Kunal Tiwari1,2,Eloi Costals2,Francesc Xavier2,Axel Medaille1,2,Sergio Giraldo2,Marcel Placidi2,Cristobal Voz2,Joaquim Puigdollers2,Edgardo Saucedo2,Zacharie Jehl Li Kao2
Catalonia Institute of Energy Research1,Universitat Politècnica de Catalunya, Av. Eduard Maristany, 16, 08019 Barcelona, Spain.2
Kunal Tiwari1,2,Eloi Costals2,Francesc Xavier2,Axel Medaille1,2,Sergio Giraldo2,Marcel Placidi2,Cristobal Voz2,Joaquim Puigdollers2,Edgardo Saucedo2,Zacharie Jehl Li Kao2
Catalonia Institute of Energy Research1,Universitat Politècnica de Catalunya, Av. Eduard Maristany, 16, 08019 Barcelona, Spain.2
MXene-class materials have emerged as promising candidates in areas currently dominated by graphene, transition metal dichalcogenide (TMD) and related 2D materials, and hold several assets for applications to energy related fields including storage and conversion. Since the first report of Ti<sub>3</sub>C<sub>2</sub>T<sub>x</sub> synthesis in 2011 [1], this ever growing family of materials has garnered significant attention from the research community owing to their remarkably tunable physicochemical properties and ease for large area synthesis using low-cost methods. Ti<sub>3</sub>C<sub>2</sub>T<sub>x</sub> MXene has been utilized as a functional layer/additive in various opto-electronic devices such as solar cells, photodetectors etc. [2]. Ti<sub>3</sub>C<sub>2</sub>T<sub>x</sub> has particularly shown remarkably promising results when used as charge selective contacts in conventional c-Si and Perovskite solar cells [3]. The high conductivity, fully tunable work function, and thickness dependent transparency coupled with a high chemical stability make Ti<sub>3</sub>C<sub>2</sub>T<sub>x</sub> an ideal material to partner with Si and possibly other emerging chalcogenide thin film absorbers as a replacement of the standard p-n junction.<br/>In the present work, we aim at investigating the interplay of a model MXene/c-Si interface with different organic molecular dipole interlayers in terms of carrier transport, carrier selectivity, and chemical compatibility. Initially, a screening of different organic dipoles is performed to identify the most suitable candidates out of PEDOT, PEI, PAMAM, APTES. Multilayer MXene is synthesized from the bulk Ti<sub>3</sub>AlC<sub>2</sub> MAX phase through Minimum Intensive Layer Delamination (MILD) technique and 2D sheets are subsequently deposited by drop casting and spray coating on the n-Si/dipole stack. Optimization routes are investigated to tune the band alignment at the MXene/n-Si interface by using the self-assembled mono layers of different organic dipoles. An in-depth characterization of the as prepared MXene sheets by means of XPS, Raman Spectroscopy, AFM and other methods is presented to assess the chemical and structural properties of the heterojunctions, along with the complete electrical characterization of the MXene/n-Si Schottky diodes where the fundamental properties of the interface formed between the 2D charge selective contact and the 3D semiconductor are investigated. Additionally, optoelectronic properties of first proof of concept devices, both solar cells as well as photodetectors, are reported and the complete set of results is presented in regard to the state of the art. Finally, the use of MXene in combination with emerging Sb<sub>2</sub>Se<sub>3</sub> photovoltaic absorbers is investigated using the c-Si as reference framework.<br/><b>References:</b><br/>[1] Naguib, Michael, et al. "Two Dimensional Nanocrystals: Two Dimensional Nanocrystals Produced by Exfoliation of Ti<sub>3</sub>AlC<sub>2</sub> (Adv. Mater. 37/2011)." <i>Advanced Materials</i> 23.37 (2011): 4207-4207.<br/>[2] Wang, Yizhou, et al. "MXenes for energy harvesting." <i>Advanced Materials</i> (2022): 2108560.<br/>[3] Aydin, Erkan, et al. "Scaled Deposition of Ti<sub>3</sub>C<sub>2</sub>T<sub>x</sub> MXene on Complex Surfaces: Application Assessment as Rear Electrodes for Silicon Heterojunction Solar Cells." <i>ACS nano</i> 16.2 (2022): 2419-2428.