Patent classifications
G02F1/3613
CROSSLINKABLE NONLINEAR-OPTICAL CHROMOPHORE SYSTEM
Crosslinked films having electro-optic activity, compositions and compounds for making the films, methods for making the films, and devices that include the films are disclosed.
Organic electro-optic chromophores
Chromophores with large hyperpolarizabilities, films with electro-optic activity comprising the chromophores, and electro-optic devices comprising the chromophores are disclosed.
Non-Linear Optical Materials Containing High Boiling Point Solvents, and Methods of Efficiently Poling the Same
The present invention is directed, in general, to compositions containing electro-optic materials and high boiling point solvents allowing for improved, more efficient poling, as well as methods of poling such materials. Various embodiments of the present invention thus provide materials with excellent electro-optic properties which can be efficiently poled for use in electro-optic devices. In the various embodiments of the present invention, materials can be applied as thin films and efficiently poled at low temperatures with normally applied voltage, while simultaneously exhibiting excellent nonlinear optical macroscopic properties and thermal stability.
NON-LINEAR OPTICAL CRYSTAL AND METHOD FOR MANUFACTURING SAME, AND TERAHERTZ-WAVE GENERATOR AND TERAHERTZ-WAVE MEASURING APPARATUS
Disclosed is a non-linear optical crystal containing pyridinium represented by the following Formula (1), 4-substituted phenylsulfonate represented by the following Formula (2a), and 2,4,6-substituted phenylsulfonate represented by the following Formula (2b).
##STR00001##
ORGANIC ELECTRO-OPTIC CHROMOPHORES
Chromophores with large hyperpolarizabilities, films with electro-optic activity comprising the chromophores, and electro-optic devices comprising the chromophores are disclosed.
ORGANIC ELECTRO-OPTIC CHROMOPHORES
Chromophores with large hyperpolarizabilities, films with electro-optic activity comprising the chromophores, and electro-optic devices comprising the chromophores are disclosed.
Optomechanical doubly resonant 2D frequency doubling devices
Optomechanical device for frequency doubling enhancement are described. The devices include a substrate through which light of a first wavelength is introduced, a first reflector mirror, a conductive layer disposed on the first reflector mirror, and a second mirror spaced apart from the conductive layer, thereby forming an optical cavity between the second mirror and the conductive layer. The devices also include a power source coupled to the second mirror and the conductive layer and a monolayer of non-linear optical material disposed within the optical cavity, the monolayer being configured to produce light of a second wavelength upon interaction with the light of the first wavelength. The second mirror is deformable upon introduction of voltage from the power source and deformation of the second mirror changes a length of the optical cavity, thereby enhancing a power output of the light of the second wavelength produced by the monolayer.
Non-linear optical crystal and method for manufacturing same, and terahertz-wave generator and terahertz-wave measuring apparatus
Disclosed is a non-linear optical crystal containing pyridinium represented by the following Formula (1), 4-substituted phenylsulfonate represented by the following Formula (2a), and 2,4,6-substituted phenylsulfonate represented by the following Formula (2b). ##STR00001##
OPTOMECHANICAL DOUBLY RESONANT 2D FREQUENCY DOUBLING DEVICES
Optomechanical device for frequency doubling enhancement are described. The devices include a substrate through which light of a first wavelength is introduced, a first reflector mirror, a conductive layer disposed on the first reflector mirror, and a second mirror spaced apart from the conductive layer, thereby forming an optical cavity between the second mirror and the conductive layer. The devices also include a power source coupled to the second mirror and the conductive layer and a monolayer of non-linear optical material disposed within the optical cavity, the monolayer being configured to produce light of a second wavelength upon interaction with the light of the first wavelength. The second mirror is deformable upon introduction of voltage from the power source and deformation of the second mirror changes a length of the optical cavity, thereby enhancing a power output of the light of the second wavelength produced by the monolayer.
Organic electro-optic chromophores
Chromophores with large hyperpolarizabilities, films with electro-optic activity comprising the chromophores, and electro-optic devices comprising the chromophores are disclosed.