Claims Analysis
Total Claims: 10
Claim 1
Independent Claim
142 words
An optically bistable device including a Fabry-Perot etalon containing intracavity optically nonlinear material and arranged to exhibit optical bistability, and wherein: (1) the cavity material refractive index is electro-optically tunable via etalon biassing means to move an etalon interference fringe maximum from a wavelength λ m1 to a wavelength λ m2 , (2) a light source having a wavelength λ s is arranged to pass light through the etalon, where λ m2 lies between λ m1 and λ s , λ s and the source intensity being arranged to initiate optical bistability at an etalon fringe wavelength of λ m2 but to be inappropriate for bistability at a fringe wavelength of λ m1 , and (3) the etalon biassing means are connected to a variable voltage source arranged at least for etalon fringe maximum tuning from λ m1 to λ m2 .
Claim 2
Dependent Claim
142 words
An optically bistable device including a Fabry-Perot etalon containing intracavity optically nonlinear material and arranged to exhibit optical bistability, and wherein: (1) the cavity material refractive index is electro-optically tunable via etalon biassing means to move an etalon interference fringe maximum from a wavelength λ m1 to a wavelength λ m2 , (2) a light source having a wavelength λ s is arranged to pass light through the etalon, where λ m2 lies between λ m1 and λ s , λ s and the source intensity being arranged to initiate optical bistability at an etalon fringe wavelength of λ m2 but to be inappropriate for bistability at a fringe wavelength of λ m1 , and (3) the etalon biassing means are connected to a variable voltage source arranged at least for etalon fringe maximum tuning from λ m1 to λ m2 .
Claim 3
Dependent Claim
54 words
A device according to claim 1 wherein the etalon cavity material has an optical nonlinearity parameter n 2 at least equal to 10 -6 cm 2 /Watt and an electro-optic coefficient and thickness appropriate for cavity phase tuning through at least a bistable loop in response to a bias voltage change of 10 Volts.
Claim 4
Dependent Claim
22 words
A device according to claim 2 wherein the cavity material is a liquid crystal material having a birefringence of at least 0.05.
Claim 5
Dependent Claim
16 words
A device according to claim 3 wherein the birefringence is in the range 0.09 to 0.11.
Claim 6
Dependent Claim
37 words
A device according to claim 3 or 4 wherein the cavity material is optically absorbing to a degree sufficient to effect temperature rise as required for optical bistability, and the etalon mirrors are of dielectric multilayer construction.
Claim 7
Dependent Claim
19 words
A device according to claim 1 having partially absorbing etalon mirrors to effect temperature rise and produce optical bistability.
Claim 8
Dependent Claim
17 words
A device according to claim 1 wherein the etalon cavity material is a multiple quantum well structure.
Claim 9
Independent Claim
129 words
A method of obtaining optical bistability including the steps of: (1) providing a Fabry-Perot etalon arranged for optical bistability and containing intracavity optically nonlinear material, the cavity material refractive index being electro-optically tunable via etalon biassing means to move an etalon interference fringe maximum from a wavelength λ m1 to a wavelength λ m2 , (2) illuminating the etalon with light having a wavelength λ s , where λ m2 lies between λ m1 and λ s , λ s and the light intensity being arranged to initiate bistability at an etalon fringe wavelength of λ m2 but to be inappropriate for bistability at a fringe wavelength of λ m1 , and (3) altering etalon bias to produce etalon fringe maximum tuning from λ m1 to λ m2 .
Claim 10
Independent Claim
129 words
A method of obtaining optical bistability including the steps of: (1) providing a Fabry-Perot etalon arranged for optical bistability and containing intracavity optically nonlinear material, the cavity material refractive index being electro-optically tunable via etalon biassing means to move an etalon interference fringe maximum from a wavelength λ m1 to a wavelength λ m2 , (2) illuminating the etalon with light having a wavelength λ s , where λ m2 lies between λ m1 and λ s , λ s and the light intensity being arranged to initiate bistability at an etalon fringe wavelength of λ m2 but to be inappropriate for bistability at a fringe wavelength of λ m1 , and (3) altering etalon bias to produce etalon fringe maximum tuning from λ m1 to λ m2 .