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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 64 (1988), S. 4384-4397 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Using space-time-resolved laser-induced fluorescence and plasma-induced emission spectroscopy, we find metastable and dissociation product densities to vary nonlinearly as Ar is diluted with SF6, Cl2, and BCl3. Because rare gases are relatively inert in the ground state, it is often assumed that rare gases change discharge chemistry through metastable interactions. Surprisingly, the measured changes cannot be accounted for by considering only direct metastable energy transfer. A model is proposed in which Ar metastable states indirectly enhance molecular dissociation by enhancing the ion density via Penning reactions; the increase in ion density in turn causes an increase in the dissociative recombination rate. This rate varies nonlinearly with concentration because both ion-producing metastable states and recombining electrons are quenched by addition of the attaching, molecular gases. The model satisfactorily explains discharge changes when small concentrations of molecular gases are added to an Ar discharge. Less well understood are changes over a broader concentration range, where dissociation and excitation rates decrease with decreasing Ar concentration because of electron attachment and cooling.
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 64 (1988), S. 598-606 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Although rate coefficients are essential ingredients in modeling chemical processes such as chemical vapor deposition and plasma etching, the values measured as a function of temperature under well-defined equilibrium conditions may be inappropriate for use in models of nonequilibrium systems. For this reason, it is important to have measurements of in situ rates that can be used as input parameters or can provide stringent tests for reactor simulations. Using time-resolved plasma-induced emission and laser-induced fluorescence spectroscopy, we measured quenching rates for Ar metastable states in radio-frequency discharges through mixtures of Ar and the molecular gases SF6, Cl2, BCl3, and N2. After verifying the validity of modulation spectroscopy to measure in situ rates, the effects of discharge power, pressure, and flowrate are investigated. The most important effect occurs when the discharge power is increased; the decline in quenching rates with increased power is attributed to increased molecular dissociation that produces products with lower collision cross sections.
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 72 (1992), S. 3934-3942 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Collisionless orbit theory is used to model isolated particles in low-pressure discharges with and without the presence of negative ions. The key results are as follows: (1) Debye–Hückel theory works well for approximating the potential profile around the particle, and (2) the size of the sheath around the particle is determined by a Debye length that results from linearizing the Poisson–Vlasov equation. These results are valid as long as the ratio of particle radius to Debye length is small and the ratio of Debye length to mean free path is small.
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  • 4
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 56 (1990), S. 1022-1024 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Particle-in-cell simulations of radio frequency glow discharges between parallel-plate electrodes were performed to test the role of secondary emission at applied frequencies above the ion plasma frequency. With the secondary electron emission coefficient set to zero, the high-energy tail of the electron energy distribution function in the center of the glow is modulated at the applied frequency, and these energetic electrons show substantial anisotropy. In addition, a pulse of ionization propagates across the glow, correpsonding to the directed velocity of the high-energy electrons in the center of the glow. These high-energy electrons originate at the plasma-sheath boundary and appear to be the result of sheath heating.
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  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 76 (1994), S. 5646-5660 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A comparison is made between particle-in-cell model (PIC) and fluid model simulations of a radio frequency (rf) gaseous discharge containing a helium model gas. The agreement in the discharge properties predicted by the two models is examined over a range of pressures and applied voltages. It is found that there is quantitative agreement in the overall discharge behavior predicted by the PIC and fluid simulations at pressures above 100 mTorr and applied voltages up to 800 V. With the exception of the ion energy at the electrodes, the two models also agree in their prediction of the scaling of discharge properties as a function of the applied voltage. Below 100 mTorr, disagreement in the period-averaged electron heating predicted by each model leads to differences in the predicted discharge properties. The estimate for the electron power input prediction can be improved in the fluid simulation by including an analytic expression for stochastic heating in the electron energy balance equation.
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 73 (1993), S. 7195-7202 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Classical scattering theory is used to calculate momentum-transfer cross sections between positive ions and isolated particulates in glow discharges for several model particle sheath potentials. Cross sections calculated from a potential profile obtained using self-consistent orbit (Poisson–Vlasov) theory, an attractive screened Coulomb potential, and an attractive cutoff Coulomb potential are compared. At high ion energies, all model potentials result in the same cross-section dependence on ion energy. At low ion energies, however, the cutoff Coulomb potential gives a cross section too low by about a factor of 10. The screened Coulomb potential and Poisson–Vlasov theory potential result in momentum-transfer cross sections equal to within 30% over the entire range of ion energies. An approximate analytic expression for the momentum transfer rate coefficient is given for order of magnitude estimation of the ion drag force.
