Edge-Emitting Semiconductor Laser Asymmetric Waveguide Design

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Solution Overview

Problem

Edge emitting semiconductor lasers face challenges with catastrophic optical damage due to small emission areas, leading to low optical output powers and impaired beam quality, while large emission areas reduce the risk of damage but compromise beam quality by supporting additional optical modes.

Innovation Solution

Incorporating a reflection layer in the n-side waveguide region with a lower refractive index than the adjoining n-side waveguide region, and optionally using an undoped spacer layer in the p-side waveguide region, to enhance beam quality and reduce internal absorption, thereby increasing optical output power and stability.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Reliability

If a small emission area is used in the active zone, then the risk of catastrophic optical damage is reduced, but the optical output power is limited and beam quality deteriorates due to support of additional optical modes

Engineering Contradiction:
Improverisk of catastrophic optical damageVSAvoidoptical output power
Core Design Contradiction:
ReliabilityVSPower

Solution Approach 1:

The patent applies asymmetry by making the n-side waveguide region thicker than the p-side waveguide region. This asymmetric waveguide structure modifies the optical mode distribution and confinement, enabling the laser to achieve stable monomode emission while supporting higher optical output powers without catastrophic optical damage. The thicker n-side region provides better thermal management and reduces optical absorption losses.

Inventive Principle:
Principle #4Asymmetry

2Power

If a large emission area is used in the active zone, then the optical output power can be increased, but the beam quality is impaired by supporting additional optical modes

Engineering Contradiction:
Improveoptical output powerVSAvoidbeam quality
Core Design Contradiction:
PowerVSStability of the object's composition

Solution Approach 1:

The asymmetric waveguide structure with a thicker n-side region than the p-side region creates specific optical confinement conditions that favor fundamental mode propagation. This asymmetry in thickness (where the n-side waveguide region has greater thickness) allows the laser to maintain stable monomode emission even at higher output powers, thereby preserving beam quality while enabling increased optical output power.

Inventive Principle:
Principle #4Asymmetry

Solution Approach 2:

The patent implements local quality by creating regions with different optical and electrical properties within the waveguide structure. The n-side and p-side waveguide regions have different thicknesses and doping characteristics, allowing each region to be optimized for specific functions: the thicker n-side region for thermal management and optical confinement, and the p-side region for carrier injection and electrical contact.

Inventive Principle:
Principle #3Local quality

3Ease of manufacture

If a symmetric waveguide structure is used, then the manufacturing is simplified, but the optical absorption by semiconductor material increases reducing efficiency

Engineering Contradiction:
Improvewaveguide structure fabricationVSAvoidinternal absorption of electromagnetic radiation
Core Design Contradiction:
Ease of manufactureVSLoss of energy

Solution Approach 1:

The patent deliberately introduces asymmetry in the waveguide structure by making the n-side waveguide region thicker than the p-side waveguide region. This asymmetric design reduces internal optical absorption by optimizing the optical mode distribution and reducing the overlap between the optical field and lossy semiconductor regions. The thicker n-side region provides better thermal and optical management, reducing overall energy losses while remaining compatible with standard epitaxial growth processes.

Inventive Principle:
Principle #4Asymmetry

Applied Scientific Principles

This section explains which scientific principles are used to turn an abstract innovation direction into a practical engineering solution.

Function Achieved in This Case

The solution achieves stable monomode emission with reduced risk of catastrophic optical damage, improved beam quality by suppressing higher modes, and increased optical output power, making high-energy semiconductor lasers suitable for applications like data storage and printing technology.

Implementation Method 1

at least one reflection layer in the n-side waveguide region... the refractive index of the reflection layer is less than the refractive index of the n-side waveguide region adjoining the reflection layer

Methodology Applied
Scientific EffectReflection: Reflection

Implementation Method 2

n- and p-side waveguide regions are suitable for guiding electromagnetic radiation... the thickness of the n-side waveguide region is greater than that of the p-side waveguide region... electromagnetic radiation is guided more within the n-side waveguide region than the p-side waveguide region

Methodology Applied
Scientific EffectWaveguide: Waveguide (optics)

Implementation Method 3

The active zone preferably comprises a pn-junction, a double heterostructure, a single quantum well (SQW) or a multi quantum well (MQW) structure for generating radiation... the active zone emits radiation from the ultraviolet to green spectral range

Methodology Applied
Scientific EffectElectroluminescence: Electroluminescence

Data Source

PatentUS8625648B2Edge-emitting semiconductor laser
Publication Date: 2014.01.07 OSRAM OPTO SEMICON GMBH & CO OHG
  • US8625648B2 patent drawing
  • US8625648B2 patent drawing
  • US8625648B2 patent drawing

AI summary

An edge emitting semiconductor laser (1) is specified, comprising an n-side waveguide region (21) and a p-side waveguide region (22); an active zone (20) for generating electromagnetic radiation; at least one reflection layer (24) in the n-side waveguide region (21), wherein the active zone (20) is arranged between the two waveguide regions (21, 22), the thickness of the n-side waveguide region (21) is greater than that of the p-side waveguide region (22), the refractive index of the reflection layer (24) is less than the refractive index of the n-side waveguide region (21) adjoining the reflection layer (24).