measurements show good agreement between the two probes across an order of magnitude in plasma
density.
-
We have investigated the performance of a microwave-cavity discharge (MWD) operating in tandem with
a fast rise-time pulsed dielectric-barrier discharge (DBD). The tandem discharge operated in a
helium/oxygen mixture, where metastable molecular oxygen could be produced efficiently using MWD in
proportionally large quantities (order of 20% of total oxygen number density). In this new
arrangement, a DBD operating at high E / N provided a metastables-rich mixture, thereby modifying
the discharge kinetics of the MWD, which operated in the E / N range centered around 10 Td. Both
discharges operated in synchronized pulse-repetitive mode, which was tailored to maximize the oxygen
metastable production efficiency. The system operated at pressures up to 350 Torr with an average
power between 3 and 20 W.
-
Laser scattering provides a very direct method for measuring the local densities and temperatures
inside a plasma. We present new experimental results of laser scattering on an argon atmospheric
pressure microwave plasma jet operating in an air environment. The plasma is very small so a high
spatial resolution is required to study the effect of the penetration of air molecules into the
plasma. The scattering signal has three overlapping contributions: Rayleigh scattering from heavy
particles, Thomson scattering from free electrons and Raman scattering from molecules. The Rayleigh
scattering signal is filtered out optically with a triple grating spectrometer. The disentanglement
of the Thomson and Raman signals is done with a newly designed fitting method. With a single
measurement we determine profiles of the electron temperature, electron density, gas temperature,
partial air pressure and the N 2 /O 2 ratio, with a spatial resolution of 50 µm, and including ab...
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The experimental and calculated results of uniformity in a glow dielectric barrier discharge (DBD)
under sub-atmospheric pressures are reported. Driven by a square-wave power source, the discharge in
a parallel-electrode DBD system shows uniform or various lateral structures under different
conditions. There exists a critical frequency below which the DBD is uniform for almost all the
applied voltages. Above the critical frequency, a non-uniform (patterned) discharge is observed and
the patterned structures change with frequency and voltage. A two-dimensional fluid modeling is
performed on this DBD system which shows similar results in agreement with the experiments. The
simulations reveal that the distribution of the space electron density at the beginning of each
voltage pulse plays an important role in achieving the uniformity. Uniform space charge results in a
uniform DBD. The patterned DBD always evolves from the initial uniform state to the eventual
non-uniform one. During ...
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Dual frequency capacitively coupled plasmas (CCPs) are widely used in (large area) etching and
plasma enhanced chemical vapor deposition processes. However, applications in physical vapor
deposition (PVD) are still sparse due to the well-established dc magnetron cathode discharges.
Nevertheless, there exist critical applications such as ferromagnetic or ceramic thin film
deposition which are difficult to handle even for dc magnetron systems. For these materials systems
dual frequency CCPs pose a good alternative, because for insulators charging can be avoided and for
ferromagnetic materials the target thickness becomes independent of the magnetron configuration at
comparable deposition rates. In this work we investigate two separate subjects. First, in dual
frequency capacitive discharges a complex coupling of the applied excitation frequencies can be
observed, which from a plasma parameter point of view limits the separability of ion flux (usually
controlled by frequencies...
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Fireballs are luminous regions produced by double layers in front of positively biased electrodes in
plasmas. Although fireballs have been investigated previously there are a great variety of
unexplained nonlinear phenomena, some of which are addressed in this work. First, it is shown that a
fireball is not an isolated local phenomenon but an integral part of the entire discharge plasma.
Current closure and limits are discussed. Fireballs with currents from milliamperes to tens of
amperes are created depending on whether the electron source is temperature limited, space-charge
limited or limited by ion currents in afterglow plasmas. Fireballs are created with highly
transparent grids which allow electron transmission through the electrodes and optimize the
ionization efficiency. The physics of pulsating fireballs is investigated. Fireballs disrupt when
density outflow exceeds production, leading to density collapse and current disruption when the
electron drift exceeds the Bunema...