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 80 (1996), S. 2614-2623 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A key need for the development and testing of models suitable for chemically active, low pressure plasmas is detailed comparisons between model predictions and experimental measurements. In this paper, a two-dimensional, axisymmetric fluid model of an inductively coupled plasma is described, and model predictions are compared to the experimental measurements of P. A. Miller, G. A. Hebner, K. E. Greenberg, P. D. Pochan, and B. P. Aragon [J. Res. Natl. Inst. Stand. Technol. 100, 427 (1995)] of electron density, electron temperature, and plasma potential. Comparisons between model predictions and experimental measurements were made in argon and chlorine discharges. Qualitative to semiquantitative agreement between the model predictions and experimental diagnostics was observed, suggesting that assumptions made in the model are reasonably accurate. © 1996 American Institute of Physics.
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  • 8
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 78 (1995), S. 2279-2287 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The most important forces that influence the motion of particles in a glow discharge plasma are the electrostatic force, the ion drag force, the neutral drag force, thermophoresis, and gravity. In this article we present a transport model that predicts the distribution of particles in plasma reactors in terms of the fundamental forces that act on the particles. We compare the model predictions to experimental measurements of particle distributions in a rf parallel plate plasma reactor. © 1995 American Institute of Physics.
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  • 9
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 77 (1995), S. 1263-1274 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Molecular dynamics simulations were performed on low-energy argon-ion bombardment (200, 50, and 20 eV) of silicon layers with varying amounts of fluorine incorporated. At low fluorine incorporation in the layers (F/Si〈0.5), only physical sputtering was observed, although the physical sputtering yield increased compared to pure amorphous silicon. At higher levels of fluorine incorporation into the silicon layer, ion impact resulted in the formation of weakly bound SiFx (x=1–3) species in the layer. This phenomenon appears to be similar to chemical sputtering as defined by Winters and Coburn [H. F. Winters and J. W. Coburn, Surf. Sci. Rep. 14, 164 (1992)]. The overall yield, due to both physical and chemical sputtering, was found to follow a square-root dependence on ion energy. The threshold ion impact energy for the formation of weakly bound species in heavily fluorinated silicon layers extrapolated to ≤4 eV, and for physical sputtering to about 20 eV. The simulations imply that the source of the ion-neutral synergism in ion-assisted etching occurs on the collision cascade time scale (∼10−12 s) with the creation of these weakly bound species. The overall rate determining step for ion-assisted etching, however, is often a much slower process involving thermal desorption, chemical reaction, or diffusion. This difference between the source of the ion-neutral synergy (creation of weakly bound species in 1 ps or less) and the rate determining step (often on much longer time scales) has probably contributed to the confusion that has surrounded discussions of the mechanisms of ion-assisted etching. © 1995 American Institute of Physics.
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  • 10
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 78 (1995), S. 6604-6615 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We report results from molecular-dynamics simulations of F+ and Cl+ impact of silicon surfaces, at normal incidence and over a range of energies (10, 25, and 50 eV). The halogen content of the silicon layer increases with halogen fluence, and the simulations are continued until an apparent, quasisteady state in halogen coverage has occurred. Although in some cases the quantitative results differ, F+ and Cl+ are qualitatively similar in steady-state halogen coverage, depth of penetration, etch mechanisms, and etch yield dependence on ion energy. In both cases, a mixed halogenated silicon layer forms, with a substantial degree of surface roughness (∼1–2 nm for 25 or 50 eV ions). At 10 eV for both F+ and Cl+, the apparent steady-state coverage is about 2 equivalent monolayers and the depth of F+ (Cl+) penetration is about 15 A(ring). For 25 and 50 eV ions, the corresponding coverage (approximately independent of ion energy and type) is about 3 monolayers. The corresponding depth of penetration is about 35 A(ring). The silicon etch yield is a function of ion composition and energy: These values ranged from 0.25 at 10 eV to 0.45 at 50 eV for F+ and from 0.06 at 10 eV to 0.14 at 50 eV for Cl+. Simulations revealed that the dominant Si etch mechanism and the silicon etch product stoichiometry changed with ion energy. In addition to physical and chemical sputtering, an additional etch mechanism has been observed in the simulations. We term this mechanism direct abstractive etching (DAE). In DAE, an incoming F+ reacts with a surface SiFx, creating a volatile SiFx+1 that leaves the surface with nonthermal energies, similar to physically sputtered products. At 10 eV F+, DAE accounts for ∼80% of the etched species, but at higher energies this mechanism is less likely. DAE is observed for Cl+ impact as well. Comparison of simulation predictions to available experimental results shows at least qualitative agreement, suggesting the approximations made in the simulations are reasonable. © 1995 American Institute of Physics.
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