Subgap density of states spectroscopy using steady-state photoconductivity-based experiments

•The continuity equation forbids the simultaneous sensitization of both carriers.•The density of states above the Fermi level impacts the electron diffusion length.•The density of states below the Fermi level influences the hole diffusion length.•The mobility edges are not sharp in hydrogenated amor...

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Veröffentlicht in:Journal of non-crystalline solids 2023-02, Vol.601, p.122046, Article 122046
Hauptverfasser: Kopprio, Leonardo, Longeaud, Christophe, Schmidt, Javier
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Sprache:eng
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Zusammenfassung:•The continuity equation forbids the simultaneous sensitization of both carriers.•The density of states above the Fermi level impacts the electron diffusion length.•The density of states below the Fermi level influences the hole diffusion length.•The mobility edges are not sharp in hydrogenated amorphous silicon.•Extended states in the valence tail cause the minority carrier thermal quenching. We solve the general equations for a semiconductor of photoconductivity dominated by one type of carrier and obtain two pairs of analytical formulas for a density of state (DOS) spectroscopy inside the band gap from the measurement of the diffusion lengths at different temperatures and generation rates. The equations are tested initially with a numerical simulation and then experimentally for unintentionally-doped hydrogenated amorphous silicon due to the extended consensus about its DOS shape. We estimate the diffusion lengths of the photocarriers using the steady-state photocurrent and the steady-state photocarrier grating. The energy dependence of the DOS below the Fermi energy is estimated. We extract the characteristic temperatures of the valence band tails and their hole capture coefficients, which are in perfect agreement with the bibliographical consensus. For the first time, we provide a consistent explanation of the free-hole concentration decrease with temperature, observed at low temperatures in this amorphous material.
ISSN:0022-3093
1873-4812
DOI:10.1016/j.jnoncrysol.2022.122046