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The interplay of gas flow and depletion by plasma dissociation determines the spatial distribution
of species and the deposition uniformity in a plasma source. Many plasma reactors use a gas
showerhead and the design of the flow dynamics is a critical aspect of the reactor performance. In
this paper, plasma deposition is considered as chemically reacting gas flow in an ideal showerhead
reactor. The gas fluid flow is described by finite-gap stagnation-point creeping flow. The
distribution of neutral species across the electrode gap is determined by diffusion equations,
whereas their lateral transport is purely convective. Parameters relevant to large-area
radio-frequency plasma deposition are particularly suitable for a complete analytical solution of
the multi-component transport. A representative reaction scheme for hydrogen/silane plasma
deposition is used for an analytical example from first principles which shows good agreement with
numerical simulation. For a laterally unifo...
-
Plasmas generated inside oxygen bubbles in water have been developed for water purification.
Zero-dimensional numerical simulations were used to investigate the chemical reactions in plasmas
driven by dc voltage. The numerical and experimental results of the concentrations of hydrogen
peroxide and ozone in the solution were compared with a discharge current between 1 and 7 mA. Upon
increasing the water vapour concentration inside bubbles, we saw from the numerical results that the
concentration of hydrogen peroxide increased with discharge current, whereas the concentration of
ozone decreased. This finding agreed with the experimental results. With an increase in the
discharge current, the heat flux from the plasma to the solution increased, and a large amount of
water was probably vaporized into the bubbles.
-
When we form a structure of plasmas distributed in a certain space in which electromagnetic waves
propagate, such a plasma structure serves as a different medium from a homogeneous bulk plasma. We
can also enhance or generate novel functions of the plasmas when we add other structural materials
such as functional components. That is to say, when we estimate such a medium from the material
properties such as permittivity, permeability and conductivity, it shows extraordinary and/or
functional effects that arise from the synthesis of the structure. We call such an artificial
material a plasma metamaterial. In this review, starting from a fundamental understanding of
electromagnetic wave propagation in and around plasmas, we review the new functions of plasmas as
metamaterials, including a photonic-crystal-like behavior, a negative refractive index state and a
nonlinear bifurcated electric response, by describing specific plasma structures. In addition, we
survey some specific appli...
-
An atmospheric steam plasma jet generated by an original dc water plasma torch is investigated using
electrical and spectroscopic techniques. Because it directly uses the water used for cooling
electrodes as the plasma-forming gas, the water plasma torch has high thermal efficiency and a
compact structure. The operational features of the water plasma torch and the generation of the
steam plasma jet are analyzed based on the temporal evolution of voltage, current and steam pressure
in the arc chamber. The influence of the output characteristics of the power source, the fluctuation
of the arc and current intensity on the unsteadiness of the steam plasma jet is studied. The
restrike mode is identified as the fluctuation characteristic of the steam arc, which contributes
significantly to the instabilities of the steam plasma jet. In addition, the emission spectroscopic
technique is employed to diagnose the steam plasma. The axial distributions of plasma parameters in
the steam plasma...
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A radio-frequency (RF) helicon plasma reaction chamber (HPRC) is developed and used to decompose
methane gas into high-purity hydrogen gas and solid carbon in the form of graphite. A single-turn (
m = 0) helicon antenna, operated at 13.56 MHz, and a 100 G dipole magnetic field are used to excite
a helicon mode in a nonthermal plasma, creating plasma densities exceeding 10 13 cm −3 using
8–20 SCCM methane gas at up to 1300 W of RF power. The HPRC device takes advantage of a uniform
large amplitude electron sheath across the exit aperture. At this aperture, all of the incident
electron flux from the plasma is extracted and all ions are reflected back into the source. In this
way, only neutrals and electrons are allowed out of the reaction chamber, enhancing the breakdown of
methane into deposited carbon and hydrogen gas that escapes. A methane decomposition percentage of
99.99 ± 0.06% is demonstrated using 1300 W of RF power and a methane gas flow rate of ...
-
The velocity and energy distribution functions of ions escaping radially from the magnetic trap
region of a HiPIMS discharge have been measured using a retarding field analyzer (RFA). Spatially
and angularly resolved measurements recorded at a representative time show more energetic ions
detected along a line-of-sight coincident with an oncoming rotating ion fluid, which circulates
above the racetrack in the same direction as the electron E × B drift. The difference in the mean
ion energies between measurements made into and against the direction of rotation is ~5 eV.
