Research Article | Open Access
Konstantinos Katsonis, Chloe Berenguer, "Global Modeling of N2O Discharges: Rate Coefficients and Comparison with ICP and Glow Discharges Results", International Journal of Aerospace Engineering, vol. 2013, Article ID 737463, 25 pages, 2013. https://doi.org/10.1155/2013/737463
Global Modeling of N2O Discharges: Rate Coefficients and Comparison with ICP and Glow Discharges Results
We developed a Global Model for N2O plasmas valid for applications in various power, gas flow rate, and pressure regimes. Besides energy losses from electron collisions with N2O, it takes into consideration those due to molecular N2 and O2 and to atomic N and O species. Positive atomic N+ and O+ and molecular N2O+, , and have been treated as separate species and also negative O− ions. The latter confer an electronegative character to the discharge, calling for modified plasma sheath and plasma potential formulas. Electron density and temperature and all species densities have been evaluated, hence the ionization and dissociation percentages of N2O, N2, and O2 molecules and the plasma electronegativity. The model is extended to deal with N2/O2 mixtures feedings, notably with air. Rate coefficients and model results are discussed and compared with those from available theoretical and experimental work on ICP and glow discharge devices.
The present work aims to characterize N2O fed plasma devices working in various configurations, as plasma reactors, hollow cathodes, and plasma thrusters, by means of a Global (volume averaged) Model (GM). The well-known GM describes a plasma device in its entirety, taking into consideration the atomic and molecular properties of the used gas or mixtures, together with the device geometry and the prevailing physical conditions. Examples and general properties of such models can be found in standard handbooks .
Obviously, the problem of N2O plasmas description becomes more complex than in the case of a monoatomic inert gas as the argon, studied previously for inductively coupled plasmas (ICP) including plasma reactor (PR) and for helicon plasma thruster (HPT) applications, by means of an adequate GM (see  and references therein). In  the HPT plasma was separated in two regions, an external, cooler region encompassing about 90% of the plasma cross section area with low ionization percentage named the “mantle” region and an internal hotter one, the “core” region, where the plasma is mostly ionized. Conditions in the “mantle” region are rather similar to those of the PR, both for Ar and for N2O and N2/O2 mixtures feedings. In the present paper only ICP and glow discharge (GD) results are given, which are also useful in modeling the “mantle” region of HPT.
The molecular structure of the N2O and that of the molecular products examined here reveal vibrationally excited states that have to be taken into account in addition to the electronic ones. Because of the presence of molecular species, the dissociation processes have been taken into account as they play a very important role, leading to species which have to be considered both in the energy loss power balance equation (PoBE) and in the particle balance equations (PaBE) of the GM. Note that the N2O dissociation by electron impact is already important at intermediate pressures, for the absorbed power and N2O flow rates considered here. Also, the negative species introduce an electronegativity in the discharge, which was not always present in previous discharge studies of molecular species as H2. However, in  the electronegativity from H2 was duly taken into account. The GM which we obtained for N2O plasma discharges is successfully applied to experimental studies of N2O discharges and its results compare favorably with existing theoretical ones. Moreover, the present model can be used to design and study discharges in N2/O2 mixtures, often leading to products similar to those encountered in N2O discharges. It is very important to note that the N2O dissociation considered primarily here may become so important that the N2O feeding leads practically to an atmosphere of N2 and O2 mixture. GMs are also of interest to some atmospheric studies cases. GMs of He and H2 were also addressed lately, partly because these gases are also important in space entry studies (cf. [4–6]), although inclusion of additional equations as those of Navier Stokes becomes necessary when high pressure conditions prevail.
In the following, the main equations used and the model description are given in Section 2. A review of the main processes encountered in the plasma follows in Section 3, where processes which have been included when writing down the PaBEs are described. In Section 4, we shortly describe the N2O structure and also additional processes concerning electron collisions with N2O. Then, we present briefly the N2 structure and N2 related processes. A similar analysis follows for the O2, O, and NO species and their ions, necessary for the evaluation. Calculations of for N2O, N2, O2, N, and O are presented and discussed in this section. Then, we give in Section 5 a short overview of three main N2O discharges regimes. Section 6 describes results obtained by our GM for a typical plasma reactor when fed with N2O. Results are compared to those existing in the literature, mainly to the recent calculations and measurements of Shutov et al.  for a plasma reactor fed with N2O, working in a pressure of about 4 mTorr. In Section 7, our GM results are compared with the and measurements of Yousif and Mondragon  made in a hollow cathode (HC) plasma discharge in pure N2O, with pressure varying from 200 mTorr to 1.1 Torr. This comparison is mainly oriented towards lower pressures, reactions not included in our model becoming possibly important in atmospheric pressure. Therefore, no comparison is made with results obtained for air in , which concern the quite higher atmospheric pressure. We also compare our results to those obtained by de los Arcos et al.  for a hollow cathode fed with N2O, with a flow rate varying from 3 sccm to 265 sccm. In Section 8 we present results obtained for N2/O2 mixtures, which are compared to results obtained by Gordiets et al. . A comparison is made of our and of vibrationally excited N2 densities with experimental and theoretical results of . Finally, in Section 9, we give the conclusions of this work.
2. Description of the Model and Governing Equations
We first briefly remind that GMs are based on an equation system (see, e.g., ) essentially composed by the following.(a)A power balance equation (PoBE), which relates the absorbed power to the electron density by means of the collisional energy loss () term, taking into account the main species. quantifies the amount of energy loss by electron collisions with a “heavy” particle, due typically to elastic scattering, excitation, ionization, and dissociation processes. The main heavy particles considered here are N2O, N2 and O2 molecules and N and O atoms. To obtain an account of the bulk of the energy spent in collisions involving electrons, a number of electronic (and vibrational in case of a molecule) excited states have been considered.(b)A system of particle balance equations (PaBE) containing the densities of species for a set of electron density and electron temperature . This is similar to the well-known statistical equations set constituting the basis of the Collisional-Radiative (C-R) models . In order to reveal the properties of the main plasma parameters, a rather simplified scheme including only eighteen species and the eighteen corresponding kinetic equations was introduced in the present model. It includes seven ground level species (N2O, N2, O2, N, O(3P), O(1D), and NO) plus the most abundant excited species and the main ions. Less important species have been taken only indirectly into account, when calculating the corresponding included in the PoBE. As N2 population is often considerable in the conditions considered here, its five lower vibrational states were included in the kinetic system.
