174 results about "Laser scanning microscope" patented technology

A laser scanning microscope produces molecular excitation in a target material 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 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 fluorescent images of living cells and other microscopic objects. The fluorescent 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. Scanning of the laser beam by a laser scanning microscope, allows construction of images by collecting multi-photon excited fluorescence from each point in the scanned object while still satisfying the requirement for very high excitation intensity obtained by focusing the laser beam and by pulse time compressing the beam. The focused pulses also provide three-dimensional spatially resolved photochemistry which is particularly useful in photolytic release of caged effector molecules, marking a recording medium or in laser ablation or microsurgery. This invention refers explicitly to extensions of two-photon excitation where more than two photons are absorbed per excitation in this nonlinear microscopy.

A method and/or arrangement for the analysis of fluorescing samples in an image-generating microscope system, preferably a laser scanning microscope, wherein the sample is scanned point-by-point or line-by-line in at least one surface section and a dispersive splitting of the radiation coming from the sample is carried out during the scanning, wherein the split radiation is detected by at least one line of detector elements in a wavelength-dependent manner, a selection of two-dimensional or three-dimensional sample parts which correspond to pre-stored two-dimensional or three-dimensional geometric objects or the like is carried out based on the recorded and stored intensity distribution of at least one of these detection elements and/or at least one other detection element for the radiation reflected from the sample by image processing, and an analysis of the spectral signature and/or spatial spectral sequence is carried out for at least a portion of these sample regions with respect to the fluorescence markers arranged thereon.

The invention describes a highly compact laser scanning microscope with integrated short-pulse laser. Direct coupling or a fiber coupling of the short-pulse laser with the laser scanning microscope is advantageously circumvented with this arrangement. This compact arrangement of the laser in the scan module of the laser scanning microscope can be used in a particularly advantageous manner, for example, in multiphoton microscopy for three-dimensionally resolved microscopic analysis, e.g., of biological specimens. Because of the inherent depth discrimination of the multiphoton technique, confocal pinholes can be entirely omitted in the detection beam path. Accordingly, the microscope system can be realized in a very simple manner with respect to engineering and is particularly simple to handle with respect to application. Through the use of a short-pulse laser system in which a plurality of wavelengths are available simultaneously, diverse applications can be realized in one and the same compact microscope system.

The invention relates to a method and apparatus for determining the polarization properties of light emitted, reflected or transmitted by a material using a laser scanning microscope with the tested material being illuminated point by point with a laser beam of known polarization state. According to the invention the light beam with a polarization state modified by the material or the light emitted by the material is being examined by measuring the intensity of two different polarization components of a selected light beam received from each point of said material essentially at the same time and assigning a signal obtained by processing the two intensity signals to a respective point of an image of said material. The apparatus has a polarization state generator between the laser light source and the material being tested, and a detector in a light beam for determining the intensity of light with a polarization state modified by the material or the intensity of light emitted by the material, the improvement of which is that a means for dividing the polarization components in space or time is used in front of the detector.

Apparatus and methods for fluorescence imaging using radiofrequency multiplexed excitation. One apparatus splits an excitation laser beam into two arms of a Mach-Zehnder interferometer. The light in the first beam is frequency shifted by an acousto-optic deflector, which is driven by a phase-engineered radiofrequency comb designed to minimize peak-to-average power ratio. This RF comb generates multiple deflected optical beams possessing a range of output angles and frequency shifts. The second beam is shifted in frequency using an acousto-optic frequency shifter. After combining at a second beam splitter, the two beams are focused to a line on the sample using a conventional laser scanning microscope lens system. The acousto-optic deflectors frequency-encode the simultaneous excitation of an entire row of pixels, which enables detection and de-multiplexing of fluorescence images using a single photomultiplier tube and digital phase-coherent signal recovery techniques.

A method for investigating specimens, wherein a spectral splitting of the radiation coming from the specimen is carried out for specimen points or point distributions, for the operation of a laser scanning microscope or a fluorescence screening arrangement or a flow cylinder comprising the steps of generating a lambd-stack so that the spectral distribution is measured by individual detection channels and storing the signals so as to be correlated to the detection signals with at least one of the spatial coordinates x, y and z and/or so as to be correlated to the measurement time t.

A laser scanning microscope includes an acousto-optic element or an electro-optic element in an illumination optical system which introduces a laser beam from a laser beam source of the laser scanning microscope into a microscope. The laser scanning microscope further includes a beam expander disposed between the laser beam source and the acousto-optic element or the electro-optic element.

A technique is described for performing critical parameter analysis (CPA) of a semiconductor device (DUT) by combining the capabilities of conventional automated test equipment (ATE) with a focused optical beam scanning device such as a laser scanning microscope (LSM). The DUT is provided with a fixture such that it can be simultaneously scanned by the LSM or a similar device and exercised by the ATE. The ATE is used to determine pass/fail boundaries of operation of the DUT. Repeatable pass/fail limits (for timing, levels, etc.) are determined utilizing standard test patterns and methodologies. The ATE vector pattern(s) can then be programmed to “loop” the test under a known passing or failing state. When light energy from the LSM scanning beam sufficiently disturbs the DUT to produce a transition (i.e., to push the device outside of its critical parameter limits), this transition is indicated on the displayed image of the DUT, indicating to the user which elements of the DUT were implicated in the transition.