Numerical solutions of the equation of motion for the ions accounting for azimuthal acceleration
(modified two-stream instability model used by Lundin et al ) have been found. The centripetal force
caused by the radial electric field and a drag force term accounting for ion collisions revealed
that only a small fraction (typically
-
A retarding field energy analyzer is used to characterize an asymmetric, 13.56 MHz driven,
capacitively coupled, parallel plate discharge operated at low pressure. The characterization is
carried out in argon discharges at 10 and 20 mTorr where the sheaths are assumed to be
collisionless. The analyzer is set in the powered electrode where the impacting ion and electron
energy distributions are measured for a range of discharge powers. A circuit model of the discharge
is used to infer important electrical parameters from the measured energy distributions, including
electrode excitation voltages, plasma potential and sheath potentials. Analytical models of the ion
energy distribution in a radio-frequency sheath are used to determine plasma parameters such as
sheath width, ion transit time, electron temperature and ion flux. A radio-frequency compensated
Langmuir probe is used for comparison with the retarding field analyzer measurements.
-
Posted: November 29th, 2011, 6:00pm MST
The PDF file provided contains web links to all articles in this volume.
-
There is an increasing concern that high power impulse magnetron sputtering (HiPIMS) systems are
being disadvantaged by relatively low deposition rates compared with traditional dc magnetrons
operating at the same average power input. Nevertheless, a minimization of the losses of ionized and
neutral species is possible in HiPIMS discharges. In the described magnetron configuration, the
majority of metal ions escaping the discharge volume can be either used for deposition or, if they
fail to reach the substrate, for discharge maintenance when charge redistribution from one
ionization area to the other takes place. The anode-to-cathode configuration allows the neutrals,
which are not deposited on the substrate, to be guided to the other instantaneous cathode and be
ionized or re-sputtered. For the same average power input, it becomes possible to increase the
self-sputtering efficiency, deposition rate and obtain a versatile control over the film
microstructure.
-
The far-field plume of a 1.5 kW Hall effect thruster is mapped with a Langmuir probe and an emissive
probe. Time-averaged measurements of the plasma potential, the electron temperature and the electron
number density are performed for different operating conditions of the thruster. The influence of
the discharge voltage, the cathode mass flow rate as well as the magnetic field strength is
investigated. The plasma potential decreases from 30 V at 300 mm on the thruster axis to 5 V at 660
mm and at 60°, the electron temperature decreases from 5 to 1.5 eV. The electron number density
drops from 3.5 × 10 16 to 1 × 10 15 m −3 in the far-field plume. The values of the plasma potential
and electron temperature measured with the Langmuir probe and the emissive probe are in good
agreement.
-
A low-frequency oscillation (
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A set of diagnostic methods to obtain the plasma parameters including power dissipation, gas
temperature and electron density is evaluated for an atmospheric pressure helium or argon radio
frequency (RF) plasma needle for biomedical applications operated in open air. The power density of
the plasma is more or less constant and equal to 1.3 × 10 9 W m −3 . Different methods are
investigated and evaluated to obtain the gas temperature. In this paper the gas temperatures
obtained by rotational spectra of OH( A – X ) and ##IMG##
[ej.iop.org] {{\rm N}_2^+} ( B – X ) are
compared with Rayleigh scattering measurements and measurements of the line broadening of hydrogen
and helium emission lines. The obtained gas temperature ranges from 300 to 650 K, depending on the
gas. The electron densities are estimated from the Stark broadening of the hydrogen α and β lines
which yi...
-
An atmospheric-pressure room-temperature plasma brush, which can deliver uniform surface treatment
effects, is reported. The plasma structure, which includes the negative glow, Faraday dark space and
positive column, is clearly visible to the naked eye. The width of the Faraday dark space diminishes
with decreasing gap distance and this phenomenon is different from that observed from low-pressure
glow discharge plasmas. High-speed photographs taken at an exposure time of 2.5 ns show that the
plasma propagates from the nozzle to the object in about 100 ns and 10 ns for gap distances of 6 mm
and 2 mm, respectively, and the results are consistent with electric measurements. The emission
spectra reveal N 2 ( B – A ) bands in addition to those of O, ##IMG##
[ej.iop.org] {{\rm N}_2^+} , N 2 ( C – B )
and He, indicating that the plasma source is reactive and suitable for a...
