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

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CHAPTER 4<br />

MINORITY-CARRIER LIFETIME MEASUREMENTS<br />

4.1 Quasi-Steady-State Photoconductance Decay<br />

One <strong>of</strong> the fundamental physical properties <strong>of</strong> a <strong>silicon</strong> <strong>solar</strong> cell is the minority-carrier<br />

lifetime. In practice, measurements on wafers yield an effective lifetime which can then<br />

be interpreted as a combination <strong>of</strong> <strong>bulk</strong> <strong>and</strong> surface recombination components. In order<br />

to do this correctly, the measurements <strong>of</strong> the effective lifetime must have a strong<br />

physical basis. Currently, there are three methods being deployed <strong>by</strong> the PV-Si industry<br />

for lifetime measurements: quasi-steady state photoconductance decay (QSSPCD),<br />

photoluminescence mapping <strong>and</strong> microwave reflection. In this thesis, QSSPCD was used<br />

to measure the minority-carrier lifetime <strong>of</strong> PV-Si.<br />

For long-lifetime wafers, the transient method (measurement after the light is<br />

extinguished) is preferred since it does not require knowledge <strong>of</strong> the photogeneration in<br />

the sample (reflection <strong>and</strong> absorption <strong>of</strong> photons in the sample) or the excitation<br />

wavelength. The QSS method has been found to be useful for lower-lifetime materials<br />

that are <strong>of</strong>ten used in the production <strong>of</strong> PV <strong>cells</strong>. The QSSPCD technique has been<br />

developed <strong>by</strong> Sinton [100]. This award-winning technique uses inductive coupling<br />

between a small coil that is placed under the sample platform <strong>and</strong> the sample under test.<br />

The frequency used is 10 MHz, <strong>and</strong> the light source is a very long duration (several<br />

milliseconds) flash lamp. The setup involves a zeroing procedure that accounts for the<br />

dark conductivity <strong>of</strong> the sample. The user also inputs the estimated carrier concentration.<br />

The sensor coil detects the photoconductivity produced <strong>by</strong> the flash lamp, <strong>and</strong> the<br />

interfaced computer processes the data. A highly calibrated onboard <strong>silicon</strong> cell, that is<br />

65

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