Abstract:
A pulse photobleaching methodology wherein a monochromatic illumination (e.g., laser illumination) having a higher power intensity (photobleaching power) just below the photodamage threshold of a luminescent sample is initially used to significantly attenuate sample luminescence without photothermally destroying the sample material. Thereafter, the laser power density may be reduced to a significantly lower level (analytical power level) to carry out spectroscopic measurements (e.g., collection of Raman scattered photons) on the sample. In one embodiment, the laser illumination wavelength remains the same despite changes in laser power intensity. Some figures-of-merit may be computed from optical measurements made at the analytical power level to guide the photobleaching process. Sample-dependent combinations of laser power density and short exposure times may be obtained to significantly expedite photobleaching to assist in collection of sample spectral data in the field without a long wait. Portable spectroscopy systems employing pulse photobleaching may be devised for expeditious collection of spectral data from luminescent samples in the field.
Abstract:
An arc flash detection system includes a sensor for determining and responding to the presence of an arc flash condition in electrical equipment by detecting a pressure rise, rate of pressure rise and/or ultraviolet radiation characteristic of an arc flash, and generating a signal in response thereto; and processing means responsive to said signal for operating a protective system to de-energize the electrical equipment within a period of time of sufficiently short duration to prevent a pressure wave from the arc flash from causing unacceptable darn age to equipment or personnel.
Abstract:
A measurement apparatus disclosed that has a radiation source configured to provide a measurement beam of radiation such that an individually controllable element of an array of individually controllable elements capable of modulating a beam of radiation, is illuminated by the measurement beam and redirects the measurement beam, and a detector arranged to receive the redirected measurement beam and determine the position at which the redirected measurement beam is incident upon the detector, the position at which the redirected measurement beam is incident upon the detector being indicative of a characteristic of the individually controllable element.
Abstract:
Within a lithography process having a critical dimension, a method, system and structure for determining a focus deviation value relative to an ideal focus position said is disclosed. By projecting a series of lines or spots characterized by the constant pitch size which is greater than the projection devise optical resolution and incrementally increasing widths onto the surface of the photoactive material, wherein the width of at least one of the lines or sports is substantially the same as the critical dimension, and the widths of the other lines or spots are substantially equally distributed around the critical dimension, approximate focus and exposure dose deviation values may be determined.
Abstract:
The present invention improves the accuracy of therapy by checking in real time whether an spread-out Bragg peak (SOBP) width agrees with a desired width during irradiation with a beam. The device for outputting a charged particle beam includes a charged particle beam generator 1 including a synchrotron 4; a range modulation device such as a range modulation wheel (RMW) 28 which forms a Bragg peak of an ion beam extracted from this charged particle beam generator 1; an irradiation device 16 which is located in the direction of ion beam propagation of this RMW device 28 and includes a dose monitor 31 for detecting a dose of the ion beam; and an SOBP width calculation device 73 which calculates ion beam Bragg peak formed by the RMW device 28 based on a detection value of the dose monitor 31.
Abstract:
A system operable to detect a light beam generated by a light source includes a substrate that is operable to be coupled to a photomask. One or more image sensors are disposed outwardly from the substrate. An image sensor of the one or more image sensors is operable to detect a light beam and generate a sensor signal representing the detected light beam.
Abstract:
An object is placed at a particular distance away from the nonreflecting side of a mirror, such that the gravitational force of the object affects the mirror. A laser is then pointed at the opposite, reflecting side of the mirror, thereby itself reflecting off the mirror and going back in to the cavity of the laser, creating a mode-hopping effect. The mirror will be affected by three forces, the force of a spring (FS), the force of a modulating signal (FMS), created by an electro mechanical device attached to the mirror, and the gravitational force of objects as they approach and recede away from the mirror.
Abstract translation:物体被放置在远离反射镜的非反射侧的特定距离处,使得物体的重力影响反射镜。 然后将激光指向反射镜的相对的反射侧,从而本身反射离开反射镜并返回激光器的空腔,产生跳频效应。 反射镜将受到三个力,弹簧的力(F S S S S S S),由机电装置产生的调制信号的力(F> MS)的影响 附着在镜子上,以及当物体接近并从镜子中退出时的重力。
Abstract:
An optical measuring device according to the present invention includes: a plane mirror (3), which has a central opening that functions as either a light entering window or a light source fitting hole (5) and an observation window 6′ that enables a photodetector (6) to take measurements; and an integrating hemisphere (2), which has its center of radius of curvature defined within the central opening of the plane mirror (3) and of which the inner wall surface functions as a light diffuse reflective surface (1). The plane mirror (3) and the integrating hemisphere (2) form an integrating space inside.
Abstract:
A light-scattering film is provided and includes a transparent support having thereon at least a light-scattering layer. When substantially parallel light is incident on a surface of the film at an incident angle of 5°, the reflectance for an angle θ in the light-receiving part measured in a plane containing the film normal line and the incident direction is R(θ), the value obtained by normalizing R(θ) by the reflectance of regular reflection is Rrel(θ), and the value calculated from the maximum variation |dRrel(θ)/dθ|max for the angle θ is a scattering coefficient A (formula 1), the reflection coefficient B (formula 2) calculated from the scattering coefficient A and the 5° specular reflectance Rs is from 2.0 to 5.0. Scattering coefficient A=1/(10×|dRrel(θ)/dθ|max) (Formula 1) Reflection coefficient B=2.2×log 10(Rs)−7.5×log 10(A)+5.9 (Formula 2)
Abstract:
Uncaging devices that can be used to uncage photoactivatable caged components are provided. Consistent, uniform and/or high throughput processing of reactions and assays that include caged components is provided. Masked multiwell plates that can be used for uncaging photoactivatable caged components are provided. Methods and apparatus for initiating assays involving caged components are provided.