-
Low-power plasma generators with two kinds of hot anode/nozzle structures, one with a natural
radiation-cooled nozzle and the other with a regeneratively cooled nozzle, were designed to
investigate the dependence of the volt–ampere characteristics on the anode temperature. Pure argon,
nitrogen or hydrogen gas was used as the plasma working gas at input powers from 130 to 1200 W in a
plenum chamber kept at a pressure of below 20 Pa. Variations of the arc voltage with changes in arc
current, gas flow rate and firing time (anode temperature) were examined, and the effects of the arc
volt–ampere characteristics on the properties of the ejected plasma flow from the nozzle exit are
discussed with respect to the evaluation of the average plume temperature and flow velocity. Results
show that there are definitely non-negligible effects of anode temperature on these characteristics.
-
A time-dependent plasma discharge model has been developed for the ionization region in a high-power
impulse magnetron sputtering (HiPIMS) discharge. It provides a flexible modeling tool to explore,
e.g., the temporal variations of the ionized fractions of the working gas and the sputtered vapor,
the electron density and temperature, and the gas rarefaction and refill processes. A separation is
made between aspects that can be followed with a certain precision, based on known data, such as
excitation rates, sputtering and secondary emission yield, and aspects that need to be treated as
uncertain and defined by assumptions. The input parameters in the model can be changed to fit
different specific applications. Examples of such changes are the gas and target material, the
electric pulse forms of current and voltage, and the device geometry. A basic version, ionization
region model I, using a thermal electron population, singly charged ions, and ion losses by
isotropic diffusion is...
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For over 80 years emissive probes have been used to measure plasma potential and a wide variety of
methods for interpreting probe data now exists. Constructions, heating methods and measurement
techniques are reviewed in detail and their various strengths and limitations are compared.
Additionally, several novel uses for emissive probes, such as measuring electron temperature are
presented. This review also includes tables of recommendations for emissive probe design given the
type of plasma and desired measurements.
-
Low-temperature RF discharges have been widely used in processing applications. Plasma diagnostics
provide useful information about the plasma state which is important for processing results. In the
deposition process, as the dielectric material is coated onto the probe surface, electrical
diagnostic techniques using a dc current cannot be applied. Instead, an ac voltage is applicable for
measuring plasma parameters. In this paper, electron temperatures and plasma densities were measured
with an anodized aluminum probe using the floating-type harmonic method and the self-bias method.
The Al 2 O 3 layer on the probe surface and the sheath were modeled as a series connection of a
capacitor and a resistor, respectively. The applied ac voltage was divided into the two parts
depending on their impedances, and the voltage across the sheath was determined by the phase between
the voltage and the current. According to experimental results, the conventional harmonic met...
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Electron motion in a CF 4 magnetic neutral loop discharge (NLD) plasma was simulated using a Monte
Carlo method. The spatial distribution of electrons illustrated the fundamental structure of the NLD
plasma, and its dynamics were depicted from the distributions of the mean electron energy, the
electron energy gain and the azimuthal electron flux. The peak of mean electron energy appeared at
the neutral loop (NL), which confirmed that electrons gain energy near this loop. High mean electron
energy was observed not only near the NL but also along the separatrices of the quadrupole magnetic
field. Energetic electrons were transported along the separatrices and induced ionization at those
locations. However, the electron distribution had valleys along the separatrices, because electrons
accelerated near the NL were likely to leave this region where the binding of the magnetic field is
weak. The azimuthal electron flux representing the loop plasma current showed that the ele...
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Anode striations and wall charges, common phenomena in the plasma display panel (PDP) discharge
process, are investigated by simulations in both alternating current coplanar and novel shadow mask
PDPs. The formation process of striations is presented and the formation mechanism is investigated.
The results reveal that in both structures there is an obvious correspondence between the striation
distribution and both the negative and the positive charge accumulation on the dielectric layer
above the anode. Each of the two contributions to the total wall charge reaches its peak at the
positions where the striations emerge. The total wall charge distribution on the other hand, which
is the sum of the wall charge collected from electrons and ions, does not show any striation effect
at all.
