Characterization of the large area plane-symmetric low-pressure DC glow discharge (original) (raw)

2016, Spectrochimica Acta Part B: Atomic Spectroscopy

Electron density and temperature as well as nitrogen dissociation degree in the low-pressure (10-50 mTorr) large area plane-symmetric DC glow discharge in Ar-N 2 mixtures are studied by probes and spectral methods. Electron density measured by a hairpin probe is in good agreement with that derived from the intensity ratio of the N 2 2nd positive system bands I C ,1− 3 /I C ,0− 2 and from the intensity ratio of argon ions and atom lines I ArII /I ArI , while Langmuir probe data provides slightly higher values of electron density. Electron density in the low-pressure DC glow discharge varies with the discharge conditions in the limits of~10 8-10 10 cm −3. The concept of electron temperature can be used in low-pressure glow discharges with reservations. The intensity ratio of (0-0) vibrational bands of N 2 1st negative and 2nd positive systems I 391.4 /I 337.1 exhibits the electron temperature of 1.5-2.5 eV when argon fraction in the mixture is higher than nitrogen fraction and this ratio quickly increases with nitrogen fraction up to 10 eV in pure nitrogen. The electron temperature calculated from Langmuir probe I-V characteristics assuming a Maxwellian EEDF, gives T e~0 .3-0.4 eV. In-depth analysis of the EEDF using the second derivative of Langmuir probe I-V characteristics shows that in a low-pressure glow discharge the EEDF is non-Maxwellian. The EEDF has two populations of electrons: the main background non-Maxwellian population of "cold" electrons with the mean electron energy of~0.3-0.4 eV and the small Maxwellian population of "hot" electrons with the mean electron energy of~1.0-2.5 eV. Estimations show that with electron temperature lower than 1 eV the rate of the direct electron impact ionization of N 2 is low and the main mechanism of N 2 ionization becomes most likely Penning and associative ionization. In this case, assumptions of the intensity ratio I N 2 + ,391 /I N 2 ,337 method are violated. In the glow discharge, N 2 dissociation degree reaches about 7% with the argon fraction in the Ar-N 2 mixture b 10% and decreases afterwards approaching to~1-2% when the argon percentage becomes 90% and higher. The atomic nitrogen species is produced by electron-impact processes such as, collisions between electrons and nitrogen molecules or between electrons and N 2 + ions. At small Ar fraction in Ar-N 2 mixtures, the atomic nitrogen species is most likely produced by the collisions between electrons and N 2 + ions.

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Specific features of the current-voltage characteristics of diffuse glow discharges in Ar:N2 mixtures

Plasma Physics Reports, 2010

The characteristics of diffuse glow discharges in pure argon and the Ar + 1%N 2 mixture at pres sures of 2-80 Torr were studied experimentally and numerically. The discharge operated in a molybdenum glass tube with an inner diameter of 2.8 cm and interelectrode distance of 75 cm. The current-voltage char acteristic of the discharge and the populations of the N 2 (B 3 Π g ) and N 2 (C 3 Π u ) states were measured. It is shown that, at relatively low pressures (P < 10 Torr), the current-voltage characteristic of a discharge in the argon-nitrogen mixture lies higher than that in pure argon. In contrast, at higher pressures (P > 15 Torr), the current voltage characteristic of a discharge in the mixture lies lower than that in pure argon. As the pressure increases, the effect of the reduction in the discharge voltage becomes more pronounced. A self consistent zero dimensional kinetic model is developed that allows one to calculate the characteristics of the positive column of a discharge in pure argon and Ar:N 2 mixtures under the conditions of high vibrational excitation of nitrogen. A detailed description of the model is presented, and the calculated results are compared with experimental data. The model adequately reproduces the observed change in the current voltage character istic in Ar and the Ar + 1%N 2 mixture with increasing gas pressure. It is shown that the main ionization mech anism in the Ar + 1%N 2 mixture at moderate pressures is the associative ionization of excited nitrogen atoms.

Ionization Mechanisms in Ar:N2 Glow Discharge at Elevated Pressures

41st Plasmadynamics and Lasers Conference, 2010

A self-consistent zero-dimensional kinetic model is used to investigate the ionization mechanism in Ar:N 2 glow discharge at elevated pressures. Calculations are performed for pure argon and Ar+1%N 2 at gas pressure 40 Torr. Results of simulations are compared with experimental data. It is shown that developed model reproduces effect of the discharge voltage decrease with the addition of nitrogen admixture to argon observed in experiments. It is also shown that under considered conditions the production of electrons in discharge plasma is provided mainly by processes of associative ionization of excited nitrogen atoms. Nomenclature P = gas pressure T g = gas temperature R = discharge tube radius L = discharge tube length I = discharge current U = discharge voltage EEDF = electron energy distribution function E/N = reduced electric field E = electric field strength N = atoms and molecules number density T v = vibrational temperature W e = electron drift velocity T e = electron temperature u = electron energy v = number of vibrational level n e = electron concentration

On the influence of metastable states and the behavior of the EEDF in the characterization of the negative glow of a N 2 -Ar discharge by OES

Journal of Physics: Conference Series, 2014

Optical emission spectroscopy (OES) is an essential diagnostic technique in many plasma systems, such as those used for surface treatments or fabrication of thin films. Despite the simplicity of application of OES, its interpretation is not straightforward. In particular, it requires the use of models, which due to the complexity and variety of discharge conditions, have not yet been fully understood [1]-[3]. In addition, Langmuir probes have been widely used to characterize plasmas. They allow the measurement of several parameters of interest, such as the electron density and temperature, as well as the determination of the electron energy distribution function (EEDF) by numerical derivation of the characteristic V − I [4] or by probe-current modulation [5]. In this work, some second positive system bands in the negative glow of an Ar-N 2 plasma at a pressure of 2.5 Torr were investigated both by OES and Langmuir probes, for different mixture concentrations. The main purpose of this study was to verify how metastable states and the behavior of the EEDF may influence the interpretation of OES data.