Concerning oxygen species, the GL of the molecule is included in the PaBE and the lower electronically excited state of the molecule in the PoBE. The first and the second ground levels of the atomic oxygen were also included in our calculations, as was also the case in previous studies [14, 15]. In describing the ionization-recombination equilibrium, the N2O+ species are included in our PaBE system. This allows for correctly evaluating not only the density of neutral species but also the electron density and temperature. The single ions , , N+, and O+ of the main products N2, O2, N, and O were also included in the PaBEs set; their densities become considerable in presence of important N2O dissociation. Moreover, O− ions are accounted in a dedicated equation of the PaBEs set because they are usually formed in an important amount and they confer the electronegative character to the discharge. Consequently, we are left with a simplified set of only seven equations for ground level species, of five for the excited states, and of six for the ions, a total of eighteen.
Charged particles (consisting here of six ionic species plus the electrons) are related through the quasi-neutrality equation, taking in the N2O plasma case the form
Modeling of N2O plasmas is based primarily on N2O data. However, N2, N, O2, and O data are also very important, because dissociation of N2O generates nitrogen and oxygen species in various percentages. Because nitrogen species are present in an important amount in various gas discharges encountered in laboratory and nature plasmas including N2O ones, we proceeded to a separate study of pure N2 plasmas. Results of this study (see ) contributed to evaluate nitrogen data and to validate the corresponding part of the present GM. Results of our GM for pure N2 discharges not presented here compare favorably with those obtained by Kang et al.  and also with those from Thorsteinsson and Gudmundsson . Both of these studies compare theoretical GM results with experiments.
Support of the part of the present GM which concerns oxygen species was obtained on the basis of our recent studies on discharges in plasmas containing O2 species, . These address particularly evaluation of electronegativity in O2 discharges. Our results for pure O2 discharges compare favorably with those obtained by Gudmundsson et al. , Gudmundsson and Thorsteinsson , and Corr et al. . Data and results from  as well as from  guided our choices on the selection of the oxygen and nitrogen species and on the processes to be retained in order to get a correct description of O2/N2 mixtures and of N2O plasmas.
Following standard procedures (see, e.g., our argon model described in  and references therein), the present N2O GM is composed of a power balance equation (PoBE) and of a particle kinetic equations set (PaBE). The PoBE is written as where is the elementary charge andthe collisional energy loss of species . Also, is the ionization rate coefficient for the species and is its recombination on the wall. The wall recombination rate is given by with the Bohm velocity given by . For , the mean kinetic energy lost per electron, the value proposed in  for electrons having a Maxwellian energy distribution was used. The mean kinetic energy lost per ion, noted by , is given in an electronegative gas by the sum of the sheath and presheath (plasma) potentials; that is, . The sheath potential is the potential of the sheath with respect to the wall, which is obtained by equating the positive ion fluxes with the electron flux , where the thermal velocity of electrons is ; the potential becomes the plasma potential when and are equal. is the cylindrical surface area of the device and is the potential of the plasma with respect to the sheath. For this potential we use the expression coming from  (see also [1, page 180]), where is the plasma electronegativity at the sheath edge, with an approximate value of conformal to . In (3), the plasma electronegativity is defined as , where is the density of species and , with being the negative ion temperature. We assume to be equal to the positive ion temperature.
The area for effective loss appearing in (2) under is given by with and being the radius and length of the device and and the axial and radial edge to center ratios of positive ion density. A convenient formula joining the three plasma regimes of low, intermediate, and high pressure was proposed previously by Lee and Lieberman . For cylindrical geometry it is given by [1, 21] where is the first order Bessel function and the first zero of the Bessel function. The ambipolar diffusion coefficient is given by , with being the diffusion coefficient for positive ions (see ). A modification of due to the presence of a magnetic field in the “core” region of the HPT is also possible for instance by using adequate formulas contained in Chapter 5 of . At the present stage, we introduced only a simple factor in the plasma wall reaction rates, taking into account both the ionic and the neutral species losses from the “core” to the “mantle” region (typically 5% for the ions and 30% for the neutrals). The mean free path of ions is calculated by where is the density of a neutral species and is the ion-neutral scattering cross section for the collision of the th neutral with the th ion. Ionic momentum transfer for atomic and molecular oxygen is assumed to be following . Moreover, ionic momentum transfers for with N and N2 correspondingly about and , following . We assume a combined momentum transfer of for the N2O plasma as well as for the N2/O2 mixtures. A term taking into account the electronegativity is to be added to the density ratios; therefore, in the N2O case, we write in which encompasses .
In addition to the PoBE (2) we need the PaBE set, of which each equation, say of species , is constituted by the sum of all the creation and destruction terms for the given species and can be written as where denotes the sum of all terms and including the production and the loss rates involving the species . Each reaction rate is given by the product of the reactant densities and the corresponding rate coefficient :
An additional pressure term is needed, which follows the perfect gas law and is written numerically as where is the density of the species given in , is the pressure which, exceptionally for (8), is given in Pa units, is the Boltzmann constant in , and is the gas temperature in . An additional term for the pressure of ions should be retained for higher power and ionization calculations.
3. Main Processes Involved in a N2O Plasma and Calculation/Evaluation of Their Rates
We describe in this section the main processes included in the PaBE kinetic system, important for the description of the plasma. Data used in the PoBE equation are investigated in Section 4. A review of the used electron collisions rates is given schematically in Figure 1. Elastic collision and excitation rates which are described in Section 4 are included in Figure 1. Note that coefficients for all dissociative processes are given by curves in red.
We introduced a total number of eighteen species in the PaBE, consisting of twelve neutral ones, N2O, N2, O2, N, O(3P), O(1D), and NO, of five positive ions N2O+, , , N+, and O+ and of one negative ion O−. These species are present in various physical situations we are interested in. Table 1 gives a synoptic view of the processes in which they appear. Table 1 includes in general more processes than those contained in similar tables of [7, 10].
In Tables 2 to 5 we report in detail the sixty-two processes which we use in the N2O GM. The processes are ordered following four sets. Data also used in the energy loss calculation are indicated with stars in the last column.
The corresponding reaction rates were taken into consideration when writing down the eighteen PaBE equations which allow for evaluating the species densities for each , set. We expect these reactions to be the most important for the considered applications, related to typical plasma cases (i), (ii), and (iii) which are described in Section 5. The model allows for evaluating the plasma and and its constituents densities as they vary with the pressure, the absorbed power, and the flow rate. For specific applications, it is possible to introduce more species and additional reactions in order to include more constituents and to enlarge the physical conditions domain.
