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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 80 (1996), S. 6142-6147 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Oxygen rf glow discharges between parallel plates were numerically analyzed by using the relaxation continuum model. The result at a frequency of 13.56 MHz, sustaining voltage of 150–350 sin ωt V, pressure of 0.15–1.0 Torr, and stainless steel surface, shows that O2(a1Δg) has a number density that is an order of magnitude larger than that of atomic oxygen. The plasma density as a function of pressure has a maximum at about 0.2 Torr, and decreases with increasing pressure due to the increase in the net rate of associative detachment from O− by O2(a1Δg). The comparison between the discharges in two surface materials, stainless steel and copper, indicates that the number densities of O2(a1Δg) and atomic oxygen strongly depend on the surface loss probability, and that consequently the plasma density is also changed by replacing the surface material. © 1996 American Institute of Physics.
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 77 (1995), S. 6181-6187 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The spatiotemporal structure of O2 rf discharges between parallel plates at 13.56 MHz is investigated by using the relaxation continuum model. The results for pressure of 0.5 Torr and the sustaining voltage of 75–200 sin ωt V are studied by considering the elementary particles, O+2, O+, O−2, O−, electrons, and O in O2. In these conditions, atomic oxygen, formed by the dissociative electron impact in O2 with density of ∼1014 cm−3, plays important role to the rf structure through the associative detachment process. That is, the expanding characteristics of the sheath width unique to the O2 rf discharge are realized with increasing the sustaining voltage. The validity of the numerical result is demonstrated with the spatiotemporal structure by the measurement by the spatiotemporally resolved optical emission spectroscopy. The flux of each particle to the electrode is also discussed. © 1995 American Institute of Physics.
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 89 (2001), S. 7756-7763 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The basic characteristics of a micro-cell plasma in a gas mixture sustained by a high-frequency voltage source with a ring-shaped electrode are described in this article. The key to maintaining a microcell plasma is to reduce wall loss and increase plasma production. The advantage of a gas mixture of Ne/Xe is the increase of the plasma production rate in a low electric field compared to that in pure gas. As a result, a microcell plasma can be sustained by a lower applied voltage by using a gas mixture of Ne/Xe under the same power condition as compared with that in pure Xe. © 2001 American Institute of Physics.
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 72 (1992), S. 3323-3329 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A numerical model based on the Boltzmann equation is proposed to simulate the physical etching by energetic particles in the sheath region of the discharge. The local profiles of the two-dimensional velocity distributions of ions and fast neutrals in the gas phase are calculated in a radially uniform discharge, under a set of collision cross sections, for external parameters: sheath voltage and width, ion current density, and pressure. A case study is performed in a dc abnormal glow discharge in Ar having a masked Al electrode. The time evolution of the etching profile is simulated as a result of the physical interaction between the surface and energetic particles from the gas phase. This enables the estimation of the etch rate and anisotropy for ions and fast neutrals. A great advantage of the present numerical procedure is that it is free from stochastic fluctuations and the lengthy central processing unit time found in particle simulations.
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  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 71 (1992), S. 2143-2150 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Radio frequency discharges at 13.56 MHz in CH4(100%), CH4(10%)/H2, and H2(100%) are investigated by time- and space-resolved optical emission spectroscopy. The spatiotemporal net-excitation profile of H(n=3) is presented and discussed. The absolute value of the net-excitation rate, the emission intensity, and the density of the optically allowed electronic excited species are also measured. The self-quenching rate of H(n=3) and CH(A) by H2 and CH4 are estimated and compared with the previous works. The importance of the quenching of CH(A) by atomic hydrogen is also discussed. Excitation by very high-energy electrons is shown from the difference of the emission profile between Hα and H2(d3Πu→a3Σg+) in H2 at 100 kHz.
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 74 (1993), S. 4907-4914 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The frequency dependence of the sustaining voltage in a radio frequency discharge has been investigated under minimum sustaining and constant power conditions in Ar. In addition to the well-known feature that the sustaining voltage is high at low frequency and low at high frequency, the difference between monoatomic and polyatomic gases is recognized. The phase shift between voltage and current at 1 Torr decreases with increasing frequency above 500 kHz. This results from the electron density modulation having a delay with respect to the applied voltage. The phase shift at high frequency increases with increasing applied voltage, due to the balance of drift and diffusion fluxes of electron. The spatiotemporal net excitation rate of Ar(3p5) was measured at 100 kHz, and 4 MHz, and 13.56 MHz. It is reconfirmed that the sustaining mechanism of the discharge at low frequency is ionization by secondary electrons from the electrode, while at high frequency it is ionization due to reflected electrons by the oscillating sheath. At middle frequency, 4 MHz, the sustaining mechanism drastically varies with input power density from the high-frequency type to the low-frequency type.