Spectroscopic Characterization of Nitrogen DC Pulsed Discharge

2008

The densities of most emitting species and gas temperature (T g) are investigated in a nitrogen DC pulsed discharge. The discharge current and gas pressure are varied from 70 to 150 mA and 133 to 470 Pa, respectively. T g is determined through rotational temperatures of first positive (1 +) and second positive (2 +) emission systems. These temperatures are deduced by comparison of simulated and measured spectra. The T g values range from 450 to 950 K and increase linearly with increasing the two discharge parameters studying. The densities of N 2 (B 3 Π g), N 2 (C 3 Π u) and N 2 + (B 3 Σ + u) species increase with increasing discharge current. This behaviour is coherent with a production process by direct impact excitation form the ground state. The densities of emitting neutral species decrease with increasing pressure due to fact that the collisional quenching starts to play a significant role at higher pressure. An opposite trend for ionic species is observed. This fact seems to prove that other production mechanisms are involved.

A comparative study of the electron distribution function in the positive columns in ? and ?/He dc glow discharges by optical spectroscopy and probes

Plasma Sources Science & Technology, 1998

We compare to the probe method a spectroscopic method for determining in plasmas the electron distribution function (EDF) over a wide energy range. For a test of the radiative-collisional model we use to describe the plasma radiation, the measured vibrational distributions of 0963-0252/7/3/008/img12(C-B) and 0963-0252/7/3/008/img13(B-X) were compared with calculated ones using our model and EDFs measured by Langmuir probes. From this comparison we obtain a value for the rate constant for vibrational relaxation at the walls. In a second step we invert the system of model equations for obtaining the EDF from measured line intensities. From the vibrational structure of the emission spectra of the nitrogen molecule the EDF is obtained in the energy range of 1.5-4.5 eV. From the relative intensities of the emission of nitrogen molecules and helium atoms the EDF for electron energies above 11 eV is derived. In the region between these ranges the EDF is interpolated. The results agree within the limits of the experimental errors with the EDF measured directly by the probe.

An investigation into dissociative mechanisms in nitrogenous glow discharges by optical emission spectroscopy

Vacuum, 1995

is studied in DC diode and thermionic triode glow discharges of pure nitrogen and nitrogen-argon mixtures. Optical emission spectroscopy is used to determine the relative proportions of atomic and molecular nitrogen in the cathode sheath and plasma regions of these discharges operated at -2 kV cathode bias in the range 0. I-10 Pa. The results show that for nitrogen-argon diode discharges at 6.67 Pa total pressure, (i) dissociation rates within the sheath compare with those of pure nitrogen discharges operated at s$nilar nitrogen pressure and the same mechanism (N;-N$ dissociative charge exchange) is believed to be primarily responsible;

Experimental evidence of Penning ionization role in a low pressure direct current nitrogen glow discharge

The European Physical Journal Applied Physics, 2004

On the basis of experimental measurements of the electric field (which varies from 5 to 60 V/cm) and the N-atom relative density variation (one order of magnitude), mechanisms of ionization and dissociation in direct current glow discharges are discussed for pressures ranging from 0.5 to 5.0 torr and current between 1 and 50 mA. It is shown that: (i) at low pressure (E/N > 40 Td) ionization is governed by electronic impact and Penning reactions; (ii) at high pressure (E/N < 40 Td) the ionization is mainly governed by Penning reactions.

DC normal glow discharges in atmospheric pressure atomic and molecular gases

Plasma Sources Science and Technology, 2008

DC glow discharges were experimentally investigated in atmospheric pressure helium, argon, hydrogen, nitrogen and air. The discharges were characterized by visualization of the discharges and voltage and current measurements for current of up to several milliamperes. Significant differences are seen in the gas temperature; however all the discharges appear to operate as temperature and pressure scaled versions of low pressure discharges. In the normal glow discharges, features such as negative glow, Faraday dark space and positive column regions are clearly observable. In hydrogen and to a lesser degree in helium and argon standing striations of the positive column were visible in the normal glow regime. Normal glow characteristics such as normal current density at the cathode and constant electric field in the positive column are observed although there are some unexplained effects. The emission spectra for each of the discharges were studied. Also the rotational and vibrational temperature of the discharges were measured by adding trace amounts of N 2 to the discharge gas and comparing modeled optical emission spectra of the N 2 2nd positive system with spectroscopic measurements from the discharge. The gas temperatures for a 3.5 mA normal glow discharge were around 420 K, 680 K, 750 K, 890 K and 1320 K in helium, argon, hydrogen, nitrogen and air, respectively. Measured vibrational and excitation temperatures indicate non-thermal discharge operation. Mixtures of gases achieved intermediate temperatures.

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