The set of reactions we use is larger than the one proposed initially by Date et al.  and used subsequently by Shutov et al. . Collisions of O(1D) with N2O and N2 have been included, like in . Moreover, we included the rearrangement collisions of O(1D) with NO and the deexcitation ones of O(1D) with O2 as in [1, page 273]. However, the reactions involving NO2 previously used by de los Arcos et al.  in a slightly reduced reaction set are here neglected. Note that  contains also an extended bibliographic study on the subject, not reproduced here. In what concerns the considered species, O(1D) which constitutes the second GL of oxygen, has been introduced in [7, 23] because plasma etching was the aimed application. This species has been also introduced here as it can be quite present (see [14, 15]) and may play an important role in the total oxygen ionization, an important process which was not introduced in [7, 23]. We do include the excitation/deexcitation of O(1D) by electronic collision. These reactions, often omitted in previous N2O work, are important for the O(1D) population which directly contributes to the N2O dissociation. Moreover, we added the , , N+, and O+ ions to the initial set of species used by Date et al. , as N2, O2, N, and O may become predominant plasma species in low and intermediate pressures and therefore their ions are important, both in order to calculate correctly the plasma density and also because they need to be precisely characterized when we consider various space applications. In the latter applications, often exist quite ionized plasma regions where the electron temperatures of interest may be high, leading to ionization percentages clearly higher than those of the PR cases also considered here.
Rate coefficients for electron collision processes were calculated by integrating the cross sections from available references (see, e.g., [1, 23–38] and references therein) in the range from threshold to 500 eV. The corresponding rates were parameterized with polynomials in a range from 0.2 to 100 eV, except when otherwise stated.
For heavy particle collisions, we used directly the rate coefficients given in [1, 7, 14, 15, 39, 40, 56]. Reactions include various neutralization processes. No charge exchange reactions were included in the final form of our GM presented here. This was also the case in  with collisions of oxygen species. Our trial calculations including charge exchange between oxygen species have not shown big differences in the GM results for the studied physical conditions.
Rate coefficient values for the processes introduced in the model are briefly discussed in the following. Data needed for modeling of N2 and O2 plasmas have been discussed and collected in dedicated databases. Their evaluation and application to dedicated GMs for N2 and O2 will be made available separately [16, 18].
3.1. N2O Ionization
Concerning the reaction rates for the N2O ionization, reaction no. 1 of Table 2, the cross section from Kim et al.  was integrated previously by Shutov et al.  for from 2.4 to 2.8 eV. We compared the cross section from Kim et al. , Dupljanin et al. , Rapp and Englander-Golden , Iga et al. , the Deutsch-Märk formula (see for instance [42, page 84]), and a semiclassical two-parameter formula reported in , as adapted for molecules. Recent cross sections by Dupljanin et al.  were integrated to obtain the rate coefficient. The latter are parameterized with a polynomial of order seven. The considered cross sections are compared in Figure 2.
3.2. N2O Dissociation Leading to N2 and Oxygen Species Products
Dissociation of the N2O by electron impact, reactions nos. 2 and 3 of Table 2, constitutes the main dissociation channel of N2O. Cross section for reaction no. 2 was plotted in . We integrated this cross section to get the rate coefficient in a temperature region going from 0.2 eV to 100 eV, assuming a Maxwellian distribution. We compared the obtained rate with the values coming from the formula given by Shutov et al.  based on results obtained from Cleland and Hess . Validity of this formula was restricted between 2 eV and 10 eV. This comparison is shown in Figure 3 as an example of our N2O data evaluation work. In Figure 3, the values of de los Arcos et al.  and those of , as reported in , are also plotted for comparison.
In the 2 eV region, after integration of the cross section provided by  we obtain dissociation rates 30% lower than those of Shutov et al. . The difference is increasing with the temperature and becomes of one order of magnitude for 10 eV. Our values are the same with those of  for but become inevitably higher with increasing , because in  a constant value of rate coefficient was used. For the same reason, our values are neatly lower than those of  for low . Moreover, we find the same rate value with  for a of 6 eV but a rather big discrepancy for 3 eV. Figure 3 clearly illustrates that the data for reaction no. 2 of N2O are badly known. Using the relative magnitude of the rates of reaction no. 3 in comparison with reaction no. 2, a cross section seven times lower was used in , while a rate coefficient factor of one order of magnitude is mentioned in  and a rate of about three times lower is used in . In the present work, in order to evaluate the rate of the dissociative excitation, reaction no. 3 in Table 2, we shifted the cross section threshold of reaction no. 2 of about 2 eV which is the difference between the two levels excitation energies, before integration over a Maxwellian distribution, keeping the same value of cross section. The so obtained result is also shown in Figure 3.
3.3. N2O Dissociation Leading to NO and N
For the electron impact dissociation of N2O, reaction no. 4 of Table 2, a cross section is provided in . After integrating it, comparison with the rate coefficient values given in Shutov et al. , also coming from a formula based on  cross section, shows a significant discrepancy. This comparison is illustrated in Figure 4. Values of Cleland and Hess  for 3 eV and 6 eV are also shown in Figure 4. We see that values of  are generally in disagreement with ours, except for 3 eV, where the curves of the two sets of data cross. Rate value of  is identical to our for a of 6 eV.
3.4. N2O Dissociative Attachment
For the dissociative attachment, reaction no. 5 of Table 2, cross section calculated by Chaney and Christophorou  as reported in Christophorou and Olthoff  has been followed by a recent experimental evaluation from Dupljanin et al. . We integrated the cross section provided by  valid for 273 K over a maxwellian distribution. Note that contribution of the excited states is included in the cross sections of [26, 29]. As the provided cross sections correspond to defined gas temperatures (273 K for  and 295 K to 1040 K for ), to obtain values for = 300 K and 500 K, we followed the theoretical data of . We find a big discrepancy with the rate given by Shutov et al. , who integrated the cross section of Younis et al.  to obtain values in the range from 2.4 to 2.8 eV represented by a simple slope. Our evaluation suggests that the cross section from  and, accordingly, also the rate given by Shutov et al.  may be underestimated up to two orders of magnitude. Comparison of rates obtained from cross sections from [26, 29] for 300 K is shown in Figure 5, together with values for which we also used.
3.5. N2O Dissociation by Collision with O(1D)
For reactions nos. 6 and 7 of Table 2, we used the rate values from Kossyi et al.  which are very close to previous experimental values of Atkinson et al. . These values from  were used instead of those proposed in . They are also shown in Figure 5.
