Abstract: The present invention discloses an optical gain equalization system for receiving and equalizing a multiple-channel input optical signal. The optical gain equalization system includes a cascaded array of tunable optical filters filtering the multiple-channel input optical signal and generating a plurality of sub-signals and a residual signal and each of the sub-signals transmitted over a mutually exclusive filter-specific spectrum-range while a combination of all the filter-specific spectrums dynamically covering the spectral portions of said multi-channel input optical signal where power equalizations are required, and all said filter-specific spectrums together with the residual signal spectrum substantially covering an entire spectral range of the multi-channel input optical signal.

Abstract: The present invention discloses a tunable optical device. The tunable optical device includes a tuning cavity having a tuning means provided for alternately bonding to at least two different tunable optical cells each comprising a tuning membrane wherein the tuning cavity disposed near the tuning membrane for moving the tuning membrane for tuning one of the at least two tunable optical cells bonded thereon. In a preferred embodiment, the tuning cavity further includes a first electrode disposed on the tuning membrane and a second electrode disposed on a substrate supporting the tuning cavity for applying a voltage to move the tuning membrane. In a preferred embodiment, the optical device further includes an optical device control circuit connected to the tuning means for controlling and moving the tuning membrane.

Abstract: This invention discloses a configuration of thin-film membrane. This thin-film membrane is freestanding, movable, and made of multiple layers of different materials such as silicon nitride, polycrystalline silicon or the combination of these two. This thin-film membrane can be actuated by external controlling forces such as electrostatic force. This thin-film membrane consists of odd number of layers, e.g., 1 layer, 3 layers, 5 layers, . . . , etc. Moreover, the layer profile of this membrane is symmetric, e.g., the bottommost layer is made to be identical to the topmost layer, the next bottommost layer is made to be identical to the next topmost layer, so on and so forth.

Abstract: The present invention discloses an electro-optical device support on a substrate. The electro-optical device includes a sacrificial layer disposed on the substrate having a chamber-wall region surrounding and defining an optical chamber. The electro-optical device further includes a membrane layer disposed on top of the sacrificial layer having a chamber-removal opening surrounding and defining an electric tunable membrane for transmitting an optical signal therethrough. The electrically tunable membrane disposed on top of the optical chamber surrounded by the chamber wall regions. The chamber-wall region is doped with ion-dopants for maintaining the chamber-wall region for removal-resistance under a chamber-forming process performed through the chamber-removal opening. In a preferred embodiment, the chamber-wall region is a doped silicon dioxide region with carbon or nitrogen. In another preferred embodiment, the chamber-wall region is a nitrogen ion-doped SiNxOy region.

Abstract: The present invention discloses an optical gain equalization system for receiving and equalizing a multiple-channel input optical signal. The optical gain equalization system includes a cascaded array of tunable optical filters filtering the multiple-channel input optical signal and generating a plurality of sub-signals and a residual signal and each of the sub-signals transmitted over a mutually exclusive filter-specific spectrum-range while a combination of all the filter-specific spectrums dynamically covering the spectral portions of said multi-channel input optical signal where power equalizations are required, and all said filter-specific spectrums together with the residual signal spectrum substantially covering an entire spectral range of the multi-channel input optical signal.

Abstract: The present invention discloses a tunable optical device. The tunable optical device includes a tuning cavity having a tuning means provided for alternately bonding to at least two different tunable optical cells each comprising a tuning membrane wherein the tuning cavity disposed near the tuning membrane for moving the tuning membrane for tuning one of the at least two tunable optical cells bonded thereon. In a preferred embodiment, the tuning cavity further includes a first electrode disposed on the tuning membrane and a second electrode disposed on a substrate supporting the tuning cavity for applying a voltage to move the tuning membrane. In a preferred embodiment, the optical device further includes an optical device control circuit connected to the tuning means for controlling and moving the tuning membrane.

