Abstract:
The optical hold unit (100) of the present invention includes an optical modulator (108) that has an electrical input, an optical input, and an optical output. A 1xN optical splitter (106) is also provided that has an optical input and N optical outputs. In addition, N optical paths (112) are individually coupled to the N optical outputs and carry one of the N output signals. Each optical path has an associated propagation delay. Optical delay elements may be located in any of the N optical paths that carry the output signals. The optical delay elements serve to lengthen the propagation delay (114a-e) of the optical path (112a-e) in which the optical delay element is located. In an alternative embodiment, the optical hold unit (200) includes an optical modulator (108) that has an electrical input, an optical input, and an optical output. An optical resonator (202) is also provided and connected to the optical output of the modulator (108). The optical resonator (202) also includes a partially transmissive output (222) to which an optical path is connected. The optical resonator (202) may also include a gain medium (208) or an optical switch (210).
Abstract:
A single-electrode, push-pull semiconductor PIN Mach-Zehnder modulator (10) that includes first and second PIN devices (12, 14) on a substrate (16). Intrinsic layers (22, 28) of the devices (12, 14) are the active regions of two arms (50, 52) of a Mach-Zehnder interferometer. An outer electrode (38) is connected to the N layer (24) of the first PIN device (12) and a center electrode (40) is connected to the P layer (20) of the first PIN device (12). An outer electrode (42) is connected to the P layer (26) of the second PIN device (14) and the center electrode (40) is connected to the N layer (30) of the second PIN device (14). An RF modulation signal biases the PIN devices (12, 14) in opposite directions and causes the index refraction of the intrinsic layers (22, 28) to change in opposite directions to give a push-pull modulation effect.
Abstract:
An optical device for use with an optical input beam comprises an optical thresholding device (OTD) having a predetermined threshold level, and is positioned along an optical path defined by the propagation direction of the optical input beam (12). A source (20) generates a control beam (22) through the OTD, wherein if the combined intensity of the optical input beam (12) and the control beam (22) is large enough to exceed the threshold level of the OTD, the optical beam passes through the OTD. The OTD attenuates the optical beam as it passes therethrough. In a preferred embodiment, the OTD is a saturable absorber. When the device is configured as an optical comparator, the intensity of the optical input beam (12) is large enough to exceed the threshold level of the OTD, the OTD saturates and turns transparent so that the control beam (22) passes through the OTD as an optical indicator beam and the optical input beam (12) passes through the OTD. When configured as an optical signal attenuator and the intensity of the optical input signal is negligible compared to that of the control beam, the combined intensity of the optical input signal and the control beam do not saturate the OTD.
Abstract:
The optical hold unit (100) of the present invention includes an optical modulator (108) that has an electrical input, an optical input, and an optical output. A 1xN optical splitter (106) is also provided that has an optical input and N optical outputs. In addition, N optical paths (112) are individually coupled to the N optical outputs and carry one of the N output signals. Each optical path has an associated propagation delay. Optical delay elements may be located in any of the N optical paths that carry the output signals. The optical delay elements serve to lengthen the propagation delay (114a-e) of the optical path (112a-e) in which the optical delay element is located. In an alternative embodiment, the optical hold unit (200) includes an optical modulator (108) that has an electrical input, an optical input, and an optical output. An optical resonator (202) is also provided and connected to the optical output of the modulator (108). The optical resonator (202) also includes a partially transmissive output (222) to which an optical path is connected. The optical resonator (202) may also include a gain medium (208) or an optical switch (210).
Abstract:
A quantum-confined Stark effect quantum-dot optical modulator (115) includes an interferometer (130) having a beam splitter (135), first and second parallel optical branches (140a,140b) fed by the beam splitter (135) and a beam combiner (145) fed by the first and second parallel optical branches and a laser (110) for feeding a laser beam to the beam splitter. First and second optical phase shifters (150a,150b) are provided in respective ones of the first and second parallel optical branches. Each optical phase shifter includes an intrinsic semiconductor crystalline planar layer and p-type and n-type planar semiconductor layers on opposite faces of the intrinsic semiconductor crystalline planar layer, the intrinsic layer lying in a plane parallel to a direction of propagation of the laser beam in the respective optical branch. The intrinsic layer has plural layers of planar arrays of quantum dots therein. A reverse bias D.C. voltage source (320,325) is connected across the p-type and n-type layers.
Abstract:
An integrated optoelectronic device (1) includes a substrate(4), at least one optoelectronic component (2) provided on the substrate (4), and a waveguide (9a ... 9n) provided on the substrate (4) and optically connected to the at least one optoelectronic component (2). The waveguide (9a ...9n) is made of a sol-gel glass. A method for making the integrated optoelectronic device (1) includes the steps of providing a substrate (4), providing at least one optoelectronic component (2) on the substrate (4), and providing at least one sol-gel glass waveguide (9a ... 9n) on the substrate (4) and optically connected to the at least one optoelectronic component (2).