3.6. NO Rearrangement
For the NO rearrangement reaction with N, no. 8 of Table 2, we used data proposed in . Rates fitted by Shutov et al.  to the values of Gamallo et al.  in the range of 200 K to 5000 K are very comparable with the values of  that we used. For the NO rearrangement reaction with O, no. 9 of Table 2, we also used the rates coming from .
3.7. Neutralizations of O− by N2O+, N2+, and O2+
For the N2O+ neutralization process no. 10 of Table 2, it is possible to use the rate given by Shutov et al. , also coming from . The same value is proposed also for and species neutralization. However, we preferred to adopt the more recent value proposed in  and reported in  for . The same value was used also for the other two neutralization reactions with and N2O+.
3.8. N2 and O2 Ionization
For the ionization of N2 and of O2, reactions nos. 1 of Table 3 and of Table 4, respectively, we integrated the experimental cross sections of Armentrout et al.  coming from Christophorou and Olthoff  for the N2 and this of Straub et al. for the O2 . Existing experimental values from other sources, both for N2 and O2, are in very good agreement with the ones we used. For the ionization from N2 vibrational levels, we calculated the rates according to a procedure which was also used in the following case of the N2 dissociation.
3.9. N2 Dissociation
Dissociation of N2 molecules by electron impact, reactions no. 2 and nos. 19–23 of Table 3, was included in our model by integrating the cross section of Cosby . We considered that the main dissociation channel leads to a mixture of the N(3P) and N(1D) products even if the latter level was not explicitly introduced. To evaluate the dissociation (and ionization) from the vibrational states we displaced the cross section for both in energy and magnitude. The factors used for the shift in magnitude are given in column of Table 8.
3.10. N2 Vibrational Excitation
For the excitation from N2 to the vibrational state , reaction no. 4 of Table 3, we used the experimental cross section values from Itikawa  measured by Brunger et al. . For the excitations from to to 5, reactions nos. 5 to 8 of Table 3, we shifted the excitation cross section of to both in energy and in magnitude. The parameters of the shift were based on the maximum values of the cross sections of Phelps and Pitchford . The obtained cross sections were integrated over Maxwellian distribution as well as the cross sections from  to obtain the corresponding rate coefficients. Rates obtained by this evaluation were slightly higher than the ones obtained from the integration of the cross sections given by Phelps and Pitchford .
3.11. N Ionization
For the electron collision ionization of N, the cross section for N(4S), the first GL, was used only in the energy loss calculation described in Section 4. It was evaluated and parameterized using the Drawin formula  duly adapted and subsequently integrated to obtain the ionization rates. However, in the kinetic system, we used the cross section given by Kim and Desclaux  for a mixture of about 70% of N(4S) and 30% of N(2D). This cross section leads to higher values for the ionization rate. Using this value instead of the one for N(4S) leads to pure N2 discharge results in rather good agreement with those of the literature [12, 17], where the level 4S, 2D, 2P were explicitly introduced.
3.12. O2 Dissociation
For oxygen dissociation, processes nos. 6–9 of Table 4, the rate coefficients were taken from Lieberman and Lichtenberg , a selection encompassing rates from various sources. Although they were originally recommended for the range of 1 eV to 7 eV, we used those values also for higher energies.
3.13. O2 Dissociative Attachment
To obtain the rates related to process no. 10 of Table 4, we integrated the cross section of Christophorou and Olthoff  for which results from the theoretical work of O’Malley  and the experimental results of Henderson et al. . We also shifted this cross section to obtain a second value applicable for 500 K. We used the first one in applying our model in the case of the discharge studied by de los Arcos et al.  (Section 6) and the second one for the application tackled by Shutov et al.  study (Section 5) and for the propulsion applications of Section 8. In Figure 6, the rate coefficients which we obtained for 300 K and 500 K are compared to the values given in [1, 14].
3.14. Recombination by Electronic Collision/O2+ Dissociative Recombination/O(1D) Deexcitation by O2 Collision
3.15. O+ and O2+ Neutralization
For neutralization rates, processes no. 14 and 15 of Table 4, two sets of data exist. The first set, given by Gudmundsson et al. in 2000 , is very similar to the one used in Gudmundsson et al. 2001  and is in good agreement with values proposed by Kossyi et al. . The second, proposed later by Gudmundsson and Lieberman in 2004  and used in the Ar/O2 model in 2007 , is reported in . The second set is based on experimental values of Hayton and Peart  and of Padgett and Peart  and it is about one order of magnitude lower than the first. Evidently, the first set gives electronegativity values much lower than the second one, especially for a pressure around 10 mTorr. In the present model, we use the most recent values reported in .
3.16. O− Recombination on N2 ()
We introduced reaction no. 1 of Table 5, N2 + O− N2 + O + e−, as an inverse process of reaction no. 5 of Table 2, N2O + e− N2 + O−. In the literature, some rates are proposed for reaction + O− N2 + O + e−, where is an electronically excited state. As we did not introduce electronically excited states of N2 in the kinetic system, we made the arbitrary choice of involving the higher vibrational levels in this reaction. However, we introduced an invariable rate coefficient instead of the value proposed by Kossyi et al.  for the excited N2(A) state. This value was chosen estimating that about 10% of N2 species are in the levels , and about 0.1% of N2 species are in electronically excited states.
No reaction was included for + O− → O3+ e− nor for + O− O2+ O + e− as these reactions are expected to be negligible for pressures lower than 100 mTorr.
3.17. O(1D) Deexcitation on N2
For reaction no. 3 of Table 5, we used a rate coefficient exclusively for the level N2. We estimate that introducing this rate for N2) species compensates the introduction of a rate cm3s−1 for all the N2 species without distinction of their vibrational state as was recommended by Kossyi et al. . Note that de los Arcos et al.  have used a constant rate of which is near to the value of .
3.18. Recombination and Reformation on the Wall
Recombination of positive ions N2O+, , , N+, and O+ on the wall was estimated by means of the effective rate coefficient of the heterogeneous decay of positive ions, as described in detail in  and also briefly mentioned by Shutov et al. . For evaluating the N2 and O2 formation on the wall, reactions nos. 25 of Table 3 and nos. 20-21 of Table 4, we used the wall recombination formula from .
4. Structure, Excitation, Elastic Collisions, and Collisional Energy Loss of the Main N2O Plasma Constituents: N2O, N2, O2, N, and O
We address here particularly the structure of the main plasma constituents, elastic collisions, and excitations and the calculation of their collisional energy losses. Rates of ionization, a key process for collisional energy losses, were already addressed in Section 3.
