This relates to sensor systems, detectors, imagers, and readout integrated circuits (ROICs) configured to selectively detect one or more frequencies or polarizations of light, capable of operating with a wide dynamic range, or any combination thereof. In some examples, the detector can include one or more light absorbers; the patterns and/or properties of a light absorber can be configured based on the desired measurement wavelength range and/or polarization direction. In some examples, the detector can comprise a plurality of at least partially overlapping light absorbers for enhanced dynamic range detection. In some examples, the detector can be capable of electrostatic tuning for one or more flux levels by varying the response time or sensitivity to account for various flux levels. In some examples, the ROIC can be capable of dynamically adjusting at least one of the frame rate integrating capacitance, and power of the illumination source.

There is provided an imaging device including: an imaging section including pixels that generate pixel signals on the basis of incident light, the pixels including a polarization pixel having a predetermined polarization direction and a non-polarization pixel; and a polarization rotating section provided on an incidence plane side of the imaging section, and configured to rotate a polarization direction of the incident light.

The present disclosure discloses a colorimetry calculation method for a display. The display includes a quantum dot backlight module and a first polarizer, wherein the quantum dot backlight module includes a light guide plate, a quantum dot thin film layer, and a backlight. The method obtains the correction spectrum of the quantum dot backlight module, and obtains the true spectrum of the quantum dot backlight module when the first polarizer is arranged on the light exit side of the quantum dot backlight module based on the correction spectrum and the measurement spectrum, that is, the modified spectrum, so as to accurately simulate the chromatic offset phenomenon due to the secondary excitation of the first polarizer, and provide the basis for the quantitative design of the display including the quantum dot backlight module. The present disclosure also discloses a chromaticity calculation method of a display.

Optical measuring system for determining polarization-optical properties of a sample, which comprises a polarization state generator (PSG) which is configured for preparing a measuring light which is propagating along an analysis beam path with a defined polarization state; a sample receptacle which is arranged downstream of the PSG in the analysis beam path and which is adapted for receiving the sample; a polarization state analyzer (PSA) which is arranged downstream of the sample receptacle in the analysis beam path; a detector which is arranged downstream of the PSA in the analysis beam path for detecting the measuring light, wherein the PSA and the detector are configured for capturing a polarization rotation .sub.P(.sub.eff) of the measuring light which is caused by the sample; and an evaluation and control unit for evaluating measuring signals from the detector and/or PSA and/or PSG, wherein a wavelength-spectrum of the measuring light contains at least a first wavelength .sub.1 and a second wavelength .sub.2, wherein the detector is configured for detecting measuring light with the first wavelength separated from measuring light with the second wavelength, and wherein the evaluation and control unit is configured for calculating a polarization rotation .sub.P(.sub.0) of the measuring light which is caused by the sample at a standardized wavelength .sub.0 in dependency from (a) a first polarization rotation .sub.P(.sub.1) at the first wavelength .sub.1, (b) a second polarization rotation .sub.P(.sub.2) at the second wavelength .sub.2, (c) a first transmission T(.sub.1) at the first wavelength .sub.1, and (d) a second transmission T(.sub.2) at the second wavelength .sub.2.

Optical measuring system for determining polarization-optical properties of a sample, which comprises a polarization state generator (PSG) which is configured for preparing a measuring light which is propagating along an analysis beam path with a defined polarization state; a sample receptacle which is arranged downstream of the PSG in the analysis beam path and which is adapted for receiving the sample; a polarization state analyzer (PSA) which is arranged downstream of the sample receptacle in the analysis beam path; a detector which is arranged downstream of the PSA in the analysis beam path for detecting the measuring light, wherein the PSA and the detector are configured for capturing a polarization rotation .sub.P(.sub.eff) of the measuring light which is caused by the sample; and an evaluation and control unit for evaluating measuring signals from the detector and/or PSA and/or PSG, wherein a wavelength-spectrum of the measuring light contains at least a first wavelength .sub.1 and a second wavelength .sub.2, wherein the detector is configured for detecting measuring light with the first wavelength separated from measuring light with the second wavelength, and wherein the evaluation and control unit is configured for calculating a polarization rotation .sub.P(.sub.0) of the measuring light which is caused by the sample at a standardized wavelength .sub.0 in dependency from (a) a first polarization rotation .sub.P(.sub.1) at the first wavelength .sub.1, (b) a second polarization rotation .sub.P(.sub.2) at the second wavelength .sub.2, (c) a first transmission T(.sub.1) at the first wavelength .sub.1, and (d) a second transmission T(.sub.2) at the second wavelength .sub.2.

