Skip to main content Accessibility help
×
Hostname: page-component-84b7d79bbc-lrf7s Total loading time: 0 Render date: 2024-07-27T03:03:56.495Z Has data issue: false hasContentIssue false

12 - Design and modeling examples of integrated optoelectronic devices

Published online by Cambridge University Press:  09 October 2009

Xun Li
Affiliation:
McMaster University, Ontario
Get access

Summary

The integrated semiconductor distributed feedback laser and electro-absorption modulator

The device structure

A schematic structure of an integrated semiconductor DFB laser and EAM is shown in Fig. 12.1.

The cross-sectional layer structures in the DFB and EAM sections are shown in Tables 12.1 and 12.2, respectively.

Both sections of this device are made of a ridge waveguide with the same ridge width of 2.0 μm, but with different ridge heights of 2.0 μm in the DFB laser section and 3.0 μm in the EAM section, respectively. Thus, the etched ditch stops on top of the laser active region but goes through the modulator active region. This design makes a better match of the effective indices between the DFB laser and EAM sections and hence the reflection from the interface between these two sections will be effectively reduced. The deep etching in the modulator section also improves the far-field pattern emitted from the front facet. Finally, by removing the EAM active region outside the ridge, the EAM insertion loss will reduce and its extinction ratio will increase as shown in Section 11.1.3.

The laser section and the modulator section are 300 μm and 200 μm long, respectively, the electrodes are isolated by a 10 μm wide and 1.0 μm deep trench etched across the ridge. The DFB laser has a uniform purely index-coupled grating with a normalized coupling coefficient of 4. This design is a balance between the output optical power, immunity to feedback from the modulator, and the lasing wavelength uncertainty in a range roughly equal to the Bragg stop-band width.

Type
Chapter
Information
Optoelectronic Devices
Design, Modeling, and Simulation
, pp. 313 - 331
Publisher: Cambridge University Press
Print publication year: 2009

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

Save book to Kindle

To save this book to your Kindle, first ensure coreplatform@cambridge.org is added to your Approved Personal Document E-mail List under your Personal Document Settings on the Manage Your Content and Devices page of your Amazon account. Then enter the ‘name’ part of your Kindle email address below. Find out more about saving to your Kindle.

Note you can select to save to either the @free.kindle.com or @kindle.com variations. ‘@free.kindle.com’ emails are free but can only be saved to your device when it is connected to wi-fi. ‘@kindle.com’ emails can be delivered even when you are not connected to wi-fi, but note that service fees apply.

Find out more about the Kindle Personal Document Service.

Available formats
×

Save book to Dropbox

To save content items to your account, please confirm that you agree to abide by our usage policies. If this is the first time you use this feature, you will be asked to authorise Cambridge Core to connect with your account. Find out more about saving content to Dropbox.

Available formats
×

Save book to Google Drive

To save content items to your account, please confirm that you agree to abide by our usage policies. If this is the first time you use this feature, you will be asked to authorise Cambridge Core to connect with your account. Find out more about saving content to Google Drive.

Available formats
×