TY - JOUR
T1 - In-plane optical polarization and dynamic properties of the near-band-edge emission of an m -plane freestanding AlN substrate and a homoepitaxial film
AU - Chichibu, S. F.
AU - Kojima, K.
AU - Hazu, K.
AU - Ishikawa, Y.
AU - Furusawa, K.
AU - Mita, S.
AU - Collazo, R.
AU - Sitar, Z.
AU - Uedono, A.
N1 - Funding Information:
The authors thank T. Ohtomo for help with the experiments. This work was supported in part by the “Program of Dynamic Alliance for Open Innovation Bridging Human, Environment and Materials” and JSPS KAKENHI (Grant Nos. JP16H06427 and JP17H02907) by MEXT, Japan.
Funding Information:
This work was supported in part by the Program of Dynamic Alliance for Open Innovation Bridging Human, Environment and Materials and JSPS KAKENHI (Grant Nos. JP16H06427 and JP17H02907) by MEXT, Japan.
Publisher Copyright:
© 2019 Author(s).
PY - 2019/10/7
Y1 - 2019/10/7
N2 - For accelerating the development of deep-ultraviolet light-emitting diodes based on high AlN mole fraction (x) AlxGa1-xN for sterilization, disinfection, and skin therapy applications, in-plane optical polarization and dynamic properties of the near-band edge (NBE) cathodoluminescence (CL) peak of a low threading dislocation density (<103 cm-2) m-plane freestanding AlN substrate and a homoepitaxial film are assessed. Consistent with the polarization selection rules, the electric field (E) component of the NBE emission was essentially polarized parallel to the c-axis (E ∥ c). Low-temperature CL spectra of the homoepitaxial film exhibited exciton fine structures: CL peaks at 6.0410 and 6.0279 eV, which were polarized E ∥ c and E perpendicular to the c-axis (E ⊥ c), respectively, are assigned as being due to the recombination of free A-excitons of irreducible representations Γ 1 and Γ 5. The hydrogenic binding energy of the Γ1 A-exciton being 51 meV is verified. Detectable CL peaks under E ∥ c polarization at 6.0315 and 6.0212 eV are tentatively assigned as Γ 1-mixed Γ 5-exciton-polaritons. The concentration of multiple vacancies consisting of an Al-vacancy (VAl) and N-vacancies (VNs), namely, V Al V N 2 - 3, in the substrate was estimated by the positron annihilation measurement to be 2-3 × 1016 cm-3, while that in the epilayer was lower than the detection limit (<1016 cm-3). The NBE CL lifetime of 28 ps of the epilayer subsurface at 300 K is likely limited by the recombination at carbon deep-acceptors on nitrogen sites (3 × 1017 cm-3) and/or V Al V N 2 - 3 Shockley-Read-Hall nonradiative recombination centers (∼1 × 1016 cm-3) with hole capture coefficients of approximately 1 × 10 - 7 and 3 × 10 - 6 cm3s-1, respectively.
AB - For accelerating the development of deep-ultraviolet light-emitting diodes based on high AlN mole fraction (x) AlxGa1-xN for sterilization, disinfection, and skin therapy applications, in-plane optical polarization and dynamic properties of the near-band edge (NBE) cathodoluminescence (CL) peak of a low threading dislocation density (<103 cm-2) m-plane freestanding AlN substrate and a homoepitaxial film are assessed. Consistent with the polarization selection rules, the electric field (E) component of the NBE emission was essentially polarized parallel to the c-axis (E ∥ c). Low-temperature CL spectra of the homoepitaxial film exhibited exciton fine structures: CL peaks at 6.0410 and 6.0279 eV, which were polarized E ∥ c and E perpendicular to the c-axis (E ⊥ c), respectively, are assigned as being due to the recombination of free A-excitons of irreducible representations Γ 1 and Γ 5. The hydrogenic binding energy of the Γ1 A-exciton being 51 meV is verified. Detectable CL peaks under E ∥ c polarization at 6.0315 and 6.0212 eV are tentatively assigned as Γ 1-mixed Γ 5-exciton-polaritons. The concentration of multiple vacancies consisting of an Al-vacancy (VAl) and N-vacancies (VNs), namely, V Al V N 2 - 3, in the substrate was estimated by the positron annihilation measurement to be 2-3 × 1016 cm-3, while that in the epilayer was lower than the detection limit (<1016 cm-3). The NBE CL lifetime of 28 ps of the epilayer subsurface at 300 K is likely limited by the recombination at carbon deep-acceptors on nitrogen sites (3 × 1017 cm-3) and/or V Al V N 2 - 3 Shockley-Read-Hall nonradiative recombination centers (∼1 × 1016 cm-3) with hole capture coefficients of approximately 1 × 10 - 7 and 3 × 10 - 6 cm3s-1, respectively.
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U2 - 10.1063/1.5116900
DO - 10.1063/1.5116900
M3 - Article
AN - SCOPUS:85073228057
SN - 0003-6951
VL - 115
JO - Applied Physics Letters
JF - Applied Physics Letters
IS - 15
M1 - 151903
ER -