-
Axial emission profiles in a parallel plate dc microdischarge (feedgas: argon; discharge gap d = 1
mm; pressure p = 10 Torr) were studied by means of time-resolved imaging with a fast ICCD camera.
Additionally, volt–ampere ( V – A ) characteristics were recorded and Ar* metastable densities were
measured by tunable diode laser absorption spectroscopy (TDLAS). Axial emission profiles in the
steady-state regime are similar to corresponding profiles in standard size discharges ( d ≈ 1 cm, p
≈ 1 Torr). For some discharge conditions relaxation oscillations are present when the microdischarge
switches periodically between the low current Townsend-like mode and the normal glow. At the same
time the axial emission profile shows transient behavior, starting with peak distribution at the
anode, which gradually moves toward the cathode during the normal glow. The development of argon
metastable densities highly correlates with the oscillating discharge c...
-
This work is devoted to the analysis of experimental results obtained in dry air at atmospheric
pressure in a positive point-to-plane corona discharge under a pulsed applied voltage in the cases
of anodic mono- and multi-tips. In the mono-tip case, the peak corona current is analysed as a
function of several experimental parameters such as magnitude, frequency and duration of pulsed
voltage and gap distance. The variation of the corona discharge current is correlated with the ozone
production. Then in the multi-tip case, the electrical behaviour is analysed as a function of the
distance between two contiguous tips and the tip number in order to highlight the region of creation
active species for the lowest dissipated power. Intensified charge-coupled device pictures and
electric field calculations as a function of inter-tip distance are performed to analyse the mutual
effect between two contiguous tips. The optical emission spectra are measured in the UV–visible–NIR
wavelength ra...
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This study evaluates the spatial expansion of barrier discharges (BDs) in oxygen, carbon dioxide,
synthetic air, and helium at atmospheric pressure. Despite being confined in narrow gas channels,
the BD plasma only partially covers the available discharge area at low applied voltages as was
experimentally observed. This is important for homogeneous surface treatment. The appearance of
local discharge zones in the plasma development results in a variation of the capacitive behaviour
of the equivalent electric circuit as a function of the applied voltage. This transient behaviour of
the apparent dielectric capacitance is therefore investigated for various discharge areas and
different gas compositions. Furthermore, a semi-empirical model describing the expansion behaviour
is proposed and validated by means of the obtained experimental data. The results clearly show that
a three times higher voltage excess is required for oxygen-containing gases compared with helium in
order to deve...
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Temporally resolved, spatially integrated measurements of the temperature of the plasma channel
formed by a hydrogen-filled discharge capillary waveguide are presented. Plasma temperatures of 4–7
eV are measured for peak discharge currents between 80 and 150 A. It is demonstrated that
laser-triggering the capillary discharge enables capillary discharges with a peak current as low as
23 A to be driven, reducing the plasma temperature to approximately 3 eV. This plasma temperature
meets the requirements of a recently proposed soft x-ray recombination laser.
-
Previous descriptions of the methods of radiation transport are generalized for two cases: small
(order of unity) absorption coefficient and large coefficient with inhomogeneous distribution of
absorbing atoms. Computation algorithms for the matrices equivalent to the integral operator of the
radiation transport are deduced. The methods described are planned for future description of excited
and resonance atoms in problems of self-consistent modeling of non-equilibrium plasmas of inert gas.
The solution of the transport equation is illustrated by model examples of atom density computation
typical for constricted discharge conditions and 'skin-effect' conditions with gas heating taken
into account.
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This review describes the experimental studies of contraction in neon, argon and helium, discussing
the basic regularities of the phenomenon. These studies, extended over a long time, are still
urgent. For pressures that are not too high a noticeable contraction of the plasma glow and a smooth
non-monotonic dependence of the degree of contraction on the current are observed. Above a critical
pressure the plasma immediately contracts into a bright thin cord, if the current reaches a critical
value. A hysteresis phenomenon is observed during the transition from the diffuse state to the
contracted state and vice versa. Experiments that show the secondary role of non-homogeneous gas
heating for contraction in neon and argon, and the main role for contraction in helium, are
described. Studies of the ionization waves (the strata), which propagate as pulses of the current
cord area, are reviewed showing the close relationship between contraction and stratification. The
roles of various ...
