Skip to main content Accessibility help
×
Hostname: page-component-84b7d79bbc-tsvsl Total loading time: 0 Render date: 2024-07-30T16:23:09.980Z Has data issue: false hasContentIssue false

7 - Noise theory of optical amplifiers

Optical beat-noise components of the photocurrent equivalent

from Part II - Principles of light polarization and optical amplification

Published online by Cambridge University Press:  05 September 2014

Stefano Bottacchi
Affiliation:
u2t Photonics AG, Berlin
Get access

Summary

Introduction

This chapter presents the semiclassical theory of beat noise generated by amplified spontaneous emission (ASE) noise during the photodetection process. Beat noise theory was proposed by N. A. Olsson [1] in 1989, when the erbium-doped fiber amplifier (EDFA) begun the first revolution in optical communications, enabling an increase of more than two orders of magnitude in transmission capacity using the dense wavelength division multiplexing (DWDM) technique. Intensity modulation (IM) and direct detection (DD) transmission systems deploying DWDM with EDFA and chromatic dispersion compensation mapping largely dominated optical transmission engineering for more than a decade, up to early 2000. More than 400 optical channels running at 10 Gb/s were tightly packed together in an ITU-T standard 25 GHz optical grid, providing an incredibly powerful transmission capacity of 4 Tb/s over several thousands of kilometers of a single-mode optical fiber. In order to support such huge optical channel multiplexing, the optical link had to be compensated for uniform transmission characteristics over at least 80 nm, approximately between 1530 nm and 1610 nm, involving what is known as the C+L bands of the optical fiber transmission windows. Moreover, to compensate for the large optical attenuation and chromatic dispersion encountered along such a link length, optical regeneration stations were used about every 80 km. In a typical 2 000 km link length about 25 optical regeneration stations, each consisting of a pair of C+L flatband optical amplifiers and a bundle of dispersion compensating fibers (DCF), were needed. Since an optical link is intended to be bi-directional, it is apparent that the number of regeneration stations must be doubled to include both senses of transmission, leading to about 100 EDFA for a 2000 km single-fiber link operating at 4 Tb/s over 400 wavelengths in a 25 GHz grid. The second revolution in Optical communications came few years ago, with the advent of coherent optical communication. Today, optical coherent detection (CD) using intradyne and polarization diversity techniques has definitely replaced the heavy, hardware-based IM-DD optical network design with a flexible optical grid allocation, allowing up to 448 Gb/s transmission using a dual-polarization 16QAM modulation format over two optical subcarriers. Of course, DWDM technology is still available and is indeed used to increase network capacity almost proportionally to the number of optical wavelengths.

Type
Chapter
Information
Publisher: Cambridge University Press
Print publication year: 2014

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.)

References

Olsson, N. A., “Lightwave systems with optical amplifiers,” J. Lightw. Technol., vol. 7, no. 7, July 1989.CrossRefGoogle Scholar
Papoulis, A., The Fourier Integral and Its Applications, McGraw-Hill, 1987.Google Scholar
Gradshteyn, I. S. and Ryzhik, I. M., Table of Integrals, Series and Products, 7th edn., Elsevier, 2007.Google Scholar
Papoulis, A., Probability, Random Variables and Stochastic Processes, 3rd edn., McGraw-Hill, 1991.Google Scholar

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
×