2022
DOI: 10.29026/oes.2022.220021
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Directional high-efficiency nanowire LEDs with reduced angular color shift for AR and VR displays

Abstract: The emission wavelength of InGaN/GaN dot-in-wire LED can be tuned by modifying the nanowire diameter, but it causes mismatched angular distributions between blue, green, and red nanowires because of the excitation of different waveguide modes. Besides, the far-field radiation patterns and light extraction efficiency are typically calculated by center dipoles, which fails to provide accurate results. To address these issues, we first compare the simulation results between central dipole and dipole cloud with ex… Show more

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Cited by 23 publications
(13 citation statements)
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“…Recent research shows that, by a proper waveguide design, a full-color dot-in-a-wire nanowire LED can achieve a higher external quantum efficiency (EQE) than μLED when its mesa size is less than 10 μm (Fig. 4(a)) [27]. In addition, the reduced angular color shift meets the AR display requirements.…”
Section: High-resolution Micro-ledmentioning
confidence: 99%
“…Recent research shows that, by a proper waveguide design, a full-color dot-in-a-wire nanowire LED can achieve a higher external quantum efficiency (EQE) than μLED when its mesa size is less than 10 μm (Fig. 4(a)) [27]. In addition, the reduced angular color shift meets the AR display requirements.…”
Section: High-resolution Micro-ledmentioning
confidence: 99%
“…Nanowire LEDs have an excellent potential in increasing the resolution density due to their sub-micron diameters. Remarkably, the emission wavelength can be modulated by the injection current, composition, or diameter [57,[122][123][124], but their demanding growth conditions remain a challenge to overcome. Recently, Plessey has demonstrated an efficient growth of InGaN-based red µLEDs, Porotech and Innovation Semiconductor have developed an innovative process for achieving DPT µLEDs, and NS Nanotech has achieved sub-micron red nanowire LEDs with 8.3% EQE [61].…”
Section: Higher Resolution Densitymentioning
confidence: 99%
“…However, the final emission result should only be a function of (θ, φ). Here, we first eliminate wavelength and 2) averaging each dipole polarization: 20,21 A1 θ,φ, x, z, a ð Þ¼…”
Section: Angular Distribution and Lee Calculationsmentioning
confidence: 99%
“…However, the final emission result should only be a function of (θ, φ). Here, we first eliminate wavelength and polarization dependence by (1) multiplying the weightage of each wavelength and (2) averaging each dipole polarization: 20,21 A1()θ,φ,x,z,agoodbreak=p=I,OA()θ,φ,x,z,λ,p,aS()λitalicdλ2S()λitalicdλ, where S(λ) is the emission spectrum without color filter as shown in Figure 3A. The position‐averaged angular distribution for long axis (A 2L ) and short axis (A 2S ) can be calculated as A2L(),θφgoodbreak=z=160RLA1L()θ,φ,x,z2italicπxdx6πRL2, A2S(),θφgoodbreak=z=160RSA1S()θ,φ,x,z2italicπxdx6πRL2, where R L and R S are radius of the circumscribed circle and inscribed circle, respectively.…”
Section: Full‐color Ingan/gan Nanowirementioning
confidence: 99%