The present invention discloses an imaging system, including an optical lens, where a spectroscopical module that can split a light wave transmitted from the optical lens into three light waves in different wavelength ranges is disposed on an imaging side of the optical lens; and the imaging system further includes three photosensitive chips configured to receive corresponding light waves, where the three photosensitive chips are correspondingly distributed at three light waves emitted by the spectroscopical module, and the spectroscopical module is a prism. In the present invention, a spectroscopical module is used to separate light whose wavelengths are different, and therefore light waves that are output from the spectroscopical module are three light waves in different wavelength ranges. These light waves in the different wavelength ranges are separately received by three different photosensitive chips. Therefore, each separate photosensitive chip receives a light wave whose wavelength range is relatively narrow.

A laser manufacturing system capable of fabricating 3-D resolved 2-D patterns. The system includes a pulse laser source generating a laser beam; a reflectance mirror arranged in the propagation path of the laser to reflect the laser, the mirror being controllable to adjust an emergent angle of the laser; a deformable dispersion unit located in the laser receiving path from the reflectance mirror and having an array of micromirrors controllable in response to the adjusted emergent angle to form required laser patterns from the reflected laser, the laser patterns having spatially separated optical spectral components with multiple propagation angles; and one or more focusing optical components positioned in the propagation path of the separated optical spectral components produced by the deformable dispersion unit; the focusing components recombine the optical spectral components at fabrication targets with patterns defined by the deformable dispersion unit. The laser pulse duration is shortest on or inside the fabrication target along the laser propagation path.

A radiation measurement device having a radiation detector, a measurement instrument provided with a signal conversion unit for carrying out signal conversion on a detection current signal output from the radiation detector, and a signal input line for supplying the detection current signal output from the radiation detector to the signal conversion unit, wherein if a test mode is selected, a test current signal is superposed on the detection current signal and supplied to the signal conversion unit through the closing of contacts and the connection of a constant-voltage source and the signal input line, and if a normal mode is selected, the constant-voltage source is connected to a point having the same potential as the signal input line and the generation of a potential difference between the contacts is prevented through the opening of the contacts and the disconnection of the constant-voltage source and signal input line.

A nanowire composite structure is provided. The nanowire composite structure includes a nanowire core, wherein a material of the nanowire core includes Se, Te or a combination thereof. The nanowire composite structure also includes a metal layer covering the nanowire core. A method for forming the nanowire composite structure, a protective structure of a nanowire, a sensing device, and a method for forming a sensing device are also provided.

A nanowire composite structure is provided. The nanowire composite structure includes a nanowire core, wherein a material of the nanowire core includes Se, Te or a combination thereof. The nanowire composite structure also includes a metal layer covering the nanowire core. A method for forming the nanowire composite structure, a protective structure of a nanowire, a sensing device, and a method for forming a sensing device are also provided.

Systems and methods of measuring ferrule-core concentricity for an optical fiber held by a ferrule are disclosed. The method includes: generating ferrule distance data by measuring distances to a ferrule outside surface as a function of rotation angle using a distance sensor and rotating either the ferrule or the distance sensor about an axis of rotation that is off-center from the true ferrule axis; aligning the axis of rotation with the fiber core; using the ferrule distance data to determine a position of the true ferrule center relative to the optical fiber core; and measuring the concentricity as the distance between the true center of the ferrule and the optical fiber core.

The present invention discloses an imaging system, including an optical lens, where a spectroscopical module that can split a light wave transmitted from the optical lens into three light waves in different wavelength ranges is disposed on an imaging side of the optical lens; and the imaging system further includes three photosensitive chips configured to receive corresponding light waves, where the three photosensitive chips are correspondingly distributed at three light waves emitted by the spectroscopical module, and the spectroscopical module is a prism. In the present invention, a spectroscopical module is used to separate light whose wavelengths are different, and therefore light waves that are output from the spectroscopical module are three light waves in different wavelength ranges. These light waves in the different wavelength ranges are separately received by three different photosensitive chips. Therefore, each separate photosensitive chip receives a light wave whose wavelength range is relatively narrow.

A new technique for sensing optical cavity mode mismatch using a mode converter formed from a cylindrical lens mode converting telescope, radio frequency quadrant photodiodes (RFQPDs), and a heterodyne detection scheme. The telescope allows the conversion of the Laguerre-Gauss basis to the Hermite-Gauss (HG) basis, which can be measured with quadrant photodiodes. Conversion to the HG basis is performed optically, measurement of mode mismatched signals is performed with the RFQPDs, and a feedback error signal is obtained with heterodyne detection.

A method of Light Detection and Ranging (LIDAR) includes generating a first optical pulse that propagates towards a target and receiving an optical return signal reflected from the target resulting from the generated first optical pulse. The optical return signal is processed to determine a number of additional optical pulses desired to be propagated towards the target to meet a performance criteria. The determined number of additional optical pulses is then generated and propagated towards the target. The additional optical return signals reflected from the target are received and processed to obtain one or more LIDAR measurements.

A method of Light Detection and Ranging (LIDAR) includes generating a first optical pulse that propagates towards a target and receiving an optical return signal reflected from the target resulting from the generated first optical pulse. The optical return signal is processed to determine a number of additional optical pulses desired to be propagated towards the target to meet a performance criteria. The determined number of additional optical pulses is then generated and propagated towards the target. The additional optical return signals reflected from the target are received and processed to obtain one or more LIDAR measurements.