High vacuum heat-treated MZO: Increased n-type conductivity and elimination of S-kink in MZO/CdSe/CdTe solar cells

Jamarkattel, Manoj K.; Phillips, Adam B.; Li, Deng‐Bing; Bastola, Ebin; Liyanage, Geethika K.; Friedl, Jared D.; Bista, Sandip S.; Pokhrel, Dipendra; Quader, Abdul; Kaluarachchi, Prabodika N.; Hussain, Zulkifl; Abudulimu, Abasi; Mathew, Xavier; Yan, Yanfa; Ellingson, Randy J.; Heben, Michael J.

doi:10.1557/s43580-022-00341-z

Cited by 4 publications

(2 citation statements)

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“…[3][4][5][6][7] Efficient power conversion in solar cells depends on the generation, transport, and collection of charge carriers, processes which are sensitive to the absorber layer's characteristics and to the device interfaces. [8][9][10][11][12][13][14][15][16][17][18] Charge carrier dynamics within this framework are described by the drift-diffusion equation, [19] which for electrons in one dimension is:…”

Section: Introductionmentioning

confidence: 99%

“…[ 3–7 ] Efficient power conversion in solar cells depends on the generation, transport, and collection of charge carriers, processes which are sensitive to the absorber layer's characteristics and to the device interfaces. [ 8–18 ] Charge carrier dynamics within this framework are described by the drift‐diffusion equation, [ 19 ] which for electrons in one dimension is:

$$\frac{\partial n \left(\right. x , t \left.\right)}{\partial t} = D \frac{\left(\partial\right)^{2} n \left(\right.

…”

Section: Introductionmentioning

confidence: 99%

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Comprehensive Study of Carrier Recombination in High‐Efficiency CdTe Solar Cells Using Transient Photovoltage

Abudulimu,

Carter,

Phillips

et al. 2024

Solar RRL

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Cadmium telluride (CdTe) solar cells represent a commercially successful photovoltaic technology, with an annual production capacity approaching 20 GW. However, improving the open‐circuit voltage (V OC ) remains challenging. This study aims to deepen the understanding of charge carrier recombination in CdTe solar cells and to explore alternative dynamical characterization methods that address the limitations found in conventionally used time‐resolved photoluminescence (TRPL) for CdTe solar cells. We utilized transient photovoltage (TPV) and transient photocurrent (TPC) techniques to investigate charge carrier dynamics under conditions resembling real‐world solar cell operation. Our results reveal that an effective non‐radiative recombination lifetime of 580 ns dominates the charge dynamics at VOC values below 850 mV. Above this threshold, radiative recombination becomes significant, with a radiative recombination coefficient of 1.1×10‐9 cm³ s‐1. Additionally, the stationary charge carrier density at 1 sun was determined to be around 1×1014 cm‐3. By accurately determining both radiative and non‐radiative recombination, this work provides a comprehensive understanding of carrier dynamics in high‐performing CdTe devices and paves the way for improving the VOC and performance of CdTe solar cells.This article is protected by copyright. All rights reserved.

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