In an embodiment, a phase shifter includes: a light input end; a light output end; a p-type semiconductor material, and an n-type semiconductor material contacting the p-type semiconductor material along a boundary area, wherein the boundary area is greater than a length from the light input end to the light output end multiplied by a core width of the phase shifter.

An optical semiconductor device according to the present disclosure includes at least one laser, a plurality of EA modulators to which an output of the laser is connected on an input side and which have absorption peak wavelengths different from each other, a multiplexer to which outputs of the plurality of EA modulators are connected on an input side and to which a waveguide is connected on an output side, a temperature detector configured to detect a temperature of the laser or the plurality of EA modulators and a selection control circuitry configured to switch an EA modulator to operate among the plurality of EA modulators in accordance with a detected temperature of the temperature detector.

Two-dimensional (2D) crystals have renewed opportunities in artificial lattice design and assembly without the constraints of epitaxy. However, the lack of thickness control in exfoliated van der Waals (vdW) layers prevents realization of repeat units with high fidelity. Uniform, wafer-scale samples permits engineering of both electronic and optical dispersions in stacks of disparate 2D layers with multiple repeating units. Systems, methods, and devices present optical dispersion engineering in a superlattice structure including alternating layers of 2D excitonic chalcogenides and dielectric insulators. Examples demonstrate >90% narrowband absorption in <4 nm active layer excitonic absorber medium at room temperature, concurrently with enhanced photoluminescence in cm.sup.2 samples. These superlattices show evidence of strong light-matter coupling and exciton-polariton formation with geometry-tunable coupling constants. The results demonstrate proof of concept structures with engineered optical properties and pave the way for a broad class of scalable, designer optical metamaterials from atomically-thin layers.

A silicon based electro-optically active device and method of producing the same, the device comprising: a silicon-on-insulator (SOI) waveguide; an electro-optically active stack within a cavity of the SOI waveguide; and a channel between the electro-optically active stack and the SOI waveguide; wherein the channel is filled with a filling material with a refractive index greater than that of a material forming a sidewall of the cavity to form a bridge-waveguide in the channel between the SOI waveguide and the electro-optically active stack.

A silicon based electro-optically active device and method of production thereof. The device comprising: a silicon-on-insulator (SOI) layer; an electro-optically active stack, disposed on top of the SOI layer: a first epitaxially grown structure comprising a first passive waveguide and a second epitaxially grown structure comprising a second passive waveguide, the first and second passive waveguides being disposed adjacent to respective sides of the electro-optically active stack, wherein the first and second passive waveguides are configured to edge couple light from the first passive waveguide into the electro-optically active stack and from the electro-optically active stack into the second passive waveguide; and an evanescent coupling structure, for evanescently coupling light between the SOI layer and the first and second passive waveguides.

Example embodiments relate to an electro-optical device that includes a vertical p-i-n diode waveguide. The electro-optical device includes a waveguide portion adapted for propagating a multimode wave, the waveguide portion including an intrinsic semiconductor region of the vertical p-i-n diode, a first contact and a second contact for electrically contacting a first electrode and a second electrode of the vertical p-i-n diode. The device also includes an input section for coupling radiation into the waveguide portion and an output section for coupling radiation out of the waveguide portion. The input section, the output section, and the waveguide portion are configured to support a multimode interference pattern for the multimode wave with an optical field with a lateral inhomogeneous spatial distribution in the waveguide portion including regions with higher optical field intensity and regions with lower optical field intensity. The second contact physically contacts the second electrode.

An optoelectronic device and a method of manufacturing the same. The device comprising: a multi-layered optically active stack; an input waveguide, arranged to guide light into the stack; an output waveguide, arranged to guide light out of the stack; and anti-reflective coatings, located between both the input waveguide and the stack and the stack and the output waveguide; wherein the input waveguide and output waveguide are formed of silicon nitride.

Photonic devices having Al.sub.1-xSc.sub.xN and Al.sub.yGa.sub.1-yN materials, where Al is Aluminum, Sc is Scandium, Ga is Gallium, and N is Nitrogen and where 0<x0.45 and 0y1.

Photonic devices having Al.sub.1-xSc.sub.xN and Al.sub.yGa.sub.1-yN materials, where Al is Aluminum, Sc is Scandium, Ga is Gallium, and N is Nitrogen and where 0<x0.45 and 0y1.

Implementations disclosed herein provide for devices and methods for obtaining parity time (PT) symmetric directional couplers through improved phase tuning, along with separate optical gain and optical loss tuning. The present disclosure integrates phase tuning and optical gain/loss tuning structures into waveguides of directional couplers disclosed herein. In some examples, directional couplers disclosed herein integrate one or more hybrid metal-oxide-semiconductor capacitors (MOSCAPs) formed by a dielectric layer between two semiconductor layers that provide for phase tuning via plasma dispersion and/or carrier accumulation depending on voltage bias polarity, and one or more optically active medium that provide for optical gain or loss tuning depending on voltage bias polarity.