2019
DOI: 10.1103/physrevb.100.235202
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Electronic energy band parameters ofCuInSe2: Landau levels in magnetotransmission spectra

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Cited by 3 publications
(2 citation statements)
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“…The electron effective mass in CuInSe 2 m * e = 0.09m 0 [21] (where m 0 is the free electron mass) is much smaller than that of the hole mass m * h = 0.7m 0 [22]. Therefore, wave-functions of donor-like defects can already overlap at quite low concentrations making this material highly doped in terms of donors whereas the concentration of acceptors can still be much below the limit necessary for highly doped semiconductors in terms of acceptors [16].…”
Section: Discussionmentioning
confidence: 99%
“…The electron effective mass in CuInSe 2 m * e = 0.09m 0 [21] (where m 0 is the free electron mass) is much smaller than that of the hole mass m * h = 0.7m 0 [22]. Therefore, wave-functions of donor-like defects can already overlap at quite low concentrations making this material highly doped in terms of donors whereas the concentration of acceptors can still be much below the limit necessary for highly doped semiconductors in terms of acceptors [16].…”
Section: Discussionmentioning
confidence: 99%
“…One may note that the u parameter depends on the inverse of the square of the lattice parameter a via equation (3). Here, we consider the experimental lattice parameters (a = 5.523 Å and c = 11.12 Å for CuInS 2 [72]; a = 5.78 Å and c = 11.62 Å for CuInSe 2 [73]) for the calculation of u vs bandgap variation. The atomic coordinates are taken from the reference [74].…”
Section: Band Structuresmentioning
confidence: 99%