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Chapter 8 Thin Film Solar Cells June 17, 2022

Chapter 8 Thin Film Solar Cells July 12, 2015

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Page 1: Chapter 8 Thin Film Solar Cells July 12, 2015

Chapter 8 Thin Film Solar Cells

April 21, 2023

Page 2: Chapter 8 Thin Film Solar Cells July 12, 2015
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Requirements for suitable materials

Doping and charge transport are more difficult for a-Si.

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Amorphous silicon

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Absorption

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Doping

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Low doping efficiency means

• P is much less than ND.

• Femi level moves toward the defect level in the center of band gap and majority carrier activation energy is large.

• The built-in potential is less.

• In addition, recombination centers for minority carriers increases.

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More explanations

• Vbi = [EFn(wn) – EFp(wp)]/q,

• Vbi = φn –φp = -(Ei – EF)/q – [-(Ei – EF)]/q

= kTln[NAND/ni2]/q

Pp0 = pn0exp[qVbi/kT]

Voc could not increase by increasing ND or N

A. kTEEc

FceNn /)(

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Transport

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The small diffusion length of a-Si is attributed to the small mobility of the carriers. Mobility of c-Si is 0.5 m2V-1s-1 for electron with low doping.

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Stability

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C; absorption by defects of dangling bond.

B: absorption by Urbach tail due to variation of bond length and angle.

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the i-region thickness to around 0.5 μm.

Amorphous Silicon Solar Cell Design

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The p-i-n solar cell device physics

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Fabrication of a-Si solar Cells

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Light induced degradation:

The Staebler Wronski effect is the most important barrier to widespread use of a-Si solar cells. Light-induced degradation is stronger

Strategies to improve a-Si cell performance

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where EF is above EC or below EV.

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