4.1. N2O Electronic and Vibrational Excitation
Let us consider the main states of the N2O molecule with its first ionization state N2O+. These are included in the PaBE as separate species. Six excited states of N2O were introduced for the evaluation of the corresponding energy loss coefficient , appearing in the PoBE. They consist in three vibrationally excited states plus three electronically excited states mentioned by Dupljanin et al.  see Table 6. The ionization energy of the ground level is 12.894 eV according to . The excitation energies coming also from  are given in Table 6.
|Energy values are those given in .|
Electronic and vibrational excitation rates of N2O molecules were obtained by integration over a Maxwellian distribution of the cross sections compiled in . The elastic collision rate, to be also added in the evaluation, was based on the total elastic scattering cross section given in  which was also integrated over a Maxwellian distribution. We also calculated dissociation and ionization rates which must be included in the calculation on the basis of the cross sections addressed previously (nos. 1–3 in Table 2). No more dissociation and attachment have been included in the calculation, because we verified that their influence is unimportant for the overall value. Cross sections integrations were made in general in the energy range from threshold up to 500 eV, for the ionization and electronic excitation. Whenever the cross sections are quickly falling to negligible values, the integration was restricted to a shorter range. This is the case for the elastic and vibrational cross sections. We estimate that the obtained rates lead to values valid from 0.2 eV up to to 100 eV.
The list of additional reactions involved in the calculation is shown in Table 7. Adding reactions of this Table 7 to those contained in Table 2 marked with a star, we obtain a set to be compared with Table 1 of Younis et al. . Four dissociations giving excited species are contained in the latter table instead of two given in our case.
|Threshold energies of the excitation cross sections given by Phelps and Pitchford .|
Lower energies for which Phelps and Pitchford  give a cross section value.
Cross section given by Engelhardt et al. .
Data reported in .
4.2. N2, N Main Nitrogen Compounds
Special care was taken for the evaluation of molecular nitrogen data, as N2 was found to be predominantly created in the N2O plasma discharge, at least in the studied conditions (ii) and (iii) described in Section 5, in which the N2O dissociation is sustained. In so doing, the GL state of the neutral N2 (), including its first vibrationally excited () states and its first ion in the ground state (), was included in the PaBE. Also, the first GL of the neutral atomic nitrogen N(4S) and also GL of its first ion N+(3P), coming from the N2O dissociation process (no. 4 of Table 2) and from the N2 dissociation processes (nos. 2, 19–23 of Table 3), were included.
In PoBE (2) an increased number of N2 vibrational and electronic levels, 22 species in total, were included in the energy loss calculation. The main data for the included species according to various authors are compared in Table 8. In this table, the first column shows the level description taken from Itikawa . The second up to the fifth column give the excitation energies coming from various authors including Allan , Hasted , Phelps and Pitchford , and Engelhardt et al. . Dissociation energy of N2 GL was taken from Cosby  and ionization energy from .
Although dissociation/ionization energies are from Cosby /Hasted , vibrational excitation energies from Allan  have been used to obtain the threshold energies of the dissociation/ionization processes from vibrationally excited levels, marked by stars in Table 8.
Calculation of includes eight vibrational excitation rates and twelve electronic excitation rates as well as three dissociation processes. Elastic and ionization rates were also included in this calculation. A list of additional processes included in calculating the energy loss of N2 is given in Table 9, while processes of Table 3 marked by a star are used both in the PoBE and PaBE.
Data for the elastic collision (no. 1 of Table 9) are taken from . The vibrational excitation cross sections of N2 were integrated using the values of . For the excitation of electronic states we made an evaluation of the cross sections based on values coming from [30, 31]. For processes 15 and 16, dissociation with simple and double ionization, we integrated the cross sections of Tian and Vidal . Note that those authors also give an ionization cross section of N2, which is very close to the values of  used here. results obtained with these data will be presented and commented in Section 4.4.
Analogous work was made for the atomic species N, for which the list of the additional reactions, taken into consideration in the energy loss calculations in addition to those listed in Table 3, is given in Table 10. We included effects of elastic collisions (process no. 1 of Table 10) that we calculated using the theoretical cross section of Bauer and Browne, as reported in Neynaber et al. . Also, we included excitations of the three outer shell excited states, namely, 2s22p23s, 3p, and 3d as well as the 2s12p4 inner shell state and we added the excitations of the ground level compounds (2p32D) and (2p32P) as was the case in .
4.3. Molecular and Atomic Oxygen and NO Formed in the Discharge
(i)The GL of the oxygen molecule O2 and its first ion were already included in the PaBE set, on the basis of a previous study of discharges in O2, , together with the GLs of the neutral atomic oxygen O(3P) and O(1D), the negative ion O−(2P) and the positive ion O+. In the concomitant energy loss calculation of O2, we took in consideration one elastic collision, two vibrational excitations, four electronic excitations, and two dissociations. The simple formula given in  was used for the elastic rate evaluation. Vibrational and electronic excitation energies and rate coefficients formulas were those of  as quoted in . We also used the dissociation rate coefficients given in  coming from . The used rates were considered being valid in the region from 1 to about 7 eV. Accordingly, values calculated in  and used also here are only approximate for high values. (ii)For the atomic oxygen we used here the values reported in .(iii)The GL of the nitric oxide NO () was also introduced in the PaBE, as at least the GL of the NO molecule species is expected to be present. Here, the NO is mainly formed by dissociation of the N2O (reactions nos. 4 and 7, Table 2). It is destroyed by rearrangement when colliding with the N atoms (reaction no. 8 of Table 2) and O atoms (reaction no. 9 of Table 2). The total amount of NO present in the discharge is then strongly related to the densities of the N and O atomic species. However, the electron collision energy loss due to the NO molecule was neglected as the latter is present in a much lower amount than the other species for all the studied conditions.
4.4. Evaluation of the Collisional Energy Losses
In calculating the various parameters, the most important energy losses due to elastic and inelastic electron collisions with the corresponding species have been taken into consideration. We expect that the energy losses coming from the electron collisions with N2O are important whenever it is not severely dissociated. The collisional energy losses in the N2O case, noted , are given by
As we threat here a molecule, energy losses by electron impact due to elastic scattering and to ionization and dissociation of the ground state and also to excitation at least of the lower vibrational and electronic excitation states have in general to be taken into account. For the N and O subproducts, electronic excitation, elastic scattering, and ionization are composing the corresponding energy loss terms. Energy losses from the atomic and molecular ions were not considered at this stage, as we are here dealing with relatively lowly ionized plasma. For the highly ionized “core” region of HPTs the Landau damping approximation can be used, as was also the case in .
