Abstract:
A procedure for self-calibration of an optical polarimeter has been developed that eliminates the need for “known” input signals to be used. The self-calibration data is then taken by moving a polarization controller between several random and unknown states of polarization (SOPs) and recording the detector output values (D0, . . . , D3) for each state of polarization. These values are then used to create an “approximate” calibration matrix. In one exemplary embodiment, the SOP of the incoming signal is adjusted three times (by adjusting a separate polarization controller element, for example), creating a set of four detector output values for each of the four polarizations states of the incoming signal—an initial calibration matrix. The first row of this initial calibration matrix is then adjusted to fit the power measurements using a least squares fit. In the third and final step, the remaining elements of the calibration matrix are adjusted to a given constraint (for example, DOP=100% for all SOPs).
Abstract:
An apparatus for information extraction from electromagnetic energy via multi-characteristic spatial geometry processing to determine three-dimensional aspects. Structure receives the electromagnetic energy, which has a plurality of spatial phase characteristics. Structure separates the plurality of spatial phase characteristics of the received electromagnetic energy. Structure identifies spatially segregated portions of each of the plurality of spatial phase characteristics, with each spatially segregated portion corresponding in a point to point relationship to a spatially segregated portion for each of the other of the plurality of spatial phase characteristics in a group. Structure quantifies each segregated portion to provide a spatial phase metric of each segregated portion for providing a data map of the spatial phase metric of each separated spatial phase characteristic of the plurality of spatial phase characteristics. Structure processes the spatial phase metrics to determine surface contour information for each segregated portion of the data map.
Abstract:
An apparatus for information extraction from electromagnetic energy via multi-characteristic spatial geometry processing to determine three-dimensional aspects of an object from which the electromagnetic energy is proceeding. The apparatus receives the electromagnetic energy. The received electromagnetic energy has a plurality of spatial phase characteristics. The apparatus separates the plurality of spatial phase characteristics of the received electromagnetic energy. The apparatus r identifies spatially segregated portions of each spatial phase characteristic, with each spatially segregated portion of each spatial phase characteristic corresponding to a spatially segregated portion of each of the other spatial phase characteristics in a group. The apparatus quantifies each segregated portion to provide a spatial phase metric of each segregated portion for providing a data map of the spatial phase metric of each separated spatial phase characteristic. The apparatus processes the spatial phase metrics to determine surface contour information for each segregated portion of the data map.
Abstract:
A system, method of configuring, and application a system for introducing a relative phase retardation into orthogonally polarized components of an electromagnetic beam entered thereinto, wherein the system involves a substantially achromatic multiple element retarder system for use in wide spectral range (for example, 190-1700 nm) rotating compensator spectroscopic ellipsometer and/or polarimeter systems.
Abstract:
Polarization evaluation mask according to one mode includes a transparent substrate, a light shielding portion, plural quarter-wavelength plates, and plural polarizers. The light shielding portion is formed on the transparent substrate and has plural openings therein. Plural quarter-wavelength plates are formed to cover at least one opening. Fast axes of the quarter-wavelength plates are different in azimuth by a certain angle. Plural polarizers are disposed upstream of the quarter-wavelength plates with respect to the illumination light and formed to overlay the quarter-wavelength plates and cover at least one of the openings. Transmission axes of the polarizers are different in azimuth by a certain angle. The plural openings are provided with different combinations of an azimuth, of the polarizer and an azimuth of the quarter-wavelength plate from one another.
Abstract:
A micropolarimeter is described for simultaneously extracting all Stokes parameters from incident light. The micropolarimeter includes at least one superpixel, which further includes three or more subpixels, each exact a different polarization components from the incident light. The micropolarimeter includes a first and second alignment layers and a liquid crystal layer disposed between the first and second alignment layers. The liquid crystal molecules of the liquid crystal layer are aligned in accordance with the first and second alignment layers to form the superpixel. A method is provided for manufacturing the photo-aligned liquid-crystal micropolarimeter array.
Abstract:
A polarimeter based on a modified Fizeau interferometer and a method for measuring the optical rotation of a polarized light beam by an optically active substance using the polarimeter, are provided.
Abstract:
A method and device for optical determination of physical properties of features, not much larger than the optical wavelength used, on a test sample are described. A beam is split into reference and illuminating beams having known polarization. The test sample is exposed to the illuminating beam and recombined to form an image. The image is detected using at least one sensor, which may be cameras. A point-to-point map of polarization, phase and power is extracted from data representing the image. Optionally, the sensor may be a camera. The sensor may detect at least three optical parameters, such as a Stokes vector, a Jones vector, a Jones matrix, a Mueller matrix or a coherency matrix.
Abstract:
The present invention relates to ellipsometer and polarimeter systems, and more particularly is an ellipsometer or polarimeter or the like system which operates in a frequency range between 300 GHz or lower and extending to higher than at least 1 Tera-hertz (THz), and preferably through the Infra-red (IR) range up to, and higher than 100 THz, including: a source such as a backward wave oscillator; a Smith-Purcell cell; a free electron laser, or an FTIR source and a solid state device; and a detector such as a Golay cell; a bolometer or a solid state detector; and preferably including at least one odd-bounce polarization state image rotating system, and optionally including a polarizer, at least one compensator and/or modulator, in addition to an analyzer.
Abstract:
This invention relates to the manufacture of semiconductor substrates such as wafers and to a method for monitoring the state of polarization incident on a photomask in projection printing using a specially designed polarization monitoring reticle for high numerical aperture lithographic scanners. The reticle measures 25 locations across the slit and is designed for numerical apertures above 0.85. The monitors provide a large polarization dependent signal which is more sensitive to polarization. A double exposure method is also provided using two reticles where the first reticle contains the polarization monitors, clear field reference regions and low dose alignment marks. The second reticle contains the standard alignment marks and labels. For a single exposure method, a tri-PSF low dose alignment mark is used. The reticles also provide for electromagnetic bias wherein each edge is biased depending on that edge's etch depth.