Abstract:
An intracavity laser absorption infrared spectroscopy system for detecting trace analytes in vapor samples. The system uses a spectrometer in communications with control electronics, wherein the control electronics contain an analyte database that contains absorption profiles for each analyte the system is used to detect. The system can not only detect the presence of specific analytes, but identify them as well. The spectrometer uses a hollow cavity waveguide that creates a continuous loop inside of the device, thus creating a large path length and eliminating the need to mechanically adjust the path length to achieve a high Q-factor. In a preferred embodiment, the laser source may serve as the detector, thus eliminating the need for a separate detector.
Abstract:
An electromagnetic wave pulse measuring device, includes an elastic vibration wave generating section which irradiates a predetermined area of a sample with an elastic vibration wave, an electromagnetic wave pulse generating section which irradiates the predetermined area, which is irradiated with the elastic vibration wave, with an electromagnetic wave pulse, and an electromagnetic wave pulse detecting section which measures a waveform of the electromagnetic wave pulse modulated in the predetermined area by the elastic vibration wave. The timing at which the electromagnetic wave pulse detecting section measures the waveform of the electromagnetic wave pulse is a timing at which a phase angle of the elastic vibration wave has a predetermined value when the elastic vibration wave generating section generates the elastic vibration wave.
Abstract:
An optical projection tomography system comprises a support arranged to support an object (63) and to rotate the object between a plurality of orientations, a first imaging system (64) arranged to image the object from a first direction to form a first image, and a second imaging system arranged to image the object from a second direction to form a second image, data acquisition means (66, 67) arranged to acquire image data from the first and second images for each of the orientations and processing means arranged to process the image data to generate an image data set.
Abstract:
The present invention concerns a multicolour excitation module 1 for a multiphoton imaging system 100. Such a module is used for imaging a sample 7 comprising at least three chromophores. The module 1 comprises: a first femtosecond laser source 2, emitting a first excitation beam 20; a second femtosecond laser source 3 emitting a second excitation beam 30. The first excitation beam 20 comprises a so-called "pumping" portion, said pumping portion acting as a pump beam to synchronously excite the second laser source 3, and a so-called "excitation" portion. An optical delay line 4 is arranged to spatially and temporally superpose the second excitation beam 30 and the excitation portion of the first excitation beam, so as to excite at least a third of the chromophores by multiphoton absorption, said absorbed photons coming from the first and second excitation beams 20, 30. The invention also concerns the complete multiphoton imaging system 100, and a method implemented in this module 1.
Abstract:
The invention relates to a nonlinear optical microscope using a Bessel laser beam so as to image a sample with good lateral resolution and extended field depth. This microscope incorporates a slide scanner. The sample is disposed on a slide, which is loaded automatically onto a motorized platen, so that the laser beam can sweep the entire slide. The useful signals originating from the sample are combined with the conventional image of the slide scanner so as to obtain a global image which clearly reveals, with good resolution, elements of interest.
Abstract:
The present invention provides a novel category of naphthalene-based two-photon fluorescent probes having a general formula I, wherein: X is selected from the X 1 , X 2 , X 3 and X 4 ; The mentioned two-photon fluorescent probes have a low fluorescence background in the non-tumor cells and tissues, and have a strong and specific fluorescent signal in the tumor cells and tissues. These probes have a certain level of water-solubility, while having good membrane permeability. In addition, they have a bigger effective two-photon absorption cross section. The compounds of the present invention also have a lower biotoxicity, phototoxicity and photobleaching. There is sufficient difference between the spectral range thereof and that of a biological sample.
Abstract:
The present invention is to present a sample analyzer capable of automatically stabilizing the laser diode in multi-mode oscillation. A sample analyzer 1 comprises: a laser diode (LD) 501d for irradiating a sample with laser light; a photodiode (PD) 501e for detecting amount of light emitted from the LD 501d; a APC circuit 501b for outputting a direct current to be supplied to the LD 501d such that the amount of light emitted from the LD 501d is maintained at a predetermined amount, based on the amount of light detected by the PD 501e; a high frequency oscillation circuit 501f for superimposing a high frequency component on the direct current outputted from the APC circuit 501b; and a high frequency automatic adjustment circuit 501c for controlling amplitude of the high frequency component outputted from the high frequency oscillation circuit 501f according to magnitude of the direct current outputted from the APC circuit 501b such that the LD 501d oscillates in a multi-mode.
Abstract:
Radiation scattering is one of the main contributors to the uncertainty of near infrared (NIR) measurements. Enhanced absorption-measurement accuracy for NIR sensors is achieved by using a combination of NIR spectroscopy and time-of-flight techniques to select photons that are the result of a given mean free path within a moving sample target. By measuring absorption as a function of path length or by windowing signals that are attributable to excessive scattering of NIR radiation within the sample, this technique affords the calculation of more accurate and more universal calibrations. The NIR sensor employs short or ultra-short laser pulses to create NIR that is directed to the moving sample and emerging radiation is detected over time. Windowing effectively truncates non-contributing measurements.
Abstract:
A fluorescence microscope in which spatial resolution is enhanced by performing observation based on the saturation component of fluorescence. The fluorescence microscope comprises a light source (10) emitting laser light to serve as pumping light, an objective lens (13) for focusing the laser light and irradiating a sample with the focused laser light, a detector (22) for detecting fluorescence generated from the sample (14) by the laser light, and a stage (15) performing scanning while varying the relative position of the laser light and the sample (14). The sample is irradiated with laser light while varying the intensity of the laser light such that the fluorescence saturates when the intensity of laser light is the greatest, the fluorescence depending on the intensity of laser light is detected by the detector (22), and observation is performed based on the saturation component of fluorescence.