Abstract: The present invention discloses an optimized optical attenuator device. It includes the design of resonator formed by two identical mirrors, which are made by MEMS process. The structure realizes the minimum insertion loss. The two membranes are chosen to be with high reflection rate. Multiple layer or metal layer or mixture of them can produce membrane of high reflection rate. High reflection rate causes low tuning voltage for one certain attenuation range.

Abstract: This invention discloses a configuration of thin-film membrane. This thin-film membrane is freestanding, movable, and made of multiple layers of different materials such as silicon nitride, polycrystalline silicon or the combination of these two. This thin-film membrane can be actuated by external controlling forces such as electrostatic force. This thin-film membrane consists of odd number of layers, e.g., 1 layer, 3 layers, 5 layers, . . . etc. Moreover, the layer profile of this membrane is symmetric, e.g., the bottommost layer is made to be identical to the topmost layer, the next bottommost layer is made to be identical to the next topmost layer, so on and so forth.

Abstract: The present invention discloses an electro-optical device support on a substrate. The electro-optical device includes two face-to-face freestanding membranes each supported near a top surface on one of two bonded substrates for defining a resonant cavity between the two membranes. Each of the substrates having an entire bulk-portion opposite the cavity etched off as a bulk micro-machining opening extended from each of the membranes through a bottom surface of the substrates.

Abstract: A conductive substrate supports an array of multi-channel optical attenuating devices. Each attenuating device includes a membrane with an optically transparent portion And a flexible support for positioning the optically transparent portion of the membrane spaced from the substrate for defining an air gap. The air gap constitutes a cross-shaped gap-chamber having a horizontally and vertically elongated chambers extended from a central intersection area functioning as an optical active area. A voltage bias circuit applies an electrical bias between the conductive substrate and the membrane to adjust and control an air-gap thickness at the optical active area between the conductive substrate and the membrane. Each of the devices can be manufactured on the same silicon wafer using the same process and can be individually controlled to accommodate different wavelength attenuation at each channel. Production costs, and time and efforts required for aligning the array to optical fibers are also reduced.

Abstract: The present invention discloses an electro-optical device support on a substrate. The electro-optical device includes a sacrificial layer disposed on the substrate having a chamber-wall region surrounding and defining an optical chamber. The electro-optical device further includes a membrane layer disposed on top of the sacrificial layer having a chamber-removal opening surrounding and defining an electric tunable membrane for transmitting an optical signal therethrough. The electrically tunable membrane disposed on top of the optical chamber surrounded by the chamber wall regions. The chamber-wall region is doped with iondopants for maintaining the chamber-wall region for removal-resistance under a chamber-forming process performed through the chamber-removal opening. In a preferred embodiment, the chamber-wall region is a doped silicon dioxide region with carbon or nitrogen. In another preferred embodiment, the chamber-wall region is a nitrogen ion-doped SiNxOy region.

Abstract: The present invention discloses an optimized optical attenuator device. It includes the design of resonator formed by two identical mirrors, which are made by MEMS process. The structure realizes the minimum insertion loss. The two membranes are chosen to be with high reflection rate. Multiple layer or metal layer or mixture of them can produce membrane of high reflection rate. High reflection rate causes low tuning voltage for one certain attenuation range. To reduce the manufacture error and the cost, the two identical membranes can be formed by bonding two MEMS cells fabricated in the same process face to face. To further reduce the insertion loss, the input mode should match the residual basic mode in the resonator. The basic residual mode is the only one surviving in the resonator. A design of the resonator will guarantee this happen. Ripple is a key specification for present optical component.

Abstract: The present invention discloses an array of multi-channel optical attenuating devices. This array of multi-channel optical attenuating devices includes this invention discloses an array of multi-channel optical attenuating devices. This array of multi-channel attenuating devices formed as a plurality of electro-optical devices support on a conductive substrate. Each of these electro-optical devices includes a membrane having an optically transparent portion. Each of these electro-optical devices further includes a flexible support for positioning the optically transparent portion of the membrane spaced from the substrate for defining an air gap. The air gap constitutes a cross-shaped gap-chamber having a horizontally and vertically elongated chambers extended from a central intersection area. The central intersection area constitutes an optical active area.