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The nature of the RT band-edge emission in n-type GaN is not well established. Donor bound exciton emission is unlikely since it is only observed at low temperatures. (Formula presented) and free exciton recombination, which nearly coincide in GaN:Si appear to be more likely than band-band transitions.
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The nature of the RT band-edge emission in n-type GaN is not well established. Donor bound exciton emission is unlikely since it is only observed at low temperatures. (Formula presented) and free exciton recombination, which nearly coincide in GaN:Si appear to be more likely than band-band transitions.
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The shoulder 65 meV below (Formula presented) is its one LO phonon replica. Their peak separation is reduced by (Formula presented) from (Formula presented) as a consequence of momentum selection rules for the zero-phonon transition (Formula presented)
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The shoulder 65 meV below (Formula presented) is its one LO phonon replica. Their peak separation is reduced by (Formula presented) from (Formula presented) as a consequence of momentum selection rules for the zero-phonon transition (Formula presented)
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Since the maximum peak shifts for the blue band exceed the LO phonon energy (91 meV) of GaN the proper value of ɛ in (Formula presented) in this case is that of the high-frequency dielectric constant.
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Since the maximum peak shifts for the blue band exceed the LO phonon energy (91 meV) of GaN the proper value of ɛ in (Formula presented) in this case is that of the high-frequency dielectric constant.
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