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An underestimation of the fundamental band gap values by the density functional theory within the local density approximation and associated approaches is a well-known challenge of ab initio electronic structure computations. Motivated by recent optical experiments [D. Santos-Cottin et al., arXiv:2301.08014], we have revisited first-principles results obtained earlier for EuCd₂As₂ and extended the computational studies to the whole class of systems EuCd₂4pt0exX₂ (X=P, As, Sb, Bi), to EuIn₂4pt0exX₂ (X=P, As, Sb), and to nonmagnetic AEIn₂As₂ (AE=Ca, Sr, Ba) employing a hybrid functional method. We find that our approach provides the magnitude of the energy gap for EuCd₂As₂ in agreement with the experimental value. Actually, our results indicate that EuSn₂As₂, BaIn₂As₂, EuCd₂Bi₂ and EuCd₂SbBi are robust topological insulators, while all other compounds are topologically trivial semiconductors. The trivial band gaps of EuCd₂P₂, EuCd₂As₂, and EuCd₂Sb₂ are in the range of 1.38--1.48 eV, 0.72--0.79 eV, and 0.46--0.49 eV, respectively. The topologically trivial Eu-based systems are antiferromagnetic semiconductors with a strong red shift of the energy gap in a magnetic field caused by the exchange coupling of the band states to spins localized on the $4f$-shell of Eu ions. Additionally, the EuIn₂X₂ (X=P, As) compounds show altermagnetic exchange-induced band spin-splitting, particularly noticeable in the case of states derived from $5d$-Eu orbitals.
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Cuono et al. (2023) studied this question.
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