Optical techniques for determining thermal properties of materials are described. Optical techniques include Raman scattering and thermal properties include relative length change and coefficient of thermal expansion. Correlations of features of bands observed in the Raman spectra of several glasses with thermal properties of the glasses are demonstrated. The technique provides a convenient method for determining thermal expansion properties of materials.

The present disclosure relates to a lens detection device and a lens detection system, wherein the lens detection device, including: a housing; and a detection module configured within the housing; wherein the detection module includes a control module, at least one light emitting module, and a photosensitive module cooperating with the light emitting module; the control module controls the light emitting module and the photosensitive module for conducting a detection process to a lens disposed between the light emitting module and the photosensitive module. As such, the lens detection may become much more convenient, the detection time may be reduced, and the lens detection device may be adopted widely thereby.

When a reticle is first used, the reticle is loaded in a projection exposure device and measured by either oblique measurement and random measurement, thereby avoiding the fear of uneven sampling and determining the reticle transmittance of the entire reticle as the parent population, without increasing the sampling count. The same effect can be obtained by making the measurement spot size, which is fixed in general, variable and by changing the angle of incidence in relation to the measurement spot size.

A dimming tester station for testing an optical object, the optical object disposed along an axis represented by a central axis of the optical object, the dimming tester station including a motion stage for supporting the optical object, wherein the optical object is disposed between at least one camera with an entrance pupil of the at least one camera disposed in a first plane and a light emitting panel configured to emit light through a front surface disposed in a second plane, the central axis is substantially perpendicular to the first plane and the second plane, the entrance pupil of the at least one camera is disposed in an orientation facing at least a portion of the front surface, the motion stage is configured to be adjustable such that the location of the optical object from each of the first plane and the second plane is alterable.

An apparatus and a method measure a reflectivity and/or transmittivity of an optical surface. The apparatus includes a pulsed coherent white light source for generating pulsed coherent white light, wherein the apparatus is adapted to irradiate the optical surface with at least a part of the generated pulsed coherent white light.

Embodiments described herein relate to an optical device metrology system including a light source to emit a light and a non-polarizing beam splitter to split the light into a first photodetector light path and an optical light path. A first photodetector is disposed in the first photodetector light path and measures a total power of the light. The optical device substrate is disposed in the optical light path and splits the light into a second and a third photodetector light path. A second photodetector is disposed in the second photodetector light path from the optical device substrate. The second photodetector measures a reflected power of the light. A third photodetector is disposed in the third photodetector light path. The third photodetector measures a transmitted power of the light. The controller receives measurements from the first, second, and third photodetectors to calculate a percentage light loss within the optical device substrate.

Disclosed is a device and a method for measuring Fabry-Parot (FP) transmittance curve by using a whispering gallery mode laser source. The device includes: a seed laser, a first polarizer, a second polarizer, a spectroscope, a beam reduction system, a lens, and Polydimethylsiloxane (PDMS) microfluidic chip arranged in sequence.

A demonstration device for demonstrating at least one thermally-reversible characteristic of a photochromic optical article, such as an optical article having a photochromic material, having a housing defining an interior, and an inspection platform within the interior of the housing configured for supporting at least a portion of the optical article. The demonstration device further has at least one ultraviolet light source configured to radiate ultraviolet light into the interior of the housing, and at least one inspection light source configured to illuminate at least a portion of the interior of the housing. The demonstration device further has at least one heating device configured to heat at least a portion of the interior of the housing. The at least one heating device has at least one heat source and at least one fan.

Disclosed is a device and a method for measuring Fabry-Parot (FP) transmittance curve by using a whispering gallery mode laser source. The device includes: a seed laser, a first polarizer, a second polarizer, a spectroscope, a beam reduction system, a lens, and Polydimethylsiloxane (PDMS) microfluidic chip arranged in sequence.

A light intensity distribution measurement apparatus is presented that is capable of accurately measuring the intensity of light in each mode at each position of an optical fiber through which light is propagated in a plurality of modes. With the light intensity distribution measurement apparatus, a gain coefficient matrix is acquired in advance, which is constituted by Brillouin gain coefficients of propagation modes with predetermined optical frequency differences measured using a reference optical fiber that exhibits the same properties as a measurement-target optical fiber and that does not cause mode coupling, and the intensity distribution of light in each propagation mode in a lengthwise direction of the measurement-target optical fiber is calculated based on the gain coefficient matrix and a difference in light intensity before and after Brillouin amplification of the probe light emitted in a predetermined propagation mode at a predetermined optical frequency difference measured using the measurement-target optical fiber.