Year: 2025
Type: article
Abstract: An AlGaN laser diode (LD) on AlN substrate using an n‐type AlN/Al 0.63 Ga 0.37 N superlattice (SL) cladding layer is compared to that using a conventional n‐type Al 0.7 Ga 0.3 N alloy. An n‐type AlN/Al 0.63 Ga 0.37 N SL cladding layer with a thickness of more than 1 μm can be pseudomorphically grown on the AlN substrate, while the Al 0.7 Ga 0.3 N alloy cladding layer should be grown to a thickness of less than around 350 nm to prevent lattice relaxation. The series resistances of the LD structures are estimated to be 18 Ω for the AlN/Al 0.63 Ga 0.37 N SLs (1.5 μm) and 38 Ω for the Al 0.7 Ga 0.3 N alloy (350 nm). Because the SLs allow to pseudomorphically grow a thicker n‐type cladding layer, they are effective for reducing the lateral resistance of n‐type cladding layers and thereby the series resistance of the LD. In the electroluminescence measurement of the LD structure with SLs, the integrated emission intensity superlinearly increases and a sharp peak appears at 289.1 nm at high current injections above around 11 kA cm −2 , indicating the emergence of stimulated emission. The LD structure with the SL cladding layer exhibits lower series resistance, leading to lower current density for stimulated emission than that with the alloy cladding layer.
Source: physica status solidi (a)
Institutions: NTT (Japan), NTT Basic Research Laboratories, Hokkaido University
Language: English
Subfield: Condensed Matter Physics
Field: Physics and Astronomy
Domain: Physical Sciences
Open Access status: bronze
OpenAlex ID: W4408587014