Expand this Topic clickable element to expand a topic
Skip to content
Optica Publishing Group
Journal Home About Issues in Progress Current Issue All Issues Early Posting

Ultra-broadband tunable continuous phase masks using optical aberrations: publisher’s note

Dimitris Mansour and Dimitris G. Papazoglou

Open Access Open Access

Abstract

This publisher’s note corrects errors in Eq. (2) of Opt. Lett. 43, 5480 (2018) [CrossRef]  .

© 2018 Optical Society of America

In Ref. [1], Eq. (2) was incorrectly displayed as

n^1=cos ϕ sin θ+sin ϕ sin θ−cos θ,n^2=−cos ϕ′ sin θ′−sin ϕ′ sin θ′+cos θ′,r12=d(cos ϕ sin 2θ+sin ϕ sin 2θ−cos 2θ),
when the correct equation is
n^1=cos ϕ sin θx^+sin ϕ sin θy^−cos θz^,n^2=−cos ϕ′ sin θ′x^−sin ϕ′ sin θ′y^+cos θ′z^,r12=d(cos ϕ sin 2θx^+sin ϕ sin 2θy^−cos 2θz^),
The Letter was corrected online as of 2 November 2018.

REFERENCE

1. D. Mansour and D. G. Papazoglou, Opt. Lett. 43, 5480 (2018). [CrossRef]  

Cited By

Optica participates in Crossref's Cited-By Linking service. Citing articles from Optica Publishing Group journals and other participating publishers are listed here.

Alert me when this article is cited.


Equations (2)

Equations on this page are rendered with MathJax. Learn more.

n ^ 1 = cos   ϕ   sin   θ + sin   ϕ   sin   θ − cos   θ , n ^ 2 = − cos   ϕ ′   sin   θ ′ − sin   ϕ ′   sin   θ ′ + cos   θ ′ , r 12 = d ( cos   ϕ   sin   2 θ + sin   ϕ   sin   2 θ − cos   2 θ ) ,
n ^ 1 = cos   ϕ   sin   θ x ^ + sin   ϕ   sin   θ y ^ − cos   θ z ^ , n ^ 2 = − cos   ϕ ′   sin   θ ′ x ^ − sin   ϕ ′   sin   θ ′ y ^ + cos   θ ′ z ^ , r 12 = d ( cos   ϕ   sin   2 θ x ^ + sin   ϕ   sin   2 θ y ^ − cos   2 θ z ^ ) ,
Select as filters
Select Topics Cancel
Top
       
© Copyright 2024 | Optica Publishing Group. All rights reserved, including rights for text and data mining and training of artificial technologies or similar technologies.
Privacy | Terms of Use