Thermo Electron Scientific Instruments Corporation

Thermo Finnigan LLC

Francis Jerome Deck

Damian W Ashmead

John Magie Coffin

Alexander Grenov

Kevin K Kim

Richard C Wieboldt

Chris Xavier Kauffold

Joe Hodkiewicz

Federico Izzia

George Douglas Jones

James Ronald Hyatt

Matthew Wayne Meyer

Alan Ronemus

Michael S Georgiadis

David L Dalrymple

Ning Ning Pan

Carla S Draper

William Robert Keefe

William Joseph McCarthy

George L Skupniewicz

Eric Jiang

Mark H Wall

Louie Delaware

William R Finch

Todd R Clermont

Gabor John Kemeny

John R O'Keefe

Steven Ralph Lowry

Koichi Nishikida

Yan Min

Michael Georgiadis

William Finch

Provided are systems and methods related to hybrid reflective microscope objectives and lens systems used in a spectroscopy system. The objective lens system includes a primary aspheric mirror having a first R-value; and a secondary aspheric mirror having a second R-value smaller than the first R-value, where in the objective lens system has a working distance of at least 20 mm and a numerical aperture of 0.29-0.65, and wherein surfaces of the primary and secondary aspheric mirrors have a non-zero sixth order aspheric parameter.

Hybrid reflective microscope objective

A web gauging system and methods of using the web gauging system are described. The web gauging system includes a supercontinuum Laser providing a light beam. A beam expander is configured to expand the light beam and provide an expanded beam to a sample illumination area. A detector unit configured to detect a sample light from the illumination area. A moving web can be placed in the illumination area, where the web gauging system measures parameters of the web.

Supercontinuum laser based web gauging system

An embodiment of a module system configured to interface with a microscope is described that comprises an input optical fiber configured to provide an excitation light beam from an external light source; dynamic alignment mirrors configured to adjust the position of the beams paths of the excitation light beam on a first plane; a coupling comprising a first end configured to engage with a complementary end, wherein the excitation light reflects off a turning mirror and travels along a beam path on a second plane through an orifice in the coupling; and an output optical fiber for delivering light from a sample to an external detector, wherein the light from the sample travels along the beam path on the second plane through the orifice in the coupling, reflects off the turning mirror and travels along one of the beam paths on the first plane to the output optical fiber.

Raman module for a microscope

An embodiment of a support structure for adjusting the position of a plurality of optical elements is described that comprises a base plate comprising a centering pin, a first translation slot, and a second translation slot; and a translatable plate configured to operatively couple with a plurality of the optical elements and move relative to the base plate, wherein the translatable plate comprises a centering slot configured to engage with the centering pin, a first cam configured to engage with the first translation slot and control movement of the translatable plate along a first axis, and a second cam configured to engage with the second translation slot and control movement of the translatable plate along a second axis.

Support structure and method for focus adjustment

Methods and apparatuses are disclosed whereby structured illumination microscopy (SIM) is applied to a scanning microscope, such as a confocal laser scanning microscope or sample scanning microscope, in order to improve spatial resolution. Particular aspects of the disclosure relate to the discovery of important advances in the ability to (i) increase light throughput to the sample, thereby increasing the signal/noise ratio and/or decreasing exposure time, as well as (ii) decrease the number of raw images to be processed, thereby decreasing image acquisition time. Both effects give rise to significant improvements in overall performance, to the benefit of users of scanning microscopy.

Enhanced sample imaging using structured illumination microscopy

A stray light reducing apparatus includes a light source and an entrance slit positioned to pass through light from the light source. A first monochromator mirror is positioned to reflect light passed through the entrance slit. A diffractive surface is positioned to receive and diffract light reflected by the first monochromator mirror. A second monochromator mirror is positioned to reflect light diffracted by the diffractive surface. An exit slit is positioned to pass through light reflected by the second monochromator mirror. A cuvette is positioned to pass through light passed through the exit slit. A long-pass interference filter is positioned to receive light from the light source, reflect light that has a wavelength below a selected value, and pass through light having a wavelength above the selected value. A first sample detector is positioned to receive light reflected by the long-pass interference filter.

Monochromator with stray light reduction

An image analysis system includes a video camera that collects YUV color images of a liquid sample disposed between a capital and a pedestal, the color images being collected while a light source shines light through an optical beam path between the capital and the pedestal, and a processor adapted to i) obtain from the YUV color images a grayscale component image and a light scatter component image, and ii) obtain at least one binary image of the grayscale component image and at least one binary image of the light scatter component image.

Image analysis system and method

A diffuse reflectance apparatus includes a housing having a window formed therein, and a diffuse reflectance mirror spaced from the window and having an aperture extending therethrough. A light source provides a beam of light. A first mirror assembly is positioned to reflect the beam of light through the aperture such that it passes through the window. A second mirror assembly is positioned to reflect scattered light from the concave mirror to a detector.

Diffuse reflectance apparatus

An embodiment of a calibration element for an analytical microscope is described that comprises a substantially non-periodic pattern of features that exhibit contrast when illuminated by a light beam.

System and method of dimensional calibration for an analytical microscope

An optical device is provided that includes a converging lens device, a transmitting optical fiber, a sample holder, and a receiving optical fiber. The converging lens device focuses light onto the transmitting optical fiber, which receives the focused light through an entrance face and transmits the light from an exit face, through a sample, and onto the receiving optical fiber. The sample holder holds the sample for analysis. The receiving optical fiber receives the light through an entrance face of the receiving optical fiber after transmission through the sample. The converging lens device is positioned to focus the light onto the entrance face of the transmitting optical fiber such that a half-angle of the angular distribution of the focused light that reaches the entrance face of the transmitting optical fiber is selected to underfill an entrance aperture of the entrance face of the receiving optical fiber in both a spatial dimension and an angular dimension.

Optical spectrometer with underfilled fiber optic sample interface

A method and corresponding apparatus provide correction of chemical images collected with a germanium hemisphere ATR microscope. A model is developed for rays passing through a simulated germanium (Ge) hemisphere attenuated total reflection (ATR) microscope. The model determines a data set for rays reaching the detector plane. Movement of the hemisphere is simulated along a first axis between each data set determination. A calculated background spectrum is produced by multiplying the percentage of rays by a background spectrum to produce a calculated background spectrum. A real Ge hemisphere ATR microscope having parameters that substantially match those of the simulated Ge hemisphere microscope is then used to collect a chemical image of a sample that is in contact with the Ge hemisphere. The collected image is then corrected to produce a corrected chemical image.

Correction of chemical image collected using ATR through germanium hemisphere

A Raman optical method and apparatus is utilized to automatically and accurately recognize laser power measurements made at a desired illumination sample plane. From such a configuration, the methods and systems disclosed herein, enable the support of multiple optical wavelengths coupled with essential components, such as, but not limited to, filters, objectives, reflectors, etc., to provide the capability of displaying and controlling the optical power at the desired sample plane through storage of power calibration factors that are associated with such components. In particular, the system utilized herein, can recognize the installation of components and recalls stored calibration factors that are associated with such components to ensure an accurate power measurement at the illuminated sample plane.

Raman spectrometer with display of laser power at the sample

An optical method and apparatus is utilized to provide rapid spatial averaging over a large sample area in a Raman spectrometer, without defocusing of the optical source or the collection optics. Spatial averaging provides a representative spectrum of a sample that is inhomogeneous, either in its composition or surface characteristics. The spatial averaging configurations and methods disclosed herein also reduce sample degradation or burning resulting from the high intensity of the directed optical source. Moreover, the dimensions of the sample area of the spatial averaging methods and configurations of the present invention are adjusted to match specific sampling requirements.

Rapid spatial averaging over an extended sample in a Raman spectrometer

A confocal spectrometer provides astigmatic optics which supply a monochromator or spectrograph with the image of a sample, with the astigmatic optics thereby providing separate first and second (tangential and sagittal) focal planes for the image. The monochromator/spectrograph has an entrance slit oriented along one of the focal planes, and this slit defines the spectral resolution of the monochromator/spectrograph and the field of view of the sample in one direction (in one focal plane). A supplemental slit is situated outside the monochromator/spectrograph adjacent the entrance slit, with the supplemental slit being oriented along the other focal plane. The supplemental slit therefore defines the field of view of the sample in a perpendicular direction (in the other focal plane). By varying the width of the supplemental and/or entrance slits, one may easily achieve the desired field of view.

Growing community of inventors

Madison, WI, United States of America

Francis Jerome Deck