A DFT approach to correlate the physical characteristics of novel chalcopyrites ASbN 2 (A = Li, Na) for green technology Junaid Munir, a Saif M. H. Qaid, b Masood Yousaf, c Moeen ud din, d Hamid M. Ghaithan, b Abdullah Ahmed Ali Ahmed e and Quratul Ain * f Semiconductor chalcopyrite compounds have been a subject of research interest due to their diverse range of physical properties that have captured the attention of scientists. In this ongoing research, we have examined the physical characteristics of LiSbN 2 and NaSbN 2 chalcopyrites using DFT. The modied BeckeJohnson (mBJ) potential is utilized for the computation of electronic structures. The stability is attained with negative formation energies and optimization curves. A bandgap of 2.60 eV in LiSbN 2 and 3.15 eV in NaSbN 2 has been achieved, which is further endorsed by the density of states. An in-depth analysis of the optical properties unveils the potential utility of LiSbN 2 and NaSbN 2 in various photovoltaic devices, attributed to its pronounced absorption in the UV spectrum. The transport characteristics are also assessed through various transport characteristics. The large electrical conductivity and ZT values for both chalcopyrite compounds are attained. Due to their remarkable capability to convert heat into electricity, these materials display potential for use in thermoelectric devices. Introduction Thermoelectric materials have gathered signicant attention recently due to their extraordinary capability to transform heat into electricity and vice versa. 1 This property makes them essential components in various energy conversion and har- vesting applications, ranging from powering spacecrato improving the eciency of industrial processes. 2,3 The literature suggests dierent classes of materials that exhibit excellent thermoelectric and optical characteristics, such as perovskites, 48 Zintl compounds, 912 Heusler alloys, 1316 chalco- genides 17,18 and many more. In past years, there has been a developing interest in chalcopyrite-type semiconductors owing to their expanding technological use. 19 The chalcopyrite possesses two general structures, A I B III C V 2 and A II B IV C V 2 , which are derived from IIVI and IIIV semiconductors, where A and B represent cations and C denotes anion. Chalcopyrites are at the leading position of renewable energy technologies due to their capacity to become indispensable, enhance their functionality, and expand their applicability across various elds. 20,21 The chalcopyrite structure CuInSe 2 exhibits excellent optical prop- erties and is used as an absorber in solar energy applications. 22 The exibility of Cu(In,Ga)Se 2 makes them high eciency solar cell materials with record eciency of 20.8%. 23 The AgInSe 2 is observed to be high performance thermoelectric material with ZT of 1.2 at 900 K. 24 The insulating state's three-dimensional topology is observed in the potential candidate AuInSe 2 chal- copyrite structure. 25 The magnetic characteristics are evaluated by exercising density functional theory in the CuFeS 2 semi- conductor with 3.64 m B magnetic moment. 26 The AgGaX 2 (X = Te, S, Se) chalcopyrite with bandgap (1.36 eV - 2.73 eV) have been studied to understand the nonlinear and linear optical eects by utilizing real space atom cutting analysis. 27 The carbon-doped BeSi 1-x C x P 2 and BeGe 1-x C x P 2 show improved optoelectronic (a10 5 cm -1 ) and related characteristics. 28 The dispersion curves of refractive index have proven the BeSiN 2 and BeCN 2 ternary compounds to possess extraordinary optical response. 29 High Seebeck coecient is seen in n-type tin- substituted Cu 1-x Sn x FeS 2 in comparison with p-type chalcopy- rite. 30 The computed data for CuPN 2 with bandgap of 2.135 eV and HPN 2 with 2.4 eV bandgap shows admirable performance in terms of optical and thermoelectric attributes. 31 . There are many other Chalcopyrites such as XPN 2 (X = Na, Li) 32 CdXP 2 (X= Sn/Ge/Si), 33 CuGaTe 2 , 34 ACuS 2 (A = In, Al and Ga), 35 LiGaX 2 (X= S, Se, Te), 36 Ag 1-x InTe 2 , 37 AgX (X = In,Ga)Te 2 (ref. 38) whose exceptional properties have been investigated. The Cu 1-x InTe 2 shows high performance in terms of thermoelectric attributes at high temperatures. 39 While existing literature has extensively a Department of Physics, Riphah International University, Lahore, Pakistan b Department of Physics & Astronomy, College of Sciences, King Saud University, P.O. Box 2455, Riyadh 11451, Saudi Arabia c Department of Physics, University of Education, Lahore, Pakistan d Department of Physics, National Taiwan University, Taipei City, 10617, Taiwan e Center for Hybrid Nanostructures (CHyN) and Fachbereich Physik, Universit¨ at Hamburg, Hamburg, 20146, Germany f Department of Physics, University of Management and Technology, Lahore, Pakistan. E-mail: ainnie357@yahoo.com Cite this: RSC Adv., 2024, 14, 5617 Received 27th November 2023 Accepted 7th February 2024 DOI: 10.1039/d3ra08109e rsc.li/rsc-advances © 2024 The Author(s). Published by the Royal Society of Chemistry RSC Adv., 2024, 14, 56175626 | 5617 RSC Advances PAPER Open Access Article. Published on 13 February 2024. Downloaded on 7/25/2024 2:07:39 AM. This article is licensed under a Creative Commons Attribution-NonCommercial 3.0 Unported Licence. View Article Online View Journal | View Issue