Kunal Datta1,Yifeng Zhao2,Bruno Branco1,Junke Wang1,Valerio Zardetto3,Nga Phung1,Dong Zhang3,1,Andrea Bracesco1,Willemijn Remmerswaal1,Luana Mazzarella2,Martijn Wienk1,Mariadriana Creatore1,Olindo Isabella2,René Janssen1
Technische Universiteit Eindhoven1,Delft University of Technology2,TNO-Solliance3
Kunal Datta1,Yifeng Zhao2,Bruno Branco1,Junke Wang1,Valerio Zardetto3,Nga Phung1,Dong Zhang3,1,Andrea Bracesco1,Willemijn Remmerswaal1,Luana Mazzarella2,Martijn Wienk1,Mariadriana Creatore1,Olindo Isabella2,René Janssen1
Technische Universiteit Eindhoven1,Delft University of Technology2,TNO-Solliance3
The intermittency of solar radiation is a key characteristic that impedes the widespread use of photovoltaic systems. As a result, a critical component of any decarbonized energy economy is solar electricity storage for release on demand.<sup>[1]</sup> Hydrogen (H<sub>2</sub>) evolution through electrochemical (EC) water splitting is an effective method for energy storage due to the high energy density of H<sub>2</sub> fuel. However, present-day H<sub>2</sub> generation relies on byproducts of fossil fuel extraction leading to a high indirect carbon cost.<sup>[2]</sup> Photovoltaic (PV)-assisted EC water splitting methods that employ concentrated photovoltaics, on the other hand, use inorganic multijunction devices whose high manufacturing costs can undermine future commercial competitiveness. As a result, a cost-effective PV device delivering high current without light concentration, coupled to a flow EC system, can potentially provide an efficient method for H<sub>2</sub> generation.<sup>[3]</sup><br/><br/>Metal halide perovskite semiconductors have been used to develop high-performance photovoltaic devices. Their tunable optical bandgap, high defect tolerance, and easy processing, are assets that allow their use in efficient multijunction devices.<sup>[4]</sup> As a result, high open-circuit voltages can be achieved which results in a high current at the operating potential for water splitting (> 1.23 V). This work describes the development of 1 cm<sup>2</sup> active area all-perovskite and perovskite-silicon tandem solar cells by combining wide-bandgap perovskites with lead-tin based narrow-bandgap perovskite and silicon heterojunction bottom-cells respectively. Upon integrating with continuous flow EC cells, high solar-to-hydrogen (STH) conversion efficiencies can be achieved without using light-concentration techniques.<br/><br/>Mixed-halide wide-bandgap perovskite compositions are developed for each multijunction structure and the defect-rich interface between the perovskite and the electron transport layer is passivated in order to increase radiative yield. Recombination layers in the multijunctions, based on thin atomic layer deposited (ALD) NiO<sub>x</sub> (perovskite-silicon) and SnO<sub>x</sub> (all-perovskite) layers, are used to maintain charge neutrality while ensuring low interfacial losses. The ALD NiO<sub>x</sub> interfacial layer increases surface hydroxyl content, thereby improving the binding of self-assembled hole-transporting monolayer (2PACz) in the top-cell in the perovskite-silicon tandem device.<sup>[5]</sup> In the all-perovskite tandem solar cell, the SnO<sub>x</sub> layer also acts as a solvent barrier to protect underlying layers from damage from subsequent solution processing steps.<sup>[6]</sup> Lastly, advanced optical simulations are used to identify key regions of parasitic absorption and reflection losses, which are mitigated by light-management strategies to yield current-matched tandem devices with a power conversion efficiency of > 23% (all-perovskite) and > 25% (perovskite-silicon) in 1 cm<sup>2</sup> active area solar cells. By integrating the device with a flow electrochemical cell using RuO<sub>2</sub> and Pt catalysts for H<sub>2</sub> and O<sub>2</sub> evolution respectively, a continuous water splitting system with a high STH conversion efficiency of > 18% (with all-perovskite) and > 21% (with perovskite-silicon) is achieved.<br/><br/>[1] International Energy Agency, <i>World Energy Outlook 2020</i>, Paris, <b>2020</b>.<br/>[2] F. Lehner, D. Hart, in <i>Electrochem. Power Sources Fundam. Syst. Appl.</i>, Elsevier, <b>2022</b>, pp. 1–36.<br/>[3] C. A. Rodriguez, M. A. Modestino, D. Psaltis, C. Moser, <i>Energy Environ. Sci.</i> <b>2014</b>, <i>7</i>, 3828.<br/>[4] M. T. Hörantner, T. Leijtens, M. E. Ziffer, G. E. Eperon, M. G. Christoforo, M. D. McGehee, H. J. Snaith, <i>ACS Energy Lett.</i> <b>2017</b>, <i>2</i>, 2506.<br/>[5] N. Phung, M. Verheijen, A. Todinova, K. Datta, M. Verhage, A. Al-Ashouri, H. Köbler, X. Li, A. Abate, S. Albrecht, M. Creatore, <i>ACS Appl. </i><i>Mater. Interfaces</i> <b>2022</b>, <i>14</i>, 2166.<br/>[6] J. Wang, V. Zardetto, K. Datta, D. Zhang, M. M. Wienk, R. A. J. Janssen, <i>Nat. Commun.</i> <b>2020</b>, <i>11</i>, 5254.