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. 2016 Jun 24;6:28576. doi: 10.1038/srep28576

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Copyright © 2016, Macmillan Publishers Limited

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Panels (a,b) delineate exciton energies as a function of magnetic field in the Faraday and Voigt configurations, respectively. Panels (c,d) are the oscillator strengths of these exciton states along the z-axis and the x-axis, respectively. Panel (e) illustrates the electric-dipole selection rule of the exciton states. Black and red lines correspond to ψ₁ and ψ₂ excitons. Green and blue lines correspond to and excitons in (a,c), and ψ_5L and ψ_5T in (c,d). Green and blue lines in (c) as well as black and blue lines in (d) are on top of each other. .

Inline graphic — Panels (a,b) delineate exciton energies as a function of magnetic field in the Faraday and Voigt configurations, respectively. Panels (c,d) are the oscillator strengths of these exciton states along the z-axis and the x-axis, respectively. Panel (e) illustrates the electric-dipole selection rule of the exciton states. Black and red lines correspond to ψ₁ and ψ₂ excitons. Green and blue lines correspond to and excitons in (a,c), and ψ_5L and ψ_5T in (c,d). Green and blue lines in (c) as well as black and blue lines in (d) are on top of each other. .