-
Combined experimental, numerical and analytical approaches are presented to address actual problems
of glow discharge physics. Such a synthesis is able to clarify relatively simple, qualitative,
self-consistent phenomena, and should allow improvement of the existing paradigms and/or formulation
of novel approaches. The following illustrative examples are discussed: * Linear and non-linear
diffusion in multispecies, currentless and current-carrying low-temperature plasmas. Both ambipolar
diffusion and ambipolar mobility are considered. * Non-local electron kinetics in radio frequency
and direct current glows. * Structures of the cathode and anode regions in direct current glows.
-
This paper presents the measured values of the total dissociative recombination coefficient of
molecular ##IMG##
[ej.iop.org] {{\rm
Ar}_2^+} ions with electrons ##IMG##
[ej.iop.org] {\alpha({\rm Ar}_2^+)} as a
function of both electron and gas temperatures. The measured recombination coefficient can be
expressed as ##IMG##
[ej.iop.org] {\[
\begin{equation*} \alpha _{{\rm Ar}_2^+ } (T_{\rm e} ,T_{{\rm gas}})=(8.1\pm 0.5)\times
10^{-7}(T_{\rm e} /300\,{\rm K})^{-0.64}(T_{{\rm gas}} /300\,{\rm K})^{-0.86}\,{\rm cm}^3\,{\rm
s}^{-1} \end{equation*} \]} in the temperature ranges 300 K ≤ T e ≤ 10 400 K and 300 K ≤ T gas ≤ 500
K.
-
A review of work centered on the utilization of multi-dimensional optical diagnostics to study
phenomena arising in radiofrequency plasma discharges is given. The diagnostics range from passive
techniques such as optical emission to more active techniques utilizing nanosecond lasers capable of
both high temporal and spatial resolution. In this review, emphasis is placed on observations that
would have been more difficult, if not impossible, to make without the use of such diagnostic
techniques. Examples include the sheath structure around an electrode consisting of two different
metals, double layers that arise in magnetized hydrogen discharges, or a large region of depleted
argon 1s 4 levels around a biased probe in an rf discharge.
-
The excitation dynamics of a micro-structured plasma channel device with an inverted equilateral
triangular cross-section are investigated. This device is operated in argon close to atmospheric
pressure with an ac voltage. It is characterized by means of electrical measurements and optical
emission spectroscopy. One emission phase is observed in each half-cycle of the applied voltage
waveform. Each shows self-pulsing of the device. The integrated intensities for both phases differ
by a factor of about two. Phase-resolved wavelength-integrated optical emission spectroscopy which
resolves the intensity profile of the plasma channel reveals clear differences between positive and
negative half period. Emission features propagating along the discharge channel at velocities of a
few km s −1 are observed. Discharge dynamics are compared with those reported for micro-structured
atmospheric pressure plasma arrays with discharge cavities of similar triangular cross-section. The
c...
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The paper discusses experimental characterization of a surface dielectric barrier discharge plasma
sustained by repetitive, high-voltage, nanosecond duration pulses. The discharge pulse energy is
controlled primarily by the pulse peak voltage and scales approximately linearly with the length of
the electrodes. Images of the plasma generated during the discharge pulse, taken by a nanosecond
gate ICCD camera, show that the plasma remains fairly uniform in the initial phase of the discharge
and becomes filamentary at a later stage. The temperature rise in the discharge, operated in both
continuous mode and in burst mode, is inferred from UV/visible emission spectra. Phase-locked
schlieren images are used to measure the speed of the compression waves generated by the nanosecond
pulse discharge and the density gradient in the wave. The density gradient is inferred from the
schlieren images using absolute calibration by a pair of wedged windows. The results demonstrate
that discharge f...
