Abstract:
Innovative techniques that result in a better signal-to-noise ratio for spectrographic analysis of substances in a target than conventional techniques. In these techniques, light illuminates a target with at least some of the light penetrating the target. At least a portion of the light that penetrates the target is collected from a region on the target's surface that is not directly illuminated. Preferably, at least a majority of the collected light is light that penetrates the target. Also preferably, the light that illuminates the target is in a pattern that partially but not completely surrounds the region from which the portion of the light that penetrates the target is collected. A spectrum of at least a portion of the collected light is analyzed.
Abstract:
Raman-enhancing structures include a photonic crystal having a resonant cavity and at least one waveguide coupled to the resonant cavity. A nanostructure comprising a Raman-enhancing material is disposed proximate the resonant cavity of the photonic crystal. Raman-enhancing structures include a microdisk resonator, at least one waveguide coupled to the microdisk resonator, and a nanostructure comprising a Raman-enhancing material disposed proximate the microdisk resonator. Methods for performing Raman spectroscopy include generating radiation, guiding the radiation through a waveguide to a resonant cavity in a photonic crystal or a microdisk resonator, resonating the radiation in the resonant cavity or microdisk resonator, providing an analyte proximate the resonant cavity or microdisk resonator, subjecting the analyte to the resonating radiation, and detecting Raman scattered radiation.
Abstract:
The present invention relates to methods of detecting analytes using nanowires having nanodisk arrays. In particular, the present invention discloses methods of detecting analytes via surface enhanced Raman scattering (SERS) and employing nanowires prepared using on-wire lithography (OWL).
Abstract:
A system and method of correlating Raman measurements with digital images of a treated sample to classify the disease state of the sample. A spectroscopic data set is obtained for the sample positioned in the field of view of a spectroscopic device. Information about the field of view is stored. The sample is removed from the field of view and treated. The treated sample is repositioned in the field of view using the stored information. A digital image of the treated sample is obtained and the spectroscopic data set is linked with the digital image. A database is provided having a plurality of spectroscopic data sets. Each data set is linked to a corresponding digital image, and associated with the known sample. Each corresponding digital image is associated with the known treated samples. The database is searched to identify and match a data set of a known sample and the sample.
Abstract:
A material which is generally transparent in the visible region of the spectrum but reflective at laser wavelengths reduces undesirable, substrate-induced Raman and fluorescence scattering. A substrate provides a surface for supporting the sample, with the material being disposed between the surface of the substrate and the sample. The material is substantially transparent in the visible region of the spectrum but reflective at the laser wavelength, thereby minimizing unwanted Raman or fluorescence scattering that would be produced by the substrate if the material were not present. The substrate will typically be a glass microscope slide or multi-cell well plate. The optical filter material is preferably a multilayer dielectric filter acting as a “hot mirror” that reflects near-infrared energy. An advantage of visible transmission is that it allows back illumination from behind/underneath the slide or well plate, thereby being visible to a microscope's eyepiece or video camera. Methods and article are also disclosed.
Abstract:
In one or more embodiments, a microscope has a first pulsed laser and a second pulsed laser arranged to irradiate a specimen. Coherent Raman scattering light emanated from the irradiated specimen is extracted, along with multiphoton excitation fluorescence and a second harmonic wave. One or more detectors detect the extracted coherent Raman scattering light, the extracted fluorescence, and the second harmonic wave. A single specimen can simultaneously be observed with respect to either parallel or selective observations of the two-photon excitation fluorescence, the second harmonic wave, and the coherent Raman scattered light.
Abstract:
A photodetection device, a photodetection method, an image sensor and an image pickup method can increase the number of pixels, while suppressing degradation of the S/N ratio. The photodetection device includes a spectroscopic element formed by means of an optical microresonator having a plurality of resonant wavelength bands differentiated by positions as a function of a geometric structure and a plurality of photoelectric conversion elements arranged at different positions to detect light of the plurality of resonant wavelength bands.
Abstract:
Nanostructures configured to enhance the intensity of Raman scattered radiation scattered by an analyte include a substantially planar substrate, a plurality of nanoparticles disposed on a surface of the substrate, and a Raman-enhancing material disposed on at least a portion of at least one nanoparticle. Each nanoparticle is configured to emit lased radiation upon stimulation of the nanoparticle and may comprise a nanowire laser. Raman spectroscopy systems include a radiation source, a radiation detector configured to detect Raman scattered radiation scattered by an analyte, a nanostructure including at least one nanoparticle configured to emit lased radiation upon stimulation, and means for stimulating the nanoparticle. Methods for performing Raman spectroscopy include providing a nanostructure including at least one nanoparticle configured to emit lased radiation upon stimulation of the nanoparticle, providing an analyte proximate to the nanoparticle, stimulating the nanoparticle, and detecting Raman scattered radiation.
Abstract:
Disclosed herein are Raman probes that include: (a) a first optical fiber for receiving laser excitation light from a light source and transmitting the same; (b) a first filter for receiving light from the first optical fiber and adapted to pass the laser excitation light and to block spurious signals associated with the light; (c) a second filter for receiving light from the first filter and adapted to direct the light toward a specimen; and (d) focusing apparatus for receiving the light from the second filter, focusing the light on the specimen so as to generate the Raman signal, and returning the Raman signal to the second filter. The second filter is further configured so that when the second filter receives the Raman signal from the focusing apparatus, the second filter filters out unwanted laser excitation light before directing the Raman signal to a second optical fiber.
Abstract:
The invention relates to a method and a device for producing and detecting a Raman spectrum. The problem addressed by the present invention is that of devising a method and a device for producing and detecting a Raman spectrum of a medium under investigation, whereby the Raman spectrum of a medium that is under investigation can be examined with a high degree of sensitivity while requiring relatively little equipment. The method is characterized by the coupling of excitation radiation into a medium (8) under investigation and the coupling of the electromagnetic radiation scattered by the medium (8) under investigation into a spectral optic system (10), a laser diode (1) for generating excitation radiation with at least two different wavelengths (λ1, λ2) being controlled with at least two different excitation conditions and at least one Raman spectrum (16, 17) being detected in each case from the scattered radiation at the different excitation wavelengths (λ1, λ2), and the Raman spectrum (20) of the medium (8) under investigation being determined from the at least two detected Raman spectra (16, 17), the two different excitation conditions for the laser diode (1) being adjusted by means of the electric current supplied to the laser diode (1).