Abstract:
A method of obtaining, in a single exposure, imaging information from an object (16) representative of more than two distinct illumination images, the method comprising the steps of generating first electromagnetic waves (14) at least some of which having spatially modulated polarisation; illuminating the object with the first electromagnetic waves; and capturing second electromagnetic waves (18) emanating from the object.
Abstract:
Embodiments of a system and method for collecting hyperspectral and polarimetric data that are spatially and temporally coincident include a dispersive element configured to receive incident electromagnetic radiation. The dispersive element is configured to disperse a non-zero order of the electromagnetic radiation into its constituent spectra, which is directed to a first focal plane array, and may be read out as hyperspectral data. The dispersive element is also configured to reflect a zero order of the electromagnetic radiation, which is directed through a polarity discriminating element to a second focal plane array, which may be read out as polarimetric data. By synchronously reading out the first and second focal plane arrays, the hyperspectral and polarimetric data may be both spatially and temporally coincident.
Abstract:
A multi-energy polarization imaging method consisting of a multi-fusion, dual-rotating retarder / multiple-energy complete Mueller matrix-based polarimeter and dual-energy capabilities The system includes a light source (14) for illuminating a target (18) with a first quantity of light having a first wavelength and a second quantity of light having a second wavelength, the first and second wavelength being different. A polarization-state generator (22) generates a polarization state for each of the first and second quantities of light, and includes a first polarizer (26) through which the first and second quantities of light are transmitted before entering a first waveplate (32). A polarization-state receiver (44) evaluates a resulting polarization state of the first and second quantities of light following illumination of the target (18), the polarization-state receiver (44) including a second waveplate (48) through which the first and second quantities of light are transmitted before entering a second polarizer (51). An optical image-capture device captures a first image of the target illuminated by the first quantity of light and a second image of the target illuminated by the second quantity of light. A processing unit assigns a weighting factor to at least one of the first and second images and evaluates a weighted difference between the first and second images to generate a multi-energy image of the target (18).
Abstract:
A dynamic self calibration process (130) periodically calibrates a system for precisely measuring low-level birefringence properties (retardance and fast axis orientation) of optical materials. Variations in birefringence measurements can be caused by, for example, changes in the environmental conditions (e.g., ambient pressure or temperature) under which birefringence properties of a sample are measured (140). In one implementation, the dynamic self calibration process (130) repeatedly calibrates the system at different selected frequencies (142, 144) to compensate for different selected baseline variations.
Abstract:
In the channeled spectroscopic polarimetry, a measurement error of a parameter showing a spectropolarization characteristic of a sample is effectively removed, the error being generated by various variations in retardation of a retarder depending upon the state of the sample. With attention being focused on that the retardation of the retarder may be kept constant by stabilization of an incident direction of light that transmits through the retarder, the retarder (R1, R2, 117, 118, 207, 208) was arranged on the light source (7, 202) side with respect to the sample (D, 50,400) so as to effectively remove an influence relative to a measurement error, such as variations in direction of a light ray due to the sample (D, 50, 400).
Abstract:
The invention relates to determining a polarization dependent property (JDUT) of an optical device under test (2), wherein a response signal (R) is received from the device under test (2) in response to an optical stimulus signal (S) having an reference state of polarization (EREF), an output state of polarization (EOUT) of the response signal (R) is determined, a reference information (REF) about the reference state of polarization (EREF) is received, and the polarization dependent property (JDUT) is determined on the base of the reference state of polarization (EREF) and the output state of polarization (EOUT).
Abstract:
A polarization state measuring apparatus of the present invention branches an input signal light into a plurality of signal lights by optical couplers, gives polarization and phase shift which are different from each other, to the signal lights by a plurality of optical elements arranged on optical branch paths, detects the power of each of the signal lights by the corresponding light receiving elements, and after adjusting at least differences in the optical branch paths, processes electrical signals output from the light receiving elements by operating means, to acquire information related to a polarization state of the input signal light. As a result, it is possible to provide a small size polarization state measuring apparatus which can correct differences in arrival times of the signal lights to the light receiving elements, which occur due to differences in the optical path lengths of the plurality of optical branch paths, to thereby measure the polarization state of the input signal light with high accuracy.
Abstract:
A method of determining polarization dependent characteristic of an optical device under test (10) having at least one input and at least one output, comprises the steps of generating and inputting a stimulus signal (4) to each of a plurality of polarization units (27a, 29b, 127c, 129d), setting each of said input stimulus signals into a unique state of polarization, attaching a characteristic identification portion (27, 29, 127, 129) to each of said input and/or polarized stimulus signals, applying said stimulus signal to said device under test (10) for effecting a response signal of said device under test, receiving and identifying (44, 52) each of said characteristic identification portions from said response signal for tracing each of said polarized stimulus signals within said response signal, deriving a polarization dependent characteristic of said device under test from said traced polarized stimulus signals. The method provides a measurement of polarization dependent loss PDL within one shot of a stimulus signal. For such simultaneous measurements couplers (105, 135) are used. Also for polarization mode dispersion PMD.