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  • 1
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Real time spectroscopic ellipsometry (RTSE) has been applied to study the nucleation, coalescence, and growth processes for ∼100–200 Å thick microcrystalline silicon (μc-Si:H) p-layers prepared by radio frequency (rf) plasma-enhanced chemical vapor deposition at 200 °C on amorphous silicon (a-Si:H) i-layers in the substrate/(n-i-p) device configuration. Analysis of the RTSE data provides the bulk p-layer dielectric function (2.5–4.3 eV), whose amplitude and shape characterize the void and crystalline Si contents in the p-layer. Among the parameters varied in this study of the deposition processes include the underlying a-Si:H i-layer surface treatment, the p-layer H2-dilution flow ratio, the p-layer dopant source gas and flow ratio, and the p-layer rf plasma power flux. Here we emphasize the differences among p-layer deposition processes using diborane, B2H6, trimethyl boron, B(CH3)3, and boron trifluoride, BF3, dopant source gases. We find that it is easiest to nucleate μc-Si:H p-layers immediately on the i-layer without any surface pretreatment when B2H6 is used as the source gas. In contrast, when B(CH3)3 or BF3 is used, a H2-plasma treatment of the i-layer is necessary for immediate nucleation of Si microcrystals; without pretreatment, the p-layer nucleates and grows as an amorphous film. For H2-plasma-treated i-layers, p-layer microcrystal nucleation at low plasma power is controlled by the catalytic effects of B-containing radicals at the i-layer surface, irrespective of the dopant source, whereas nucleation at higher plasma power is controlled by the bombardment of the i-layer by Si-containing ions. Under high power plasma conditions using BF3, dense single-phase μc-Si:H p-layers can be obtained over a wide range of the dopant gas flow ratio. In contrast, for B2H6 and B(CH3)3, such properties are obtained only over narrow flow ratio ranges owing to the relative ease of dissociation of these gases in the plasma. © 1999 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 2
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: In studies of hydrogenated amorphous silicon (a-Si:H) n–i–p solar cells fabricated by rf plasma-enhanced chemical vapor deposition (PECVD), we have found that the maximum open circuit voltage (Voc) is obtained by incorporating p-type doped Si:H layers that are protocrystalline in nature. Specifically, these optimum p layers are prepared by PECVD in the a-Si:H growth regime using the maximum hydrogen-to-silane flow ratio possible without crossing the thickness-dependent transition into the mixed-phase (amorphous+microcrystalline) growth regime for the ∼200 Å p-layer thickness. The strong dependence of the p-layer phase and solar cell Voc on the underlying i-layer phase also confirms the protocrystalline nature of the optimum Si:H p layer. © 2002 American Institute of Physics.
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  • 3
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 80 (2002), S. 2666-2668 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Real time spectroscopic ellipsometry has been applied to develop extended phase diagrams that can guide the deposition of hydrogenated silicon (Si:H) thin films for highest performance solar cells. Previous such studies have shown that optimization of amorphous Si:H intrinsic layers by rf plasma-enhanced chemical vapor deposition (PECVD) is achieved using the maximum possible H2 dilution of SiH4 while avoiding a transition to the mixed-phase (amorphous+microcrystalline) growth regime. In this study, we propose that optimization of amorphous Si:H in higher rate rf PECVD processes further requires the largest possible thickness onset for a surface roughening transition detected in the amorphous film growth regime. © 2002 American Institute of Physics.
    Type of Medium: Electronic Resource
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