2013
DOI: 10.1364/oe.21.030227
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Strong bound exciton-photon coupling in ZnO whispering gallery microcavity

Abstract: We report the cathodoluminescence (CL) study of bound-exciton-polaritons in ZnO whispering gallery (WG) microcavity. Thanks to the very high spatial resolution (: 100 nm) of CL technique, a scanning CL mapping along the tapered ZnO nanowire is achieved. We observe a clear anticrossing behavior which demonstrates the strong coupling between cavity mode and bound-excitons. Coupled oscillator model including both bound excitons and free excitons fits well with the experimental results. The energy splitting of bou… Show more

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Cited by 7 publications
(2 citation statements)
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“…To further confirm whether the peaks P 4 and P 5 at RT (Figure a) originate from the WGM resonance, the mode numbers in the UV region for sample 2 (the 435 nm ZnO nanowire on Al 2 O 3 /Ag) were calculated. In the UV region, the polarization of emission mainly shows TE preference because the recombination of TE-polarized A, B excitons and their phonon replicas dominate the emission, and thus, the observed peaks P 4 and P 5 may be assigned to the TE–WGMs. , The refractive index for TE polarized light can be expressed using Sellmiere’s dispersion function where n 1 (λ) represents the ZnO refractive index at a wavelength of λ. For the hexagonal WGM resonance, the phase shift of total internal reflection (TIR) follows the equation where N is the interference order of the resonance (i.e., the mode number), D is the diameter of the ZnO nanowire, is the phase shift of TIR at the ZnO–air interface, and ϕ′ is the phase shift of TIR at the ZnO–Al 2 O 3 /Ag interface. , The derivation process of ϕ′ is described in the Supporting Information.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…To further confirm whether the peaks P 4 and P 5 at RT (Figure a) originate from the WGM resonance, the mode numbers in the UV region for sample 2 (the 435 nm ZnO nanowire on Al 2 O 3 /Ag) were calculated. In the UV region, the polarization of emission mainly shows TE preference because the recombination of TE-polarized A, B excitons and their phonon replicas dominate the emission, and thus, the observed peaks P 4 and P 5 may be assigned to the TE–WGMs. , The refractive index for TE polarized light can be expressed using Sellmiere’s dispersion function where n 1 (λ) represents the ZnO refractive index at a wavelength of λ. For the hexagonal WGM resonance, the phase shift of total internal reflection (TIR) follows the equation where N is the interference order of the resonance (i.e., the mode number), D is the diameter of the ZnO nanowire, is the phase shift of TIR at the ZnO–air interface, and ϕ′ is the phase shift of TIR at the ZnO–Al 2 O 3 /Ag interface. , The derivation process of ϕ′ is described in the Supporting Information.…”
Section: Resultsmentioning
confidence: 99%
“…In the UV region, the polarization of emission mainly shows TE preference because the recombination of TE-polarized A, B excitons and their phonon replicas dominate the emission, and thus, the observed peaks P 4 and P 5 may be assigned to the TE−WGMs. 45,46 The refractive index for TE polarized light can be expressed using Sellmiere's dispersion function 47…”
Section: Resultsmentioning
confidence: 99%