A liquid-crystal based color switch for use with an image sensor having sub-diffraction-limited (SDL) pixels. The color switch may switch between a first mode where green light is passed (and blue and red light is blocked) and a second mode where blue and red light is passed (and green light is blocked). The color switch may include an achromatic switch (such as a liquid crystal switch) and retarder stack filter that are both sandwiched between a first and a second polarizer. The SDL pixels may be distributed so that green subpixels are never adjacent to other green subpixels in the same row or column, so that red subpixels are always adjacent to green subpixels in the same row or column, and so that blue subpixels are always adjacent to green subpixels in the same row or column.

The present inventive concepts relate to an inspection apparatus that snapshots an interference image pattern having a high spatial carrier frequency produced from a one-piece off-axis polarimetric interferometer and that precisely and promptly measures a Stokes vector including spatial polarimetric information. The inspection apparatus dynamically measure in real-time a two-dimensional polarization information without employing a two-dimensional scanner.

A method of operating a hyperspectral imaging device includes receiving a light beam at a liquid crystal retarding device, and driving the liquid crystal retarding device with a pre-computed voltage waveform, wherein the voltage waveform is selected to reach a target optical retardance over time for the liquid crystal retarding device.

The present invention provides a sensor having, one or more optical slab waveguides having one or more target regions. The target regions may interact with gas molecules or trap, entrain or capture one or more targets of interest. The optical slab waveguides are adapted to receive one or more input optical beams from one or more light sources to create a plurality of propagating optical waves in optical slab waveguide. The propagating optical waves interact with said one or more target regions to create an optical output wavefront that may be in the form of a diffraction pattern. The target regions may be functionalized with an antibody, polymer, cell, tissue, or biological material.

An apparatus for carrying out polarization resolved Raman spectroscopy on a sample (15), in particular a crystalline sample, comprises: at least one light source (11), in particular at least one laser, for providing excitation radiation to a sample (15), a spectrograph (31) for dividing light from the sample (15), in particular Raman scattered light from the sample (15), into at least one spectrum of spatially separated wavelength components and for directing at least a portion of the at least one spectrum to a detector (29), in particular a CCD detector, a polarization state control element (27) for the light from the sample (15), the polarization state control element (27) being arranged in a light path of at least one light beam (25) traveling from the sample (15) towards the detector (29), and the polarization state control element (27) comprising at least one polarization sensitive optical element (45, 47), in particular a Wollaston prism, the at least one polarization sensitive optical element being adapted to split the at least one light beam (25) into at least two, in particular orthogonally, polarized light beams (35a, 35b, 37a, 37b).

Described herein is non-grain composition, comprising at least a thermally inhibited or HMT waxy tapioca starch having a post-retort viscosity of less than 1500 centipoise. Such composition can be used for retort food applications, shelf-stable, thermally processed food applications, canned food applications: and/or aseptic packing and ultra-heat treated process food applications.

A light receiving device includes a plurality of photoelectric conversion element units 10A.sub.1, 10A.sub.2, 10A.sub.3, and 10A.sub.4 each composed of four types of photoelectric conversion elements including four types of polarization elements 50.sub.1, 50.sub.2, 50.sub.3, and 50.sub.4 and further includes a polarized component measurement unit 91 and a polarized component calculation unit 92, wherein the polarized component measurement unit 91 obtains, for example, a first polarized component and a third polarized component on the basis of output signals from a first photoelectric conversion element and a third photoelectric conversion element, and the polarized component calculation unit 92 calculates, for example, polarized components of a third polarization azimuth and a first polarization azimuth in the first polarized component and the third polarized component on the basis of the obtained third polarized component and the first polarized component.

A circular dichroism spectrometer which comprises a metasurface. The metasurface has a plurality of anisotropic antennas configured to simultaneously spatially separate LCP and RCP spectral components from an incoming light beam. An optical detector array is included which detects the LCP and RCP spectral components. A transparent medium is situated between the metasurface and the optical detector array.

An optical device includes: (1) a substrate; and (2) multiple meta-lenses disposed on the substrate, each meta-lens of the meta-lenses including multiple nanofins disposed on a respective region of the substrate, the nanofins together specifying a phase profile of the meta-lens.

A multi-angle imager (10) comprises an imaging array (Mij) configured to receive light beams (Li) via one or more entrance pupils (A1) according to distinct fields of view (Vi) of an object (P0) along each of multiple entry angles (αi). The imaging array (Mij) comprises multiple imaging branches (M1j, M2j) configured to form respective optical paths for the light beams (L1, L2) through the imager (10) for imaging respective subsections (S1, S2) of the object (P0). Each imaging branch (M1j) comprises a distinct set of optical elements (M11, M21) configured to receive the respective light beam (L1) along the respective entry angle (α1) and redirect the respective light beam (L1) towards the imaging plane (P1). The light beams (L1, L2) from each of the multiple imaging branches (M1j, M2j) are redirected to travel in a common direction (y) between the imaging array (Mij) and the imaging plane (P1).