Collisional energy losses for the N2O molecule following equation (9) are shown in Figure 7 in comparison with those of N2, N, O2, and O species. Energy losses for N2O calculations include those due to elastic collisions, three vibrational states, three electronic excited states, and two dissociation processes. Importance of introducing enough vibrational and electronic excitations as well as the relevant dissociation processes has been demonstrated. Here, the first dissociation process corresponds to the reaction no. 2 of Table 2 leading to the O compound in its first ground state 3P, whereas the second one corresponds to reaction no. 3 with the O atom in another ground level 1D.
In what concerns N2 species, calculated values showed the significant influence of the two first vibrational and two first electronic states of N2 on the overall value. Results vary considerably also when including one, two, and three dissociation processes. We also investigated the relative influence of the eight lower vibrational states on the results and we observed that including five vibrational levels in the calculations gives a satisfactory result, very close to the one with eight states. For the energy losses coming from electron collisions with N, we included excitation to two ground levels, N(2D) and N(2P), and to four excited states. Results agree well with those obtained in .
Our collisional energy losses of O2 species, coming from the electron collision with O2, were compared to those of Gudmundsson  as quoted in [1, page 80], showing a good agreement. This was somehow expected, as we used some of the existing rates, also used in .
In comparing values corresponding to the five species N2O, N2, N, O2, and O illustrated in Figure 7, we observe that the values for the N2O molecule are very near to those corresponding to O for the low , while they become close to those of N2 for high . While we evaluated values for various species , it has to be stressed that each level population constitutes only a factor in the sum corresponding to the total collisional energy loss calculation (see (2) of Section 2).
For energies lower than 8 eV, which are often of interest here, the values of N2O become more and more low than those of N2. In the low temperature region they are quite comparable to the values corresponding to O2 and become close to those of O for very low . For high energies (near to 100 eV), the value is close to the one of N2 as it was expected. Indeed, for high energies the values tend to the ionization energy plus a contribution of the dissociation energy, as the dissociation thresholds are often lower than the ionization ones. Globally, we can say that the values around the 1 eV to 2 eV region are mainly due to the vibrational excitation processes, elastic processes playing also an important role for low energies; the values in the 3–8 eV region are mainly due to the electronic excitation processes and in the 8 eV to 100 eV region they are due to both electronic excitation and dissociation processes.
Electronic ionization processes have been introduced in Section 3. Their participation in the overall energy loss was found considerable in all the energy regions, with their rates being present in terms belonging to equations analogous to (9), adapted for the N2, N, O2, and O species.
5. Regimes of N2O Discharges
Taking into consideration existing experimental and theoretical results in conjunction with those of our GM, the presence of the N2O and its products in the plasma can be roughly described by distinguishing the following three main regimes.
(i) The Plasma Is Mostly Composed of N2O Molecules. This happens when the absorbed power is very low and/or the pressure is quite high. Sustained flow rates can lead to such a physical condition; compare . The exact ranges of values of power, pressure, and flow rates also depend on the device form factor and size. In this situation, the molecular properties of N2O and principally the excitation of electronic and vibrational levels, as well as the N2O ionization process, are of big importance in the overall description of the physical situation. Diminishing the flow rate constitutes a simple way to pass to the next case (ii).
(ii) The N2O Species Are Quite Dissociated in the Plasma. This is typically the case of a plasma reactor in an intermediate pressure regime, with both length and radius of 15 cm, for absorbed powers varying from 250 to 500 W in presence of a flow rate typically of 60 sccm. N2 and O2 species are also within the main compounds of the plasma besides N2O. Such a situation, studied here with our GM, was also previously addressed by Shutov et al. . Our GM results for this case are comparable to those of , which are discussed and compared with ours in Section 6. A quite similar situation case is encountered in the “mantle” region of a relatively low absorbed power HPT; say of 100 W or less. The corresponding flow rate is about 12 sccm and the pressure of a few mTorr. This similarity of the low power HPT with those of the PR physical conditions prevailing here is partially due to the small radius of the former, around 1 cm, leading to a reduced total plasma volume. We estimate that low power absorption in the “mantle” region of a HPT corresponds to a situation where the PR plasma absorbs an intermediate amount of power (150–500 W) in a big volume. The expected and the ionization and dissociation percentages of the main constituents as well are then comparable.
Concerning the dissociation of the main N2O products, namely, N2 and O2 species, leading to nitrogen and oxygen atomic subproducts, it is found to become important with diminishing pressure. Specifically, products of N2 dissociation have been studied in detail recently [12, 17] in two typical cases of PR. A N2 dissociation of around 50% was found for a pressure of 5 mTorr. Dissociation was found to decrease with pressure to reach about 5% to 10% at 20 mTorr.
(iii) The N2O Species Are Almost Totally Dissociated. For high absorbed power (e.g., in the HPT “core” region similar to this of Ar feeding case studied in ), the ionization degree may become very high. However, the ionization degree may remain low if the flow rate is high. Hence, situation (iii) is typical for high absorbed power and low pressure regimes associated with low flow rates. In such a situation, the plasma becomes mainly a high power or/and low pressure N2/O2 plasma under the influence of electron collisions with heavy particles and notably of those leading to dissociation. Therefore, electronic collisions involving the N2 and O2 products gain importance. With the latter having a low dissociation energy (, ) the atomic oxygen may become particularly abundant. The N2 dissociation products may also appear in significant amounts, especially for high , due to its higher dissociation energy (, for the primary dissociation mechanism leading to N(2D) + N(4S) fragments, ). N2 and O2 species abundances vary considerably following their reformation on the wall depending on the device geometry and the material of the wall.
Although becoming more important in (iii), N2 and O2 dissociation is already present in conditions like those described in (ii). As the O2 dissociates easier than N2, atomic oxygen lines are commonly observed in spectra acquired in plasmas under such conditions together with the intense molecular N2 bands (see ). The N2 bands and the atomic O lines become more pronounced when plasma conditions pass from type (ii) to type (iii), although in conditions pertaining to high power the N2 molecules are quite dissociated. Under the aforementioned (ii) and (iii) conditions, reactions involving the N2 and O2 products and their excited states and and also their subproducts both in ground and excited states (mainly N, N*, O, O*, and O−) are important. In view of its preponderance in the N2O molecule, nitrogen becomes the predominant species of the plasma, while atomic O is also quite present. The quantity of oxygen species admixture confers to the plasma significantly different global properties due to electronegativity, as illustrated in Figures 15 and 17, Section 8. Results corresponding to N2 have been obtained recently by Kang et al.  and by Thorsteinsson and Gudmundsson . We obtained similar results  for N2 plasma discharges by a dedicated GM.