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 73 (1993), S. 2163-2172 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Space- and time-resolved emission spectroscopy was applied to obtain information on the kinetics of radio-frequency (rf) discharges for 100 kHz, 800 kHz, and 13.56 MHz in SF6. Emission lines of fluorine and SFx radical were used, but particularly useful were the second positive (2+) and the first negative (1−) bands of nitrogen. The two nitrogen bands gave an opportunity to separate, respectively, the behavior of middle-energy (11–20 eV) and higher-energy (above 20 eV) electrons. Development of double layers was studied from the excess emission close to the anode due to an increased electric field. Also observed were the emission from the bulk and emission due to the electrons accelerated in the instantaneous cathode sheath. The development of these features was followed as a function of the pressure, frequency, and power.
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  • 8
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Radio frequency glow discharges in SiH4(50%)/H2 at 13.56 MHz and 100 kHz have been investigated by using time- and space-resolved optical emission spectroscopy. The relative net-excitation rate is obtained by deconvolving the spatiotemporal emission profile considering the influence of the radiative lifetime. From the results, we infer the behavior of electrons with energy greater than the threshold energy for the dissociative excitation and we discuss the discharge structure. Lines of SiI(4s 11P0→3p 21D), SiH(A2Δ;v'=0→X2Π;v‘=0), Hα, and H2(d 3Πu→a 3Σ+g) are selected for observation. It is concluded that there exists a considerable population of negative ions compared with positive ions, which has not been previously proposed in high-frequency discharges in SiH4 because of the small degree of electron attachment. At 13.56 MHz, the optical emission oscillates at 2ω in the bulk plasma region, in addition to the emissions at the plasma-sheath boundaries. It implies that the field in the bulk is strengthened by the external sinusoidal field to make up for the loss of electrons by electron attachment. The bulk field is estimated at 69 sin(ωt) V cm−1 from V-I characteristics. The existence of a double layer by the modulation of electrons is strongly suggested even in a high frequency at 13.56 MHz. At low frequency (100 kHz), a double layer is observed, which is formed by the large modulation of negative and positive ions. Consequently, excitation by electrons accelerated in the field at the double layer is observed in addition to excitation by secondary electrons from ion bombardment. Consideration of the role of negative ions in high-frequency SiH4 discharges at 13.56 MHz is necessary to understand the discharge structure of the silane plasma and the deposition of the hydrogenated amorphous silicon.
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  • 9
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Electrical characteristics of rf discharges in SF6 and in its mixtures with N2 were experimentally investigated. In addition space- and time-resolved emission spectroscopy was used to gain a better understanding of kinetics of processes leading to various observed characteristics. A complicated dependence of minimum sustaining voltage on frequency was observed with a peak at 3 MHz. It was explained as the result of transition from the conditions where discharge is sustained by ionization in the bulk and the double-layer region to the conditions where secondary electron yield makes a large contribution. Another possible explanation is the one invoking transition from the conditions where at high-frequency double layer is formed by electron modulation to the condition where a double layer is formed by positive and negative ions. In voltage-current dependencies at 13 MHz two distinct regions were observed similar to the α to γ transitions observed for electropositive gases. Ionization by secondary electrons, however, is not supported by spatiotemporal emission measurements, thus explanation may be sought in different processes such as development of double layers and increased field in the bulk. The current-to-voltage phase is much smaller than in electropositive gases, thus the discharge appears more resistive. For a range of operating conditions the phase even becomes inductive due to negative ion inertia.
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  • 10
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 56 (1990), S. 818-820 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The diagnostic technique of the rf glow discharge at 13.56 MHz is developed by using the spatiotemporally resolved optical emission spectroscopy. New experimental evidence that the temporal excitation rate at the sheath peaks in phase with the maximum of the total current is obtained in a parallel-plate geometry at 13.56 MHz in CH4(10%)/H2 under a typical condition of the plasma chemical vapor deposition of amorphous carbon film at room temperature.
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