The present invention relates to a programmable multicore photonic integrated circuit comprising at least one programmable photonic modules or cores, and/or other photonic units like specific high performance blocks, capable of implementing multipurpose signal processing, by the appropriate programming of its resources, routing within the circuits and the blocks to achieve multifunctional operation and the selection of its input and output ports. The invention also relates to a scalable programmable photonic integrated circuits arranged in a modular multicore approach to increase the processing power of the overall system and/or adding a multitude of functionalities enabled by complex photonics circuitry and parallelization as well as the related operation methods.

An optical circuit including an optical waveguide including temperature compensation structure filled with a temperature compensation material, the optical circuit including adiabatic transition structure in which an optical wave propagating through the optical waveguide adiabatically transitions to the temperature compensation structure filled with the temperature compensation material.

An example device in accordance with an aspect of the present disclosure includes a diamond waveguide disposed on a substrate. The substrate includes a dielectric material. A tuner is to extend from the substrate, and is disposed at least in part over the waveguide. The tuner includes a tuner electrode to control a variable distance between the tuner and the waveguide to vary an effective refractive index of the waveguide.

A system including an optical transmitter. In some embodiments, the system includes: a first array of lasers; a first wavelength multiplexer, connected to the first array of lasers; a first coupler, connected to the wavelength multiplexer; and a first wavelength meter, connected to a first output of the first coupler.

The present invention discloses a wavelength controllable arrayed waveguide grating, of which the dispersion equation of the arrayed waveguide grating is:

[00001]$n_s\left(\frac{d_1.Math.x_1}{f_1}-\frac{d.Math.x}{f}\right)+n_c\Delta L=m\lambda ,$

where, λ is the work wavelength of the arrayed waveguide grating; ΔL is the geometric length difference between the adjacent arrayed waveguides in the waveguide array; m is the multiple of the central wavelength; n_s is the effective refractive index of the free transmission region; n_c is the effective refractive index of the transmission waveguide; d_1 and d represent the distances between the arrayed waveguides in the first free transmission region and the second free transmission region, respectively; f_1 and f are focal lengths of the first slab waveguide and the second slab waveguide, respectively; x_ 1 and x represent the positions of the input waveguide and the output waveguide on the Rowland circle, respectively.

Methods and apparatus for tuning a photonics-based component. An opto-electrical detector is configured to output an electrical signal based on a measurement of light intensity of the photonics-based component, the light intensity being proportional to an amount of detuning of the photonics-based component. Analog-to-digital conversion (ADC) circuitry is configured to output a digital signal based on the electrical signal output from the opto-electrical detector. Feedback control circuitry is configured to tune the photonics-based component based, at least in part, on the digital signal output from the ADC circuitry.

Methods and apparatus for tuning a photonics-based component. An opto-electrical detector is configured to output an electrical signal based on a measurement of light intensity of the photonics-based component, the light intensity being proportional to an amount of detuning of the photonics-based component. Analog-to-digital conversion (ADC) circuitry is configured to output a digital signal based on the electrical signal output from the opto-electrical detector. Feedback control circuitry is configured to tune the photonics-based component based, at least in part, on the digital signal output from the ADC circuitry.

A dependency of a characteristic of an optical circuit on an optical signal intensity occurring due to input of a high intensity optical signal is reduced in a waveguide type optical interferometer circuit. The waveguide type optical interferometer circuit is a waveguide type optical interferometer circuit formed in one plane, and includes an input waveguide, an optical branching unit, an optical coupling unit, an output waveguide, and optical waveguides having different lengths from each other and being interposed between the optical branching unit and the optical coupling unit. A light intensity compensating region is formed on an optical path extending from the optical branching unit to the optical coupling unit, and the light intensity compensating region is formed by using a light intensity compensating material having a light intensity coefficient different from a light intensity coefficient of an optical distance relative to an incident light intensity in the optical path.

A photonic biosensor including a biological probe disposed on a mid-infrared-transparent waveguide can be used to detect biological analytes in biological samples, using specific binding of the analyte to the probe in conjunction with absorption spectroscopy. In various embodiments, the biosensor is used for molecular diagnostics, e.g., to detect oligonucleotides or proteins associated with a coronavirus.

The wavelength response of an arrayed waveguide grating can be tuned, in accordance with various embodiments, using a beam sweeper including one or more heaters to shift a lateral position of light focused by the beam sweeper at an interface of the beam sweeper with an input free propagation region of the arrayed waveguide grating.