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Surface and bulk passivation of multicrystalline silicon solar cells by ...

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LIST OF FIGURES<br />

(Continued)<br />

Figure<br />

Page<br />

2.7 The calculated reflectance <strong>and</strong> absorbance spectra <strong>of</strong> a Si <strong>solar</strong> cell operating in<br />

air (thick lines) <strong>and</strong> in an encapsulated module (thin lines). The nonabsorbing<br />

nitride is assumed to have n=2 for air <strong>and</strong> n=2.2 for module operation [42] ..... , 31<br />

3.I B<strong>and</strong>-to b<strong>and</strong> recombination in a direct b<strong>and</strong>-gap semiconductor [76] ..... , . , , . , . 39<br />

3.2 Schematic diagram <strong>of</strong> impurity-related energy levels within the forbidden gap <strong>of</strong><br />

a semiconductor. Levels are labeled as to whether the defect is likely to be a trap<br />

or a recombination center according to the SRH model 40<br />

3.3 Charge distribution <strong>and</strong> b<strong>and</strong> diagram at the Si-insulator interface under<br />

non-equilibrium.conditions. The non-equilibrium conditions are indicated <strong>by</strong> the<br />

separation <strong>of</strong> electron <strong>and</strong> hole quasi—Fermi levels ψ <strong>and</strong> ψ . Note the surface<br />

potential ψs is positive when the energy b<strong>and</strong>s bend down ......43<br />

3.4 Schematic diagram <strong>of</strong> a numerical algorithm for the calculation <strong>of</strong> surface<br />

recombination rates at the Si-insulator interface for given excess concentration<br />

at the edge <strong>of</strong> surface space region .[82] ................................... . ............. 46<br />

3.5 The calculated dependence <strong>of</strong> effective SRV (Seff on the fixed positive charge<br />

density. (Q) for different interface-state densities. The results are shown for<br />

two injection levels: (a) 1014cm-3 <strong>and</strong> (b) 1016cm-3 [84] 47<br />

3.,6 Calculated effective surface recombination velocity Seff for p-Si surface as a<br />

function <strong>of</strong> the injection level Δn in the quasi-neutral <strong>bulk</strong> for different values <strong>of</strong><br />

interface state density Dit. Input parameters: Doping concentration = 1 x 10 16<br />

cm-3 ; σn= 1x10-14cm2,.σp=1x10-16cm2; Qι= 1.3x10 11 cm-2 ..........................<br />

3.7 Measured Seff(Δn) dependence at the SiΝx -passivated surfaces <strong>of</strong> three 1.5 Ω cm<br />

FZ p-Si wafers. The SiNx films were fabricated with three different PECVD<br />

methods: low-frequency(I00 kHz direct) PECVD, high-frequency (13.56 MHz)<br />

direct PECVD, <strong>and</strong> remote PECVD [56] ,. 53<br />

3.8 Calculated dependence <strong>of</strong> Seff for n-Si <strong>and</strong> p-Si surfaces as a function <strong>of</strong><br />

injection level (Δn) for different. wafer resistivities. D it=5x10 10 cm2 eV-1 ,<br />

Q-1I0 1 . 1 cm2 54

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