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Color online Spatial amplifications for ionization wave modes as a function of wavenumber at different discharge currents. 

Color online Spatial amplifications for ionization wave modes as a function of wavenumber at different discharge currents. 

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Article
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A quasi-logistic, nonlinear model for ionization wave modes is introduced. Modes are due to finite size of the discharge and current feedback. The model consists of competing coupled modes and it incorporates spatial wave amplitude saturation. The hysteresis of wave mode transitions under current variation is reproduced. Sidebands are predicted by...

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Context 1
... Fig. 5. The model parameters in Eq. 1 can be derived from experimental results. The spatial amplification can be derived from measurements see Fig. 5. Since the dispersion of ionization waves f = f is accessible as well, the wave numbers can be determined and the amplification i can be expressed as a function of wave-number i, which is shown in Fig. ...
Context 2
... Fig. 7 indicates, the spatial amplification is well ap- proximated by a unimodal function in the considered param- eter range. The maximum spatial amplification becomes positive above a critical current supercritical Hopf bifurca- tion. Increasing the discharge current leads to an increased maximum and a shift of the maximum to smaller wave ...
Context 3
... is instructive to consider the spatial amplifications for fixed wave numbers under current variations by Fig. 7. First, it is evident that currents exist for which the three wave modes considered have a positive amplification. For a given wave mode an increase of the current results in a minimum and maximum current for which i 0. This is the current region for which a self-excited wave can exist. In between the limiting currents, a current for ...

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Citations

... Recent experiments on ionization waves [69][70][71][72][73][74] provide experimental spatiotemporal patterns with light-emission fluctuations similar to that shown in figure 4, providing independent experimental validation of our numerical results. The impact of the dust particles on the stabilization of the striations has been studied in [75] in the PK-4 system as well as by means of fluid type numerical discharge modeling. ...
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... Ionization instability accompanied by striation was obtained in [22] in nitrogen. Attempts to build a physical model of the spherical ionization instability were made in [23][24][25]. Nevertheless, it was not yet possible to fully understand the conditions for the emergence and maintenance of this type of gas discharge. ...
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... [24][25][26][27][28][29] Presently, such approaches have also found acceptance in treating localized structures and nonlinear properties of ionization instabilities in dc-driven gas discharge systems. [30][31][32][33] The purpose of the present work was to solve the problem formulated by Pekarec, namely, to develop, around the strategy proposed in Ref. 22, modern calculation techniques for basic properties of positive-column plasma; to provide a uniform description to the conditions of spatial homogeneity of plasma column; to consider, within a unified approach, the formation of striations and the emergence of jumps and hysteresis in the current; to place the physical states and properties of positive-column plasma of noble d.c. gas discharges in their proper framework (How does all this fit into the general scheme of things?); and to investigate into the various plasma states more deeply than ordinary deductions from experimental observations usually go. ...
... The origin of the various terms in (33) can be figured out considering the following. By way of illustration, consider the case in which the ionization is caused by step plasma reactions. ...
... However, it can be used for a good approximation not only over these regions, but, surprisingly, for the analysis of regions numbered 1 and 2 as well. In the latter case, the condition r d ≥ R is valid, electrons would be partially 'free' and quasi-free and we should take into account only the first terms of Eq. (33). Equations (33) and (57) contain some basic properties of 1 and 2 regions, that is to say that the processes under review is primarily responsible for the properties of the gas discharge. ...
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... Striations originate due to growing instability during the ionization process, which may be caused by step-wise ionization when metastable atoms are produced by electron impact decay as a result of diffusion to the wall. 13 In earlier studies, ionization wave in dc discharge of rare gases 14,15 have been extensively studied. Striations depend on system parameters, i.e., discharge current, the neutral gas pressure, length and diameter of the plasma column etc. ...
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