For the purpose of calibration which is simple and can also be carried out as often as desired, an arrangement and a method for calibrating a preferably confocal laser scanning microscope, it being possible for an object (1) to be scanned by a scanning beam (2), are defined by calibration means (12) which are arranged in the plane of an intermediate image (11) and can likewise be scanned by the scanning beam (2).

A method of finding, recording and optionally evaluating object structures, especially on slides, preferably of fluorescent object structures such as gene spots. A microscope with a CCD camera, a scanning microscope or a preferably confocal laser scanning microscope can be used for recording and for the rapid and reliable detection of the object structures, with the image data being recorded using an illumination pattern that is projected into the object plane.

In a confocal laser scanning microscope with an illuminating configuration (2), which provides an illuminating beam for illuminating a specimen region (23), with a scanning configuration (3, 4), which guides the illuminating beam over the specimen while scanning, and with a detector configuration (5), which via the scanning configuration (3, 4) images the illuminated specimen region (23) by means of a confocal aperture (26) on to at least one detector unit (28), it is provided that the illuminating configuration (2) of the scanning configuration (3, 4) provides a line-shaped illuminating beam, that the scanning configuration (3, 4) guides the line-shaped illuminating beam over the specimen f while scanning and that the confocal aperture is designed as a slit aperture (26) or as a slit-shaped region (28, 48) of the detector unit (28) acting as a confocal aperture.

A Device for coupling a short pulse laser into a microscope beam path, wherein the spectral components of the laser radiation are spatially separated by means of a dispersive element, the individual spectral components are manipulated and are then spatially superimposed again by means of another dispersive element.

A scanning optical microscope using a wavefront converting element suffers minimum off-axis performance degradation and allows the wavefront converting element to be controlled by a simple method. Further, a pupil relay optical system is simple in arrangement or unnecessary. A laser scanning microscope includes a laser oscillator and a wavefront converting element for applying a desired wavefront conversion to a laserbeam emitted from the laser oscillator. An objective collects a wavefront-converted approximately parallel laser beam emerging from the wavefront converting element onto a sample. A detector detects signal light emitted from the sample. An actuator scans the objective along a direction perpendicular to the optical axis.

A method for controlling laser scanning microscopy of a probe comprising at least one cell is disclosed. The method comprises the steps of acquiring at least one initial image of the probe and identifying at least one cell within an initial probe image. Using a pre-defined grammar, a first set of scanning mode parameters for monitoring the cell(s); a first set of trigger parameters including at least one physiological parameter defining an event in the cell(s); and a second set of scanning mode parameters for monitoring at least one cell of the probe after an occurrence of the event is defined. A successive set of probe images acquired according to the first set of scanning mode parameters is provided and processed to determine if the event has occurred. Responsive to the event occurring, microscope modality is changed to the second set of scanning mode parameters.

A method is disclosed for operation of an image-generating optical system for detection of characteristic quantities of the wavelength-dependent behavior of an illuminated specimen, such as the emission behavior and/or absorption behavior and, in particular, the fluorescence and/or luminescence and/or phosphorescence and/or enzyme-active light emission and/or enzyme-active fluorescence, for the operation of a laser scanning microscope, comprising the steps of splitting the image point information of the specimen into spectral components in a spatially resolved manner on the detection side in dependence on wavelength and carrying out at least one summing for different spectral components.

Laser-scanning microscope with at least one detection radiation input, in which an aperture plate is installed in front of the detector, whereby optics with variable transmission lengths and a fixed focal distance is provided for focusing varying wavelengths of the detected light onto the aperture plate level at the detection radiation path, which realizes the imaging from the infinite space into an image level with a finite conjugate distance,

and/or

with at least one light source launched via an optical fiber, whereby collimator optics with a fixed focal distance, and a variable conjugate distance are down-streamed from the fiber output, which transfers the point source at the fiber output with a numerical aperture into a parallel beam in the infinite space in front of the scan-objective lens, whereby a wavelength-dependent, at least partial compensation of the chromatic distortion of the micro-objective lenses occurs by means of turning the chromatic curve for the illumination wavelength used.

A calibration device for managing a variety of performance tests and/or calibration tasks in a laser scanning microscope. The calibration device, which has focusing optics and a test structure arranged in the focal plane of the focusing optics, with structural elements detectable in reflected and/or transmitted light aligned to each other in a common mounting, can be switched into the microscope beam path in a laser scanning microscope, so that the pupil of the focusing optics coincides with the objective pupil of the laser scanning microscope or lies in a plane conjugated to it.