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A model for the formation of a stationary current-free double layer in collisionless plasmas
expanding in a magnetic nozzle is presented. The model consists of the dynamics of cold ions,
isothermal hot electrons and fere-isothermal, i.e. almost isothermal, cold electrons. It can
determine the position and amplitude of the double layer including the jump in cold electron
temperature across the layer. The magnitude of the jump is consistent with experimental
observations. Plasmas are accelerated mainly by the magnetic nozzle and the contribution from the
double layer is small. The important effects of the ion charge state Z on the flow speed at the
nozzle throat and at the exit are also discussed. It is found that the Mach number at the magnetic
nozzle throat is ##IMG##
[ej.iop.org] {\sqrt
Z} which can be tested in experiments. The exit velocity also scales as ##IMG## {\sqrt Z}
-
Temporal evolution of plasma bremsstrahlung emitted by a 14 GHz electron cyclotron resonance ion
source (ECRIS) operated in pulsed mode is presented in the energy range 1.5–400 keV with 100 µs
resolution. Such a high temporal resolution together with this energy range has never been measured
before with an ECRIS. Data are presented as a function of microwave power, neutral gas pressure,
magnetic field configuration and seed electron density. The saturation time of the bremsstrahlung
count rate is almost independent of the photon energy up to 100 keV and exhibits similar
characteristics with the neutral gas balance. The average photon energy during the plasma breakdown
is significantly higher than that during the steady state and depends strongly on the density of
seed electrons. The results are consistent with a theoretical model describing the evolution of the
electron energy distribution function during the preglow transient.
-
Absolute densities of metastable He(2 3 S 1 ) atoms were measured line-of-sight integrated along the
discharge channel of a capacitively coupled radio-frequency driven atmospheric pressure plasma jet
operated in technologically relevant helium–oxygen mixtures by tunable diode-laser absorption
spectroscopy. The dependences of the He(2 3 S 1 ) density in the homogeneous-glow-like α-mode plasma
with oxygen admixtures up to 1% were investigated. The results are compared with a one-dimensional
numerical simulation, which includes a semi-kinetical treatment of the pronounced electron dynamics
and the complex plasma chemistry (in total 20 species and 184 reactions). Very good agreement
between measurement and simulation is found. The main formation mechanisms for metastable helium
atoms are identified and analyzed, including their pronounced spatio-temporal dynamics. Penning
ionization through helium metastables is found to be significant for plasma s...
-
The assumption of thermodynamic equilibrium in low-temperature plasmas can lead to errors in
determination of electron energy distribution functions (EEDFs) using optical diagnostics.
Significant improvements in the accuracy of EEDFs determined using optical diagnostics on
argon-containing inductively coupled plasmas (ICPs) are possible by fitting an analytic
representation of the EEDF with two adjustable parameters ( x and T x ) to recorded optical emission
spectra. This so-called x -form of the EEDF captures the well-known suppression of the high-energy
portion of the EEDF (compared with the Maxwellian form) observed in ICPs. A review of electron
kinetics summarizes the physical mechanisms that lead to this form, and explains the weak dependence
of x on operating pressure. For the 1–25 mTorr pressure range of argon-containing mixtures in the
system examined, the fixed value x = 1.2 is found to represent the EEDF very well, follow...
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Micro-hollow cathode discharges (MHCDs), driven by a dc voltage source, may operate in a
self-pulsing regime during which the voltage and the current across the discharge are pulsed with a
frequency of several tens of kilohertz. A model for the self-pulsing regime of MHCDs is proposed
based on an equivalent electrical circuit of the whole device. The discharge itself is modeled by a
non-linear resistance in series with an inductance, and it is placed in parallel with the
capacitance of the electrode–dielectric–electrode sandwich hosting the discharge micro-hole. The
capacitance of the coaxial cable used to feed the device is also included. It is shown that a
detailed comparison between theory and experiments allows the discharge non-linear resistance to be
accurately determined. When the discharge current is maximum, this resistance is about 2500 Ω at 50
Torr and decreases to about 750 Ω at 150 Torr. The absorbed power is calculated throughout the
self-pulsing cycle and may be ab...
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Ion energy distributions (IEDs) on a grounded substrate in a Faraday-shielded argon inductively
coupled plasma were measured with a retarding field energy analyzer. A Langmuir probe was also used
to measure space- and time-resolved plasma parameters. IEDs and plasma parameters were studied with
continuous or pulsed positive dc bias voltage on a 'boundary electrode' in contact with the plasma.
For continuous wave plasmas without applied bias, the IED exhibited a single broad peak at the
plasma potential. Applying a continuous positive dc bias on the boundary electrode shifted the peak
of the IED to higher energy. Application of a synchronous dc bias on the boundary electrode during
the afterglow of a pulsed plasma resulted in a double-peaked IED. The mean energies of the two
peaks, as well as the peak separation, were controlled by adjusting the applied dc bias and the
discharge pressure. The full width at half maximum (FWHM) of the peak corresponding to the
synchronous dc bias di...
