Abstract:
The invention provides a dynamically swept tunable laser system and method for measuring sensor characteristics obtained from an array of optical sensors comprising means for dividing the total wavelength sweep of the laser into different regions in any particular order where each region contains single or multiple contiguous sweep segments and where each sweep segment is referenced by a start and a stop reference and can have different lengths compared to the other sweep segments. The sensor characteristics are determined from each region swept by the tunable laser. The invention provides for the tunable laser to be adapted to operate in a quasi-continuous mode to select segments in any order. The relative sweep rates of regions can be changed such that some regions can be swept more times than other regions.
Abstract:
A method and system based on spectral domain interferometry for detecting intense THz electric field, allowing the use of thick crystal for spectroscopic purposes, in order to makes long temporal scans for increased spectral resolutions, and overcoming the limitation of over-rotation for presently available high power THz sources. Using this method and system the phase difference of approximately 8898π can be measured, which is 18000 times higher than the phase difference measured by electro-optic sampling ( π/2 ).
Abstract:
An optical semiconductor package includes an optical semiconductor device, a temperature detection unit, and a temperature control unit (46) including a support member (46S), the optical semiconductor device and the temperature detection unit being arranged such that a temperature of a portion (P44) of a surface of the support member (46S) where the optical semiconductor device is arranged and a temperature of a portion (P45) of the surface of the support member (46S) where the temperature detection unit is arranged are substantially in thermal equilibrium with each other.
Abstract:
Exemplary apparatus and method can be provided for obtaining data regarding a plurality of samples. For example, using at least one arrangement, it is possible to receive interferometric information that is based on radiations provided from a reference and the samples that are provided in respective chambers. Alternatively and/or in addition, based on the interferometric information, it is possible to discriminate between agents to identify a particular agent that affects a particular function within at least one of the samples.
Abstract:
The reported invention belongs to spectral interference devices and can be used for spectral research in various fields of technology. The objective of the present invention is to improve the optical characteristics of the spectrometer in which reduced loss of light from the radiation object on aberration is attained with a minimum number of optical elements produced at lower costs. The objective is achieved by the fact that the static Fourier spectrometer contains an input collimator optically coupled with the interferometric unit consisting of a beam splitter and at least two mirrors installed with the ability to create an interference image localized in the plane of the mirrors, and an image recording device optically coupled with the interferometric unit by means of the projective system with the ability to project the figure of the indicated interference image on the image recording device. Besides, the projective system includes a spherical mirror and an objective lens centered against the normal line to the optical surface of the mirror. The mirror and the objective lens are produced to enable optical radiation to pass through the objective lens from the interferometric unit to the spherical mirror, being reflected from it and passing through the same objective lens to the recording device. 4IL.
Abstract:
Current apparatuses and methods for analysis of spectroscopic optical coherence tomography (SOCT) signals suffer from an inherent tradeoff between time (depth) and frequency (wavelength) resolution. In one non-limiting embodiment, multiple or dual window (DW) apparatuses and methods for reconstructing time-frequency distributions (TFDs) that applies two windows that independently determine the optical and temporal resolution is provided. For example, optical resolution may relate to scattering information about a sample, and temporal resolution may be related to absorption or depth related information. The effectiveness of the apparatuses and methods is demonstrated in simulations and in processing of measured OCT signals that contain fields which vary in time and frequency. The DW technique may yield TFDs that maintain high spectral and temporal resolution and are free from the artifacts and limitations commonly observed with other processing methods.
Abstract:
A Micro Electro-Mechanical System (MEMS) spectrometer architecture compensates for verticality and dispersion problems using balancing interfaces. A MEMS spectrometer/interferometer includes a beam splitter formed on a first surface of a first medium at an interface between the first medium and a second medium, a first mirror formed on a second surface of the first medium, a second mirror formed on a third surface of the first medium and balancing interfaces designed to minimize both a difference in tilt angles between the surfaces and a difference in phase errors between beams reflected from the first and second mirrors.
Abstract:
Described are a method and apparatus for high-speed phase shifting of an optical beam. A transparent plate having regions of different optical thickness is illuminated by an optical beam along a path of incidence that extends through the regions. The transparent plate can be moved or the optical beam can be steered to generate the path of incidence. The optical beam exiting the transparent plate has an instantaneous phase value according to the region in which the optical beam is incident. Advantageously, the phase values are repeatable and stable regardless of the location of incidence of the optical beam within the respective regions, and phase changes at high modulation rates are possible. The method and apparatus can be used to modulate a phase difference of a pair of coherent optical beams such as in an interferometric fringe projection system.
Abstract:
L'interféromètre statique comporte une pupille d'entrée, une lame séparatrice, un premier miroir et un second miroir agencés de façon à ce que des faisceaux lumineux provenant d'une source collimatée se divisent sur la lame séparatrice, se réfléchissent sur chacun des miroirs et se recomposent en interférant en sortie de l'interféromètre. L'interféromètre comporte une lame prismatique d'indice n comportant une épaisseur e j variable, le premier faisceau traversant la lame prismatique avant de se réfléchir sur une surface réfléchissante du premier miroir, la surface réfléchissante comportant une pluralité de zones, chaque zone j étant située à une distance moyenne Δ j d'un plan de référence. Le plan de référence étant perpendiculaire à un axe optique et correspondant à une position d'un miroir plan pour laquelle la différence de marche entre les deux faisceaux réfléchis interférant est nulle, chaque épaisseur e j étant sensiblement égale à Δ j · n/(n-1).