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      <image:title>One Second QE</image:title>
      <image:caption>Mapper generates 3-D maps of EQE, R and IQE at each wavelength, as well as a Jsc map that is calculated from each EQE spectrum in real time.</image:caption>
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      <image:caption>Repeatability over 9 hours and 32,000 measurements.</image:caption>
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      <image:title>Electro &amp; Photoluminescence</image:title>
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      <image:title>ELE: Electroluminescence Excitation</image:title>
      <image:caption>Figure 1.  Schematic of traditional non-contact PLE apparatus.</image:caption>
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      <image:title>ELE: Electroluminescence Excitation</image:title>
      <image:caption>Figure 3. From H. Mackel and A. Cuevas, Solar Energy Materials and Solar Cells 71 (2002) 295-312.  Demonstrates the expected long-wavelength discrepancy between contacting, short-circuit spectral response technique and a non-contact photoconductance technique.</image:caption>
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      <image:title>ELE: Electroluminescence Excitation</image:title>
      <image:caption>Figure 4. The effect of DC bias light on the strength of the ELE emission signal.  Increasing the DC bias increases the gain of the EL emission ‘indicator light’.  Note that the ELE technique is full-spectrum, unlike traditional PLE, and wavelengths can extend to (or below) the bandgap: incident light does not enter the detection region, and so there is no crosstalk between the illuminator and the luminescence signal.  From references 9, 12.</image:caption>
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      <image:title>ELE: Electroluminescence Excitation</image:title>
      <image:caption>Figure 2.  A comparison of PLE vs QE for typical direct gap (left) and indirect gap (right) materials.  For indirect materials, the long-wavelength discrepancy is significant.</image:caption>
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