Skip to main content Accessibility help
×
Hostname: page-component-76fb5796d-25wd4 Total loading time: 0 Render date: 2024-04-27T19:08:55.649Z Has data issue: false hasContentIssue false

12 - Reflectivity and thickness optimization

Published online by Cambridge University Press:  05 January 2012

Innocenzo M. Pinto
Affiliation:
University of Sannio
Maria Principe
Affiliation:
Corso Garibaldi
Riccardo Desalvo
Affiliation:
Universitá degli Studi del Sannio
Gregory Harry
Affiliation:
American University, Washington DC
Timothy P. Bodiya
Affiliation:
Massachusetts Institute of Technology
Riccardo DeSalvo
Affiliation:
Università degli Studi del Sannio, Italy
Get access

Summary

Introduction

This chapter is focused on design strategies for minimizing Brownian (see Chapter 4) and, more generally, thermal noises (see Chapters 3 and 9) in high-reflectivity optical coatings. It is organized as follows: in Section 12.2 we review the basic formulas needed to describe the optical properties of dielectric coatings (an ab-initio derivation of these formulas is included in the Appendix). Brownian noise formulas are the subject of Section 12.3. Section 12.4 presents the key ideas of coating thickness optimization. Thermo-optic noise issues are reviewed in Section 12.5, together with a discussion of pertinent minimization criteria. Section 12.6 contains a few comments on material characterization, and touches the important topic of glassy mixture modeling and optimization.

Coating formulas

In this section we summarize the basic coating formulas on which the subsequent analysis is based. A compact ab-initio derivation of these results is given in the Appendix.

Optical coatings are modeled as stacks of planar layers terminated on both sides by homogeneous halfspaces; the relevant geometry and notation is sketched in Figure 12.1. Layers are identified by an index i = 1, 2, …, NL. It is understood that i = 0 and i = NL + 1 correspond to the left halfspace and the substrate, respectively. It is convenient to introduce a local coordinate system (x, y, zi) for each layer, so that the internal layers i = 1, 2, …, NL correspond to -dizi ≤ 0, the left halfspace is defined by - ∞ < z0 ≤ 0, and the substrate by 0 ≤ zNL + 1 < ∞.

Type
Chapter
Information
Publisher: Cambridge University Press
Print publication year: 2012

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
×