A N2O fed plasma reactor at rather high pressures (about 0.5 Torr to 1 Torr) has been studied previously by Date et al. , investigating a plasma in conditions between our (i) and (ii) cases described previously. As the authors kept rather big flow rate values, the N2O was dissociated only in a small percentage. Atomic lines in the UV and especially in the VUV region are very important as they largely contribute to plasma cooling in various applications (see, e.g.,  for the Ar plasma case). Dissociative excitation of N2O leading to emission in the Vacuum Ultraviolet (VUV) spectral region was studied recently by Malone et al.  in an electron impact collision chamber. These authors identified the main N I, N II, O I, and O II lines in the wavelength region from 80 nm to 180 nm, with the most intense lines belonging to the N I species. Results of  illustrate the importance of plasma radiation in the VUV region, addressing atomic spectral lines from species formed after dissociation of the initial molecular N2O, N2, and O2 species. They concern plasma conditions of type (iii), as an electron gun furnishes a high power to a plasma confined in a low or intermediate pressure vacuum chamber. These conditions are similar to those expected to prevail in the “core” region of a HPT, with a high and considerable ionization degree.
When absorbed power increases, plasma is passing from conditions of type (i) to (ii) and to (iii) one, and the ionization percentage increases, leading to a high plasma. In this case, inclusion of more ionized species may become necessary, while the dissociation plays a very important role. The dissociation-recombination equilibrium is strongly related to the wall recombination processes. The latter depends greatly on the device geometry and wall material. In the GM, the wall material is described by the sticking coefficient, which is unfortunately often badly known.
Keeping in mind that the present work aims to characterize various plasma devices, it should be noted that throughout (i) to (iii) cases, inclusion of excited states in the GM (N2O* for high pressures and also , , NO* and N*, and O* for lower pressures/higher power) allows for comparison of the model results with experimental measurements based on Optical Emission Spectroscopy (OES) diagnostics. This was already made in the simpler case of Ar plasma OES, using an Ar GM in correlation with a C-R model. Both models are available and have been described elsewhere, [2, 62]. Also, puffing of gases in small amount can improve OES, verifying at the same time the GM results.
Preliminary measurements in different type of devices contributed to the corroboration of our theoretical estimations concerning rare gases and nitrogen plasmas. These include observations in an air fed plasma reactor  and in a capillary tube fed with Ar. Both experiments have been performed in the LPGP Laboratory of the University Paris-Sud in Orsay, France. Also, measurements have been made in an inductively coupled plasma (ICP) torch, fed with various gases, including rare gases (He, Ne, and Ar) and their mixtures and N2 (and its mixture with rare gases), and in air environment, available in the LAEPT Laboratory of the University of Clermont-Ferrand, France; see, for example, [4, 6] for Helium and  for Neon feedings. Spectra of Ar-air mixture (95–5%) were also obtained in an HPT build in the CISAS institute of the University of Padova, Italy, in the frame of the HPH.com project of the EC . Although none of these plasmas concern N2O feeding, they contained a significant number of common products. Consequently, nitrogen and oxygen spectra acquired in air discharges can be comparable to those encountered in N2O fed plasmas.
6. Results of GM for N2O Plasma Reactors
In order to compare our results for N2O plasma reactors with experimental and theoretical ones existing in the literature, we calculated GM results in conditions similar to those chosen by Shutov et al.  for a PR of length and radius , fed with a flow rate of . In this experiment, the gas temperature was considered to be and the absorbed power was varied from up to 500 W with a fixed pressure of 4 mTorr.
6.1. Variation with the Pressure
Results of our GM in conditions similar to those of  and for a pressure varying from 1 mTorr up to 100 mTorr are shown in Figures 8 and 9, which report species densities and (where stands for all the encountered species), and in Figure 10, which reports the electron temperature , the ionization percentage, the remaining N2O percentage, and the electronegativity. For calculations corresponding to Figures 8, 9, and 10 the absorbed power was fixed at 300 W and the flow rate at 60 sccm. We also varied the pressure for higher absorbed powers. The obtained results vary with the pressure in a similar way.
Our results for and contained in Figures 8 and 9 show that the main constituents of the plasma are here N2, O2, N, O, and N2O. For pressures higher than 4 mTorr, N2 and O2 are the prevailing species. For low pressure, atomic N and O are present in a very important amount, but for 100 mTorr their densities become correspondingly between three and one orders of magnitude lower than the densities of N2 and O2. The N2O density increases slowly up to 10 mTorr and faster for higher pressures. The remaining N2O percentage decreases with the pressure (see Figure 10). This effect is due to the fact that while the flow rate remains constant the pumping efficiency must increase for low pressures in order to maintain a lower gas density. Hence, the residence time is lower for low pressure and N2O tends to be less dissociated even if the is higher. This is illustrated in Figure 10. On the opposite, N2 and O2 species are less dissociated for high pressures because their O and N products form again N2 and O2 on the wall in a very important amount; hence the pumping has a less pronounced effect on them as explained elsewhere . For all pressures, the sum of the nitrogen atoms contained in the totality of the calculated species is twice the sum of the oxygen ones, as all nitrogen and oxygen species come from the decomposition of N2O and the pumping is considered to be the same for all species. Concerning the NO species, densities are much smaller than those of the other neutral molecular densities, because the rate coefficient of reaction no. 4 of Table 2 is much smaller than the one of reactions nos. 2 and 3 of the same table. Also, NO is destroyed by collisions with N and O, which are present in considerable amount (reactions nos. 8 and 9 of Table 2). The vibrational states of N2 are quite populated. This is illustrated with the first vibrational state density, which is given separately in Figure 8, because it is the most populated among the excited ones. Inspection of Figure 8 indicates that 20% of N2 is typically expected to be in the first vibrational excitation state. Concerning the charged species, we see that the is slightly decreasing with pressure, while the ionization percentage is drastically decreasing, up to three orders of magnitude (see Figure 10). Our calculations show that and increase with the pressure, varying from 1 mTorr up to 100 mTorr. At the same time, densities of N2 and O2 increase by more than two orders of magnitude. This variation is also illustrated in Figures 8 and 9. Inversely, as we can also see in Figure 9, the N+ and O+ densities are important for low pressures. However, they diminish fast when the pressure increases and become between one and two orders of magnitude lower than those of and for a pressure of 100 mTorr. The O− density is lower than the one of O+ for 1 mTorr but increases continuously with pressure. Eventually, the O− density becomes comparable to the electron density and to the density for 100 mTorr with an electronegativity around 1 (see Figure 10). For all pressures the density is slightly lower than this of O−.
