Abstract
We show that a single thin layer (thickness much less than an optical wavelength) of nonlinear optical material can display optical bistability solely as a consequence of local field effects. Optical bistability is predicted when the phase of the complex third-order susceptibility χ (3) is nearly opposite that of the linear dielectric constant ϵ and when the incident field amplitude is adjusted so that | χ (3)|| E 0| 2 is approximately equal to 10 −3| ϵ| 3.
Sign-in/Register to access full text options 
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Schedule a callDisclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.