A laser radar system capable of active polarization comprises a signal processing unit for sending a control signal; a laser emitting unit for emitting a first laser to a target after receiving the control signal, wherein the laser emitting unit comprises a liquid crystal polarization driver and a liquid crystal polarization component group, and the liquid crystal polarization driver controls a phase delay of the liquid crystal polarization component group to therefore change a polarized state of the first laser; and a laser receiving unit for receiving a second laser reflected off the target and analyzing polarization information of the second laser through the signal processing unit to evaluate surface characteristics of the target.

A laser radar system capable of active polarization comprises a signal processing unit for sending a control signal; a laser emitting unit for emitting a first laser to a target after receiving the control signal, wherein the laser emitting unit comprises a liquid crystal polarization driver and a liquid crystal polarization component group, and the liquid crystal polarization driver controls a phase delay of the liquid crystal polarization component group to therefore change a polarized state of the first laser; and a laser receiving unit for receiving a second laser reflected off the target and analyzing polarization information of the second laser through the signal processing unit to evaluate surface characteristics of the target.

A polarimeter includes a Polarization Maintaining (PM) coupler with an input configured to receive input light and split the input light to a first output and a second output; a first PM fiber coupled to the first output; a second PM fiber coupled to the second output; a first polarization device coupled to the first PM fiber; a second polarization device coupled to the second PM fiber; and a plurality of detectors coupled to the first polarization device and the second polarization device, wherein outputs i.sub.1, i.sub.2, i.sub.3, i.sub.4 are determined based on outputs of the plurality of detectors, the outputs i.sub.1, i.sub.2, i.sub.3, i.sub.4 are linear projections of corresponding Stokes Parameters of the input light.

A polarimeter includes a Polarization Maintaining (PM) coupler with an input configured to receive input light and split the input light to a first output and a second output; a first PM fiber coupled to the first output; a second PM fiber coupled to the second output; a first polarization device coupled to the first PM fiber; a second polarization device coupled to the second PM fiber; and a plurality of detectors coupled to the first polarization device and the second polarization device, wherein outputs i.sub.1, i.sub.2, i.sub.3, i.sub.4 are determined based on outputs of the plurality of detectors, the outputs i.sub.1, i.sub.2, i.sub.3, i.sub.4 are linear projections of corresponding Stokes Parameters of the input light.

Apparatus are described herein related to augmenting human vision by means of adaptive polarization filter grids. A preferred embodiment is described as smart sunglasses, realized as see through head mountable device (HMD) configured to reduce glare originating from polarized light. Each eyeglass of the HMD is associated with a grid comprising a plurality of dynamically configurable polarization filters placed in the path of the light. A polarization analyzer module analyzes the polarization characteristics of a field of view and performs an optimization calculation. The polarization analyzer controls the said grid via a controller module in such a way that the filter state of each grid element can be addressed separately. The grid of polarization filters causes the polarization characteristics of the incident light to be adapted in such a way as to reduce glare and/or to provide a user of the said head mountable device with an enhanced visual perception of the field of view. The user of the described head mountable device has the option of selection between a plurality of polarization enhancement modes, such as horizontal or vertical polarization filtering only or a hybrid mode combining both horizontal and vertical polarization filtering on an individual basis for each grid element. Additionally smart window and smart mirror embodiments of the described adaptive polarization filter grids are introduced.