Abstract:
A diffraction grating and devices employing same are disclosed. In one particular exemplary embodiment, the present invention may be realized as a diffraction grating comprising a reflective material having a blazed surface with a blaze angle between about 33 degrees and about 41 degrees, and an optically transmissive material disposed adjacent the reflective material having an index of refraction (n), wherein the blazed surface of the reflective material has approximately (350null30)*n number of grooves per millimeter.
Abstract:
An apparatus and method in which illumination light and collected emitted light share a pathway and subsequently are physically separated. The optical configuration is designed such that at the point of separation, the illumination light is at has a smaller cross sectional area than the collected light. Collected light is directed away from the pathway of the illumination light and to detection optics. This configuration is adaptable to illumination and light collection across a broad wavelength spectrum. This configuration is adaptable to scanning in a limited depth of field to allow high throughput optical analysis of samples.
Abstract:
An optical system (20) provides a variable dispersion that helps to collect multi-spectral information on an object within the field of view. The system (20) includes at least two sets (24, 26) of optical elements (42x 42y, 44x, 44y) that have minimal deviation of a center wavelength and a non-zero deviation of at least one other wavelength. By rotating the sets of optical elements (24, 26) relative to one another or together, the degree of wavelength dispersion and the direction of the wavelength dispersion can be varied, respectively. By selectively rotating the sets of optical elements, the system also can be operated in a non-dispersed “white light” mode with no net dispersion at the image plane.
Abstract:
Tomographic approaches to hyperspectral imaging, such as CTHIS1 (Chromotomographic Hyperspectral Imaging Sensor), can eliminate the need for the slit, filter, or resonant cavity and substantially increase the optical throughput of the system. These systems capture a large fraction of the photon energy from the entire spectral band over the entire frame time. CTHIS uses a rotating direct view prism as the dispersing element, consequently, the extended image must be reconstructed from the blurred measured data. Only radiation from monochromatic sources such as LEDs, LASERs and signals with high spectral definition, such as the flames of chemical reactions, remain un-blurred in passing through the prism. Thus, the position, wavelength, and temporal evolution of LEDs, LASERs and certain flames can be easily identified in a wide field of view with minimal signal processing.
Abstract:
Light from an object moving through an imaging system is collected, dispersed, and imaged onto a time delay integration (TDI) detector that is inclined relative to an axis of motion of the object, producing a pixilated output signal. In one embodiment, the movement of the image object over the TDI detector is asynchronous with the movement of the output signal producing an output signal that is a composite of the image of the object at varying focal point along the focal plane. In another embodiment, light from the object is periodically incident on the inclined TDI detector, producing a plurality of spaced apart images and corresponding output signals that propagate across the TDI detector. The inclined plane enables images of FISH probes or other components within an object to be produced at different focal points, so that the 3D spatial relationship between the FISH probes or components can be resolved.
Abstract:
A device for monitoring wavelength division multiplexed optical signals for use in an optical network and in an optical performance monitor. A device has a structure for supporting components of the device. An optical component is supported at one end of the structure for transmitting the optical signals. A diffraction grating is supported at an opposing end of the structure for diffracting the optical signals from the optical component. An optical sensor is supported in relation to the diffraction grating by the structure for monitoring the optical signals. A telephoto lens assembly is supported by the structure and disposed between the optical sensor and the diffraction grating, the lens assembly having a focal length for focusing the optical signals in relation to the optical sensor. Thermal effects on the structure are balanced against thermal effects on the lens assembly. A prism is disposed between the lens assembly and diffraction grating. The prism is configured to anamorphically compress the diffracted optical signals. Thermal effects on the diffraction grating are balanced against thermal effects on the lens and prism.
Abstract:
An apparatus and method in which illumination light and collected emitted light share a pathway and subsequently are physically separated. The optical configuration is designed such that at the point of separation, the illumination light is at has a smaller cross sectional area than the collected light. Collected light is directed away from the pathway of the illumination light and to detection optics. This configuration is adaptable to illumination and light collection across a broad wavelength spectrum. This configuration is adaptable to scanning in a limited depth of field to allow high throughput optical analysis of samples.
Abstract:
In an instrument generating images from the fluorescent emissions of a plurality of fluorescent dyes carried by objects in a flow stream, spectral dispersion is used to expand the images of the objects along one axis of a two-dimensional photosensor array according to emission wavelength. The dispersion is unable to completely separate the emissions of a plurality of dyes because the emission spectra of the dyes overlap in wavelength. The method of the present invention accomplishes accurate estimation of the intensity of the light received from each of a plurality of dyes by decomposing the two dimensional spectrally dispersed images into a set of characteristic parameters using either an iterative curve fitting optimization method or a linear algebraic method.
Abstract:
A tunable spectral source includes an enclosure having first and second apertures; an optical dispersive element positioned in the enclosure; and multiple pixel source elements that are individually controllable for selectively directing one or more broadband light signals through the first aperture to irradiate the optical dispersive element. Each of the broadband light signals irradiates the optical dispersive element at a unique angle of incidence. The optical dispersive element disperses the broadband light signals into spectral component signals at dispersion angles that are dependent upon the angle of incidence of each broadband light signal that irradiates the optical dispersive element. The portions of the spectral component signals that are emitted through the second aperture are determined by selecting one or more particular pixel source elements to irradiate the optical dispersive element.
Abstract:
A device for the adjustable coupling of wavelengths or wavelength regions into the illumination beam path of a microscope, preferably in the beam path of a confocal microscope, comprising at least one dispersive element for wavelength separation of the illumination light and at least one at least partially reflecting element arranged in the wavelength-separated portion of the illumination light for reflecting back a wavelength region in the direction of the microscope illumination, and a device for the adjustable detection of object light coming from an illuminated object, preferably in a microscope beam path, comprising at least one dispersive element for wavelength separation of the object light and means arranged in the wavelength-separated portion of the object light for the adjustable stopping down or cutting out of at least one wavelength region and deflection in the direction of at least one detector.