| Authors | M. Chahi1,2, A. Gharou3, H. Nehmar4, M. Kasdi3, H. Benhabara4, A. Bouhekka3,4 |
| Affiliations |
1Laboratoire de Génie Electrique et Matériaux LGEM Ecole Supérieure en Génie Electrique et Energétique ESGEE d'Oran, Oran, Algeria 2Institute of Nature and Life Sciences, Tissemsilt University – Ahmed Ben Yahia ELWancharissi, P.B. 182 Bougara Road, 38000 Tissemsilt, Algeria 3Department of Matter Sciences, Faculty of Sciences and Technology, Tissemsilt University – Ahmed Ben Yahia ELWancharissi, P.B. 182 Bougara Road, 38000 Tissemsilt, Algeria 4Laboratoire de Physique des Couches Minces et Matériaux pour l'Electronique – LPCMME, Université Oran 1 Ahmed Ben Bella, B.P. 1524, El M’naouar 31100 Oran, Algeria |
| Е-mail | nehmarmora@gmail.com |
| Issue | Volume 18, Year 2026, Number 4 |
| Dates | Received 10 February 2026; revised manuscript received 15 August 2026; published online 21 August 2026 |
| Citation | M. Chahi, A. Gharou, et al., J. Nano- Electron. Phys. 18 No 4, 04029 (2026) |
| DOI | https://doi.org/10.21272/jnep.18(4).04029 |
| PACS Number(s) | 72.80.Jc, 73.63.Bd |
| Keywords | Nanocrystalline silicon (5) , wxAMPS software, Dark conductivity, Activation energy (7) , Hopping (6) , Simulation study. |
| Annotation |
The main objective of this research is a numerical investigation of the transport properties in hydrogenated nanocrystalline silicon thin films for solar cells applications using the wxAMPS software tool. The simulated samples were fabricated at 100 °C using radiofrequency magnetron sputtering (RFMS) method with RF power 220 W, a gas mixture of 30 % of argon and 70 % of hydrogen under a total pressure of 3 Pa and the target – sample holder distance, fixed at 70 mm, were maintained constant for the three categories intrinsic, phosphorus doped and boron doped films at deposition times of 3 and 30 minutes. The simulation carried out in this research, is based on a layer of nanocrystalline silicon that was constructed using successive and alternative crystalline and amorphous thin layers where their total number is depending on the thickness of the considered sample. The electronic transport mechanism is studied and findings clearly demonstrated that doped and undoped samples have different activation energy () which obviously illustrates the crucial role of doping. The is less than 0.2 eV for all the simulated samples strongly indicating a hoping transport mechanism. These results were compared to experimental and previous works where a good agreement was observed. |
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