In order to compare our results for N2O, N2, O2, N, O, and NO species densities presented in Figure 8 with calculations and probe measurements obtained by Shutov et al. , values for 4 mTorr given in Figure 2 of  are reported in Figure 8. They are shown by big symbols, namely, triangles for N2, inversed triangles for O2, squares for N2O, full circles for NO, hollow circles for O(3P), hollow squares for O(1D), and diamonds for N. All the aforementioned species densities are theoretical. Moreover, the big pink empty triangle in Figure 9 indicates an experimental N2O+ value from ; because in  is about equal to , the measured values were taken as equal to the N2O+ ones throughout this reference. In our model we introduced explicitly many different types of ions; therefore according to the quasi-neutrality equation (1). We also repeat (indicated by small circles) the values of densities corresponding to 5 mTorr positions, by shifting of 1 mTorr the values attributed to 4 mTorr by Shutov et al. , as we believe that after dissociation the pressure in the experiment could be slightly higher than 4 mTorr. Throughout the figures of this section, theoretical values from  and experimental value are indicated by two black vertical arrows. In Figures 8 and 9, our results for species for which densities are also given in  are represented by small symbols. Consequently, data from  are noted with similar symbols to ours but bigger. Points of our results are joined by lines, only to ease the eye. Plain curves not associated with symbols represent our density results for ions (, N+, , O+, and O−) which were not given in . Our results are plotted with a thick pink dash-dotted line giving different values for electrons and N2O+, which was not the case for . Moreover, although we calculated densities of five vibrational states of N2, only this of the first one is represented in Figure 8 by a thin blue dashed line. In general, nitrogen densities are plotted in blue, whereas in Figures 8 and 9 oxygen densities are in red and the N2O, N2O+, and NO values are in black.
When comparing our results with those of Shutov et al.  in Figures 8 and 9 for the pressure of 4 mTorr (supposedly corresponding to a final pressure of around 5 mTorr), we see that N2O, N2, O2, and O(3P) results are in rather good agreement. Still, there is a slight difference on the N2 densities and a big discrepancy in the N densities. After introducing dissociation of the N2 product we found an important part of N2 being dissociated. We believe that this is the reason why we obtain N densities much higher than those of . Here, it should be reminded that the N2 (and O2) dissociation percentages strongly depend on the wall constitution, hence on the sticking coefficients used. In the present case, we used for N and for O. These values come from standard studies of PR [14, 15, 17] for walls composed of stainless steel with quartz windows. As in  lower values are proposed, we also tried these and they lead to higher dissociation percentages. Concerning the NO species, values similar to ours were obtained in . In fact, even if fewer N species destroying the NO (reaction no. 8 of Table 2) are present in  calculations, also fewer O(1D) species dissociating N2O towards NO (reaction no. 7 of Table 2) are present. Moreover, we used different rates for reaction no. 4 of Table 2 which also leads to NO formation. These three differences tend to equilibrate and we finally obtain NO densities close to those of . Concerning the charged species, the main observation is that the values given by our model are very similar to those measured in .
The electronegativity is also calculated by our model. Results are plotted in Figure 10 with plain blue lines. In Figure 10 the obtained N2O percentage is given in conjunction with the calculated plotted with a plain red line. is continuously diminishing with increasing pressure, as shown in Figure 10. The remaining N2O percentage is represented in Figure 10 by a black curve. For comparison, the values of  are also shown in Figure 10, by a red circle for the and by a black star for the remaining N2O percentage. We observe that the remaining N2O percentage is decreasing with the pressure as discussed previously. Plasma potential is also represented by a blue line.
6.2. Sensitivity of the Results to the Absorbed Power, Flow Rate, and Sticking Coefficients
Sensitivity of the results obtained for the same conditions as those of Figures 8 and 9, namely, a reactor of length and radius , around with a flow rate of , and an absorbed power for a gas temperature K, is addressed in Table 11. In this table, increase (decrease) in the obtained results is indicated by upper (lower) arrows. The number situated at the right of each arrow indicates the factor of increase (decrease) of the results. Table 11 corresponds to a pressure fixed at 5 mTorr.
|Values from  are included in first row(bold brackets)except for /.|
**Small peak at 40 sccm before decreasing.
Variation of the results when the absorbed power increases from 250 W up to 500 W is contained in the first row of Table 11. In this line of the table, we see that the is higher for an absorbed power of 500 W than it was for 250 W, as expected due to the increase in power absorbed by the plasma. Results for 300 W shown in Figures 8 and 9 lie within the values of the first row of Table 11.
N2O, N2, and O2 species are more dissociated when absorbed power increases, as is shown in column 2 of Table 11 (percentage of remaining N2O, is shown in this column instead of dissociations) and in columns 3 and 4 (dissociation percentages of N2 and of O2). Also, atomic species densities of the created N and O (composed of O(3P) and O(1D)) for 500 W are about the double of those obtained for 250 W. Note that in Table 11, and stand for the density of atomic nitrogen and oxygen formed in the discharge by the various dissociation processes. The corresponding variations of the electronic density, of electronegativity (), and of are also shown in columns 1, 5, and 6 of Table 11. Electron density, remaining N2O percentage, and dissociation percentages variations from Shutov et al.  are also given inside bold brackets in Table 11 for comparison. These are varying similarly to our results. It has to be noted that in results from , electron density was put equal to this of N2O+, while in our model we used the aforementioned quasi-neutrality condition. The two slightly different values of variation according to  are due to small changes in the experiment following the values. Besides the increase in both electron density and dissociation of N2, O2, and N2O with the absorbed power as shown in columns 3, 4, and 2 (remaining N2O density diminishes) of Table 11, the densities of all positive ions, not shown in Table 11, increase. However, it was found that N2O+ density decreases. The O− density slightly decreases, due to small increase in O− neutralization, whereas the O− formation by electronic impact for the conditions encountered here is diminishing. The calculated electronegativity (see column 5 of Table 11) is small and slightly decreasing, as expected for a pressure of 5 mTorr.