Abstract: A non-refrigerated tunable semiconductor laser based on a multi-wavelength array includes a thermistor, a tunable laser array, a multiplexing structure, an optical amplifier, an optical splitter, an optical detector, and a main controller. The tunable laser array include a plurality of laser units with different wavelengths, and the tunable laser array is connected to the optical splitter and the main controller through the multiplexing structure and the optical amplifier in sequence. When the laser is influenced by the external environment temperature, the value of the influence caused by the external environment temperature is calculated, and drive currents of the tunable laser array and the optical amplifier are adjusted and controlled respectively according to the calculation result, so as to achieve the purpose that parameters of the final output light are consistent with parameters of the theoretical light.

Abstract: A method for manufacturing a multi-dimensional target waveguide grating and volume grating with micro-structure quasi-phase-matching. An ordinary waveguide grating is used as a seed grating, and on this basis, a two-dimensional or three-dimensional sampling structure modulated with a refractive index, that is, a sampling grating, is formed. The sampling grating comprises multiple shadow gratings, and one of the shadow gratings is selected as a target equivalent grating. A sampled grating comprises Fourier components in many orders, that is, shadow gratings, a corresponding grating wave vector is [Formula 1], and the grating profile of all the shadow gratings changes with the sampling structure [Formula 2]. In a case where a seed grating wave vector [Formula 3] and a required two-dimensional or three-dimensional grating wave vector do not match, a certain Fourier periodic structure component of the Fourier components of the sampling structure is used to compensate for the wave vector mismatch.

Abstract: A method for manufacturing a multi-dimensional target waveguide grating and volume grating with micro-structure quasi-phase-matching. An ordinary waveguide grating is used as a seed grating, and on this basis, a two-dimensional or three-dimensional sampling structure modulated with a refractive index, that is, a sampling grating, is formed. The sampling grating comprises multiple shadow gratings, and one of the shadow gratings is selected as a target equivalent grating. A sampled grating comprises Fourier components in many orders, that is, shadow gratings, a corresponding grating wave vector is [Formula 1], and the grating profile of all the shadow gratings changes with the sampling structure [Formula 2]. In a case where a seed grating wave vector [Formula 3] and a required two-dimensional or three-dimensional grating wave vector do not match, a certain Fourier periodic structure component of the Fourier components of the sampling structure is used to compensate for the wave vector mismatch.