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Electron transport in CF 4 under linearly gradient antiparallel magnetic fields was analysed in
order to investigate the fundamental properties of magnetic neutral loop discharge plasmas used for
material processing. The electron motion was simulated by a Monte Carlo method under a
radio-frequency (rf) electric field applied perpendicularly to the directions of both the magnetic
field and its gradient. Two typical electron motions, meandering in a weak magnetic field and
gyration in a strong magnetic field, were observed with particular directionalities. The meandering
electrons drifted forward on average similarly to those under a dc electric field. The gyration
induced an electron drift towards the inverse direction. The direction of electron flux was
dependent not only on the rf phase but also on the distance from the magnetically neutral midplane
between the antiparallel magnetic fields. The electron conduction path formed along the midplane had
a structure consisti...
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A floating emissive probe is applied in conjunction with pulsed laser photo-detachment of O − ions
to enable measurement of the dynamic evolution in a plasma potential resulting from the presence of
photoelectrons in a 13.56 MHz inductive radio-frequency oxygen discharge. The emissive probe emits
thermionic electrons, allowing it to reach a saturation potential which is characterized as the
local space potential of the plasma. After the photo-detachment pulse, the local space plasma
potential in the illuminated region shoots up to a higher positive value and then relaxes to
equilibrium in microsecond time scales. Using the relaxation time of the space potential, the
negative ion temperature of O − is estimated over a 10–50 mTorr range and is found to be in the
0.19–0.03 eV range. The negative ion temperature measured by this method is found to be lower than
that calculated from the time evolution in electron density resulting from photo-detachment which is
ind...
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A non-thermal microplasma has been intensively investigated because of its ability to generate high
electron densities with low gas temperatures, even at atmospheric pressure. This work demonstrates
linear arrays of microplasmas generated in atmospheric pressure argon driven by a series of
microstrip resonators. Small arrays of such resonators were previously shown to sustain up to five
microplasmas, but intrinsically weak coupling between resonators is shown to be insufficient to form
wider uniform arrays. An electrical connection between each resonator is shown to enhance the
coupling among resonators, allowing arrays composed of at least 88 elements that extend 11 cm in
width. The application of coupled-mode theory to this system shows good agreement with measurements
of microplasma emission intensity as well as with electromagnetic simulations of these devices.
Operation of arrays at microwave frequencies allows a nearby ground electrode to participate in the
resonance. These...
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The optical characteristics of surface dielectric barrier plasma actuators with a wire/planar
electrode combination and 1 kHz triangular applied voltages were studied using an intensified
charge-coupled device camera and a monochromator in atmospheric pressure air. The spatial and
temporal images were recorded both parallel and perpendicular to the aerodynamic actuator surfaces
on nanosecond time scales. Arc-shaped discharges jumping from above the powered wire across the
dielectric above the grounded planar electrode were observed for the first time. Nitrogen molecular
second and first positive band lines were observed and the discharge temperatures were calculated by
matching the experimental spectra with SPECAIR lines (Laux et al 2003 Plasma Sources Sci. Technol.
12 [/0963-0252/12/2/301] 125–138 ). The electron temperatures were found to be 6800 ± 400 K from the
SPECAIR code.
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The tuneable diode-laser-induced fluorescence (TD-LIF) technique was used to investigate both
velocity and flux distributions of ground-state titanium atoms sputtered from a planar circular
magnetron target working at a low pressure (0.4 Pa) and a high pressure (4 Pa). TD-LIF Doppler
profiles were measured in front of the racetrack: (i) normal ( v z ) and parallel ( v r ) to the
target at several distances ( z ), and (ii) for different angles (α) at 10 mm from the target,
addressing the same local volume. The space variation of the velocity and flux distribution
functions was deduced with high accuracy from the Doppler shift. Thus it was possible to determine
the energetic over thermalized relative atom flux ratio going away from the cathode. The energy
distribution function of Ti sputtered atoms in the normal direction is in good agreement with the
extended Thompson's formula only for the collisionless sputtering regime, namely in...