Real- and momentum-space description of the excitons in bulk and monolayer chromium tri-halides

Excitons with large binding energies ~2–3 eV in CrX 3 have been characterized as being localized (Frenkel) excitons that emerge from the atomic d  −  d transitions between the Cr-3 d - t 2 g and e g orbitals. The argument has gathered strength in recent years as the excitons in recently made monolay...

Full description

Saved in:
Bibliographic Details
Published inNPJ 2D materials and applications Vol. 6; no. 1; pp. 1 - 10
Main Authors Acharya, Swagata, Pashov, Dimitar, Rudenko, Alexander N., Rösner, Malte, Schilfgaarde, Mark van, Katsnelson, Mikhail I.
Format Journal Article
LanguageEnglish
Published London Nature Publishing Group UK 23.05.2022
Nature Publishing Group
Springer Nature
Nature Portfolio
Subjects
Online AccessGet full text

Cover

Loading…
More Information
Summary:Excitons with large binding energies ~2–3 eV in CrX 3 have been characterized as being localized (Frenkel) excitons that emerge from the atomic d  −  d transitions between the Cr-3 d - t 2 g and e g orbitals. The argument has gathered strength in recent years as the excitons in recently made monolayers are found at almost the same energies as the bulk. The Laporte rule, which restricts such parity forbidden atomic transitions, can relax if a symmetry-breaking mechanism is present. While what can be classified as a purely Frenkel exciton is a matter of definition, we show using an advanced first principles parameter-free approach that these excitons in CrX 3 , in both its bulk and monolayer variants, have band origin and it is the d p hybridization between Cr and X that primarily acts as the symmetry-breaking mechanism that relaxes the Laporte rule. We show that the character of these excitons is mostly determined by the Cr- d orbital manifold, nevertheless, the fractions of the spectral weight shared with the ligand halogen states increases as the d p hybridization enhances. The hybridization enhances as the halogen atom becomes heavier, bringing the X- p states closer to the Cr- d states in the sequence Cl → Br → I, with an attendant increase in exciton intensity and a decrease in binding energy. By applying a range of different kinds of perturbations that qualitatively mimics the effects originating from the missing vertex in self-energy, we show that moderate changes to the two-particle Hamiltonian that essentially modifies the Cr- d -X- p hybridization, can alter both the intensities and positions of the exciton peaks. A detailed analysis of several deep-lying excitons, with and without strain, elucidates the fact that the exciton is most Frenkel-like in CrCl 3 and CrBr 3 and acquires mixed Frenkel–Wannier character in CrI 3 , making the excitons in CrI 3 most susceptible to environmental screening and spin–orbit coupling.
Bibliography:NREL/JA-5F00-82163
USDOE Office of Science (SC), Basic Energy Sciences (BES)
AC36-08GO28308; FWP ERW7246
ISSN:2397-7132
2397-7132
DOI:10.1038/s41699-022-00307-7