Laser vision will develop new markets

Epitaxial regrowth and GaAs can unlock new semiconductor laser markets, argues Richard Hogg.

Design engineers might use epitaxial regrowth to enhance semiconductor laser performance and unlock new markets. Relatively mature epitaxial regrowth process for indium phosphide (InP) lasers are commonly used in 5G, datacom, telecom and co-located optics applications.

Gallium arsenide (GaAs) is a less mature material system, which suits a multitude of emerging laser applications in industrial, biomedical imaging, datacom and sensing.
Epitaxial regrowth better meets the need for greater heat dissipation, reduced optical loss and the ever-increasing demand for photonics integration. It also brings the device performance necessary for semiconductor lasers of the future.


Current InP device manufacturing technologies involve multiple epitaxy (additive) and fabrication steps (lithography and subtractive etch) to form the semiconductor laser. These technologies contrast with the more basic ridge laser structures, where one epitaxy step is followed by subtractive etching to form a waveguide, with passivation and isolation to produce electrical contacts (Figure 1).


Figure 1: Example of a simple ridge laser, epitaxially regrown buried heterostructure laser and epitaxially regrown distributed feedback laser

For InP devices, these epitaxial regrowth processes enable a range of photonic integrated circuit (PIC) building blocks to be produced, such as low loss digital feedback (DFB) and distributed Bragg reflector sections, gain and passive sections and buried heterostructures for low optical loss and enhanced heat extraction.

InP material systems operate in the 1200-1700nm range, whereas GaAs material systems range from red, 650nm quantum wells, to near infrared, 1300nm quantum dots. This wide range enables new applications in optical datacom, silicon photonics, biomedical imaging, displays and data storage. Epitaxial regrowth processes for GaAs are immature in comparison to InP. To realise next-generation devices it is critical that performance is extended beyond that of current epitaxy and ridge waveguide technologies.

Figure 2: Distributed feedback lasers manufactured by epitaxial regrowth

DFB lasers are typical of a device manufactured by epitaxial regrowth (Figure 2). Initially, the lower cladding and active elements (quantum wells) of the laser are epitaxially grown on a substrate. After cleaning and etching, a grating structure is formed in the wafer substrate surface, using electron beam lithography and etching to give the DFB laser mechanism. This produces the correct period and depth of grating for the optical properties required.

Epitaxial regrowth is usually performed by a metal organic, chemical, vapour deposition machine, which deposits semiconductor layers onto the substrate surface and grating. A cladding and cap layer sandwich the active region with the DFB grating of the laser. This provides optical confinement and guides the light, which is emitted from the laser’s facet.

 

Figure 3. Epitaxial regrowth steps for buried heterostructure

Within the process, a range of parameters are controlled, such as temperature, supply of reagents and pressure, to achieve the correct material properties, crystalline quality and uniformity across the wafer. Dopants can be introduced to ensure the required conductivity. From here, the wafer may be processed into an individual laser die in the form of a ridge waveguide laser. Alternatively the wafer may proceed through other epitaxial regrowth steps to make a buried heterostructure, as shown in Figure 3. Here, optical confinement is much gentler than for a ridge laser and current confinement is achieved through either a blocking p-n-p-n structure or making the overgrown material semi-insulating, such as through doping with iron.

Figure 4: GaAs-based laser using marker layers to track the regrowth front

Buried heterostructures allow improved heat extraction and hence greater output power. They also allow more symmetrical output beams, resulting in lower power loss in the subsequent optical systems and reducing the costs to fibre package.

Figure 5: Novel, GaAs-based PIC device

Marker layers track regrowth (Figure 4) to produce novel, GaAs-based, PIC devices (Figure 5), while in-situ etching (cleaning) of the wafer and doping of regrown materials enable current blocking layers, such as iron doped indium phosphide lasers (InP:Fe).

 

About The Author

Richard Hogg is CTO, III-V Epi


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