Abstract:
A device (1; 10; 20; 30; 40) for optically examining the interior of a turbid medium is provided. The device comprises an illumination system (2; 12; 22; 32; 42) adapted for illuminating a turbid medium to be examined and an imaging device (106) adapted for generating images from detected light. The illumination system (2; 12; 22; 32; 42) is adapted to be operable in at least a first mode in which a large area is illuminated and a second mode in which at least one selected region (110) of the large area is illuminated.
Abstract:
An optical inspection system or tool can be configured to inspect objects using dynamic illumination where one or more characteristics of the illumination is/are adjusted to meet the inspection needs of different areas. For example, the illumination intensity may be increased or decreased as the tool inspects areas of memory and periphery features in a wafer die. In some embodiments, the adjustment can be based on data obtained during a pre-inspection setup sequence in which images taken based on illumination with varying characteristics are evaluated for suitability in the remainder of the inspection process.
Abstract:
An optical phantom produces a time-resolved diffuse reflectance spectrum and includes: a light source; a spatial light modulator; and an optical delay line including optical fibers of different length that produce different time-of-flight distributions, such that different time-of-flight distributions are combined and produce phantom light having the time-resolved diffuse reflectance spectrum.
Abstract:
An apparatus for detecting a material within a sample includes a light emitting unit for directing at least one light beam through the sample. A plurality of units receive the light beam that has passed through the sample and performs a spectroscopic analysis of the sample based on the received light beam. Each of the plurality of units analyze a different parameter with respect to the sample a provide a separate output signal with respect to the analysis. A processor detects the material with respect each of the provided separate output signals.
Abstract:
A super-resolution scanning confocal polarisation contrast microscope is provided. The microscope has a laser light source (1), sample stage (10) for mounting a sample 6 and detector (8). A polarisation controller (3) is used to set the polarisation state of the light beam to any one of a defined set of different polarisation states. A spatial light modulator (5) modulates the light beam in amplitude and/or phase to focus a sub-diffraction-limit central spot on the sample together with unwanted sidebands. A scanning confocal scheme is used with a pin hole 9 in front of the detector (8) so that only that portion of the light is detected which has comes from the central spot, while rejecting light that has been scattered by the sample from the sidebands. Polarisation contrast images with sub-diffraction limit resolution can thus be acquired.
Abstract:
A super-resolution observation device includes an illumination optical system collecting a first illuminating light having a first optical frequency co, on a first region of an observation object, collecting a second illuminating light having a second optical frequency ω2′ on a second region partially overlapping the first region, and collecting a third illuminating light having a third optical frequency ω2 on a third region containing a non-overlap region which is a region of the first region and does not overlap the second region; and an extraction unit extracting a signal light generated in accordance with a change in an energy level of a substance in the non-overlap region from a light generated in all of the first region, the second region, and the third region.
Abstract:
An imaging device includes a camera 31, a light source 32, a polarizer 35 arranged between the camera 31 plus the light source 32 and an object 11, and a spatial light modulator 40A arranged between the polarizer 35 and the object 11 to control a revolution angle of an emitting light polarization plane relative to an incident light polarization plane.
Abstract:
Systems and methods are disclosed to enhance three-dimensional photoacoustic imaging behind, through, or inside a scattering material. Embodiments of the invention can increase the optical fluence in an ultrasound transducer focus and/or enhance the optical intensity using wavefront shaping before the scatterer. The photoacoustic signal induced by an object placed behind the scattering medium can serve as feedback to optimize the wavefront, enabling one order of magnitude enhancement of the photoacoustic amplitude. Using the enhanced optical intensity, the object can be scanned in two dimensions and/or a spot can be scanned by re-optimizing the wavefront before post-processing of the data to reconstruct the image. The temporal photoacoustic signal provides information to reconstruct the third-dimensional information.
Abstract:
Excitation light is focused to a focus within a sample and the focus is scanned within a volume in the sample with scanning optical elements. Signal light emitted from the focus is de-scanned, with the one or more scanning optical elements, onto a wavefront sensor as the focus is scanned within the volume. Based on the descanned signal light, an average aberration created by the volume of the sample of a wavefront of the excitation light is determined. A wavefront of the excitation light is corrected by an amount according to the determined average aberration while the focus is scanned within the volume, the signal light is imaged onto a photosensitive detector as the focus is scanned within the volume, and a wavefront of the imaged signal light is corrected by an amount according to the determined average aberration while the focus is scanned. These steps can be repeated for a plurality of different volumes in the sample, and an image of the sample can be generated based on the detected signal light from scanned foci within the different volumes.