Abstract:
In a method of observing a specimen through a fluorescence microscope, molecules that could cause double-resonance absorption process in an appropriate manner are used to dye the specimen, and the specimen is irradiated with a plurality of light beams of different wavelengths in a good timing, so that a microscopic image with high spatial resolution is obtained. In the microscope to be used in the method of observation, the specimen is irradiated with two light beams of different wavelength bands via an aperture with an annular-zonal structure and an optical system that has different in-focus positions for these two wavelength bands, so that one of the two light beam is focused on a surface of the specimen and the other light beam is defocused thereon. Consequently, the microscope achieves improvement of the spatial resolution as to overcome the diffraction limit determined by the wavelengths in use.
Abstract:
Provided is a nonlinear optical microscope capable of improving the spatial resolution. The nonlinear optical microscope includes: an illuminating part for irradiating, through an objective lens, a sample with at least two colors of illumination light beams spatially and temporally overlapping each other; and a detecting part for detecting signal light generated from the sample due to nonlinear optical effect, the signal light resulting from the irradiation of the sample with the at least two colors of illumination light beams, in which the illuminating part irradiates the sample with the two colors of illumination light beams in which at least one of the illumination light beams has a wavefront distribution different from a wavefront distribution of the other one of the illumination light beams.
Abstract:
A surface analyzing apparatus includes a laser plasma radiation source, an optical condensing system for converging ultraviolet light, vacuum ultraviolet light, or X rays emitted from the laser plasma radiation source on the surface of a sample, and a mass spectrometer or a time-of-flight spectrometer for detecting the secondary ions emitted from the sample. Thus, the surface analyzing apparatus is capable of analyzing two-dimensionally adsorbed substