Abstract:
An apparatus for producing optical pulses of a desired wavelength includes an optical pulse source operable to generate input optical pulses at a first wavelength, and a higher order mode (HOM) fiber module operable to receive the input optical pulses at the first wavelength, and thereafter to produce output optical pulses at the desired wavelength by soliton self-frequency shift (SSFS). The present invention also relates to a method of producing optical pulses having a desired wavelength. This method includes generating input optical pulses using an optical pulse source, where the input optical pulses have a fist wavelength and a first spatial mode. The input optical pulses are delivered into an HOM fiber module to alter the wavelength of the input optical pulses from the first wavelength to a desired wavelength by soliton serf-frequency shift (SSFS) within the HOM fiber module, thereby producing output optical pulses having the desired wavelength.
Abstract:
Apparatus and methods relating to non-imaging, multiphoton fluorescence and optical second harmonic generation (SHG) (and higher harmonic generation) emission and detection. A weakly focused excitation beam is used to generate fluorescence emission in a volume of between about 0.1 cm 3 to one cubic centimeter (1 cm 3 ), which is significantly larger than the conventional MPM focal volume. A method for shaping and/or controlling (confining) the focal volume of a non-imaging, fluorescence emission excitation field in a target medium involves decoupling the axial dimension dependence of the focal volume from the lateral spot size of the excitation field. The method involves the step of spatially separating at least some of the spectral components of a short duration, multichromatic excitation field outside of the focal volume and spatially recombining the spectral components in a short duration, high intensity, weakly focused field incident on the target medium. The apparatus and methods described herein are particularly suitable for, but not limited to, non-invasive, in-vivo biological assay and disease state indication in target tissue and, more particularly, to potential early detection of Alzheimer's and other diseases.
Abstract:
Embodiments of the invention include an optical system and an optical system module, coupled to a distal end of a fluorescence emission endoscope apparatus, an optical waveguide-based fluorescence emission endoscopy system, and a method for remotely- controlled, multi -magnification imaging of a target or fluorescence emission collection from a target with a fluorescence emission endoscope apparatus. An exemplary system includes an objective lens disposed in a distal end of an endoscope apparatus. The lens is adapted to transmit both a visible target illumination and a fluorescence-emission-inducing target illumination as well as fluorescence-emission and visible light from the target. Thee system can thus simultaneously provide low magnification, large field of view imaging and high magnification, high-resolution multiphoton imaging with a single lens system.
Abstract:
A technique for simultaneous spatial and temporal focusing of femtosecond pulses improves the signal-to-background ratio (SBR) in multiphoton imaging. This is achieved by spatially separating spectral components of pulses into a "rainbow beam" and recombining these components at the spatial focus of an imaging system (100). The temporal pulse width becomes a function of distance, with the shortest pulse width confined to the spatial focus. The technique can significantly improve the axial confinement and reduce the background excitation in multiphoton microscopy, and thereby increase the imaging depth in highly scattering biological specimens.
Abstract:
The present invention includes an apparatus and method for producing optical pulses of a desired wavelength. The apparatus includes an optical pulse source operable to generate input optical pulses at a first wavelength. The apparatus further includes a higher-order-mode (HOM) fiber module operable to receive the input optical pulses at the first wavelength, and thereafter to produce output optical pulses at the desired wavelength by exciting Cherenkov radiation using the input optical pulses. The present invention also relates to a method of producing optical pulses having a desired wavelength, where the input optical pulses have a first wavelength and a first spatial mode and the output optical pulses have a second wavelength and a second spatial mode, which may be converted to another spatial mode.
Abstract:
A laser scanning micrsocope (10) produces molecular excitation in a target material (14) by simultaneous absorption of three or more photons to thereby provide intrinsic three-dimensional resolution. Fluorophores having single photon absorption in the short (ultraviolet or visible) wavelength range are excited by a beam (16) of strongly focused subpicosecond pulses of laser light of relatively long (red or infrared) wavelength range. The fluorophores absorb at about one third, one fourth or even smaller fraction of the laser wavelength to produce fluoroscent images of living cells and other microscopic objects. The fluoroscent emission from the fluorophores increases cubicly, quarticly or even higher power law with the excitation intensity so that by focusing the laser light, fluorescence as well as photobleaching are confined to the vicinity of the focal plane. This feature provides depth of field resolution comparable to that produced by confocal laser scanning microscopes, and in addition reduces photobleaching and phototoxicity.
Abstract:
A fluorescence emission imaging method and apparatus allows for high frame rate imaging in scattering medium as well as for fluorescence, phosphorescence, or luminescence lifetime imaging, time-resolved fluorescence, phosphorescence, or luminescence lifetime spectroscopy and imaging. A method involves providing an illumination beam, propagating the illumination beam to a light modulator array, modulating the illumination beam so as to generate an array of point sources, wherein each of the point sources is modulated at a frequency, imaging the modulated illumination beam on the object, and detecting a fluorescent, phosphorescent, or luminescent emission from the object. An optical imaging component in the form of a modulation mask has multiple bands. Each band has alternating transmissive and/or reflective and/or absorptive regions that are patterned such that light scanned over a band will be modulated at a band-related frequency.
Abstract:
The present invention includes an apparatus and method for producing optical pulses of a desired wavelength. The apparatus includes an optical pulse source operable to generate input optical pulses at a first wavelength. The apparatus further includes a higher-order-mode (HOM) fiber module operable to receive the input optical pulses at the first wavelength, and thereafter to produce output optical pulses at the desired wavelength by exciting Cherenkov radiation using the input optical pulses. The present invention also relates to a method of producing optical pulses having a desired wavelength, where the input optical pulses have a first wavelength and a first spatial mode and the output optical pulses have a second wavelength and a second spatial mode, which may be converted to another spatial mode.
Abstract:
The present invention relates to an apparatus for producing optical pulses of a desired wavelength. The apparatus includes an optical pulse source operable to generate input optical pulses at a first wavelength. The apparatus further includes a higher order mode (HOM) fiber module operable to receive the input optical pulses at the first wavelength, and thereafter to produce output optical pulses at the desired wavelength by soliton self- frequency shift (SSFS). The present invention also relates to a method of producing optical pulses having a desired wavelength. This method includes generating input optical pulses using an optical pulse source, where the input optical pulses have a first wavelength and a first spatial mode. The input optical pulses are delivered into an HOM fiber module to alter the wavelength of the input optical pulses from the first wavelength to a desired wavelength by soliton self- frequency shift (SSFS) within the HOM fiber module, thereby producing output optical pulses having the desired wavelength.