Abstract:
Optical chirped return-to-zero (CRZ) data signals are generated without the need for a separate phase modulator, by using a dual-drive Mach-Zehnder modulator for RZ pulse carving that is driven with two typically sinusoidal signals of either unequal amplitude or unequal relative phase, i.e. of non-vanishing phase difference.
Abstract:
A thermo-optic interferometer switch is arranged to operate in a Push-pull mode by placing approximately a quarter-wavelength effective path-length difference (90 degree bias) between the arms of an interferometer switch in the zero-drive state, and then driving one arm to activate the switch to one state (e.g., the bar state), and driving the other arm to go to the other state (e.g. the cross state).
Abstract:
A coplanar integrated optical waveguide electro-optical modulator comprises a substrate (1) of an electro-optic material, at least two optical waveguides (41, 42) integrated in the substrate in correspondence of a surface (71) thereof, and an electrode system (80, 90, 100; 80, 90, 900; 12-15; 120, 130, 140, 150, 160, 170) arranged on the surface for applying a modulating electric field to the waveguides suitable for causing a modulation of a refractive index of the two waveguides in a device modulation region (50). The waveguides are formed, for at least a section thereof (411, 421) in the device modulation region, in respective substrate regions (61, 62) which have electro-optic coefficients of opposite sign along an axis transversal to the waveguide sections, so that a modulating electric field of same direction and orientation in the waveguide sections causes refractive index modulations of opposite sign in the waveguide sections. Chirp-free coplanar waveguide modulators and single-drive double coplanar strip modulators can thus be obtained.
Abstract:
The optical modulator comprising an optical input signal waveguide, first and second interferometric waveguide arms, a modulated output signal waveguide, a splitter for dividing the input signal between the first and second arms, and a combiner for recombining the signals, transmitted along each of the first and second arms into the output signal waveguide. The first and second electrodes each of a segmented structure having a plurality of elements each extending from a respective one of the first and second electrodes and each terminating at position adjacent a length of corresponding one of the first and second arms wherein only a proportion of the elements terminate at positions such as to have an electro-optic effect on a signal transmitted through the corresponding one of the arms. Thus, only proportion of the elements are in active in the sense that only they induce a phase shift in the signal transmitted through the respective one of the arms.
Abstract:
An interferometer is integrated on an optical chip. The optical chip is formed on a layer of silicon separated from a substrate by a layer of insulating material. The optical chip includes an integrated fiber connector for connecting the optical chip to one or more optical fibers. The fiber connector includes a groove formed in the substrate for receiving an optical fiber and a waveguide for transmitting light to or from the fiber connector. The waveguide includes rib waveguides formed in the layer of silicon and at least one phase modulator for altering the phase of light traveling along one of the rib waveguides. This arrangement forms an interferometer in which light transmitted along different optical paths can be combined and the effective path length of at least one of the optical paths can be altered by the phase modulator.
Abstract:
There is provided an optical circuit including a plurality of optical wave guides each composed of electro-optic crystal such as LiNbO3, or LiTaO3 and each designed to have a domain orientation different from each other. In accordance with the present invention, a portion of an optical device is inverted with respect to a domain. For instance, in an optical wave guide having a domain-inverted portion, if electric fields having the same orientation are applied to a plurality of portions which are to vary an index of refraction thereof, indexes of refraction are caused to vary in opposite polarities. Hence, it is possible to lower a voltage at which an optical device operates. For instance, if the present invention is applied to a Mach-Zehnder type phase shifter, it would be possible to accomplish push-pull operation, only if an electric field having one orientation is applied thereto. In addition, it is possible to further lower a voltage at which the phase shifter operates, by making a difference in an index of refraction between two optical wave guides.
Abstract:
A optical switch comprising: a substrate; and a Mach-Zehnder interferometer circuit provided on the substrate, the Mach-Zehnder interferometer circuit comprising two directional couplers and two optical transmission lines for connecting the directional couplers to each other; elements having Peltier effect provided respectively on the two optical transmission lines; and energizing means for energizing the elements in such a manner that heat is generated from one of the elements with absorption of heat being created in the other element. By virtue of the above construction, the optical switch can realize low power consumption, low extinction ratio, and low crosstalk.
Abstract:
An optic intensity modulator includes a substrate of an optic material that is conductive to light and acoustic waves and has both electrooptic and piezoelectric properties. A pair of associated elongated light waveguides is formed in the substrate, with the waveguides extending substantially coextensively with one another, and being separated from one another by a transverse distance that gradually varies along the courses of the waveguides. Each of two portions of light of substantially identical properties is launched into one of the waveguides for propagation longitudinally thereof, and different phase shifts are induced in the light portions as they propagate in the waveguides by imposing different variable electric fields onto each of the waveguides. The light portions are combined with one another subsequently to their emergence from the waveguides with attendant amplitude modulation of the combined output light due to interference between such phase-shifted light portions.
Abstract:
An apparatus for modulating a beam of light with balanced push-pull mechanism. The apparatus includes a first waveguide comprising a first PN junction on a substrate and a second waveguide comprising a second PN junction on the silicon-on-insulator substrate. The second PN junction is a replica of the first PN junction shifted with a distance. The apparatus further includes a first source electrode and a first ground electrode coupled respectively with the first PN junction and a second source electrode and a second ground electrode coupled respectively with the second PN junction. The apparatus additionally includes a third ground electrode disposed near the second PN junction at the distance away from the second ground electrode, wherein the first ground electrode, the second ground electrode, and the third ground electrode are commonly grounded to have both PN junctions subjected to a substantially same electric field varied in ground-source-ground pattern.
Abstract:
A dual-ring-modulated laser includes a gain medium having a reflective end coupled to an associated gain-medium reflector and an output end, which is coupled to a reflector circuit through an input waveguide to form a lasing cavity. The reflector circuit comprises: a first ring modulator; a second ring modulator; and a shared waveguide that optically couples the first and second ring modulators together. The first and second ring modulators have resonance peaks that are tuned to be offset in alignment from each other to provide an effective reflectance having a flat-top response, which is aligned with an associated lasing cavity mode. The first and second ring modulators are driven in tandem based on the same electrical input signal, whereby the resonance peaks of the first and second ring modulators shift wavelengths in the same direction during modulation, and an effective reflectance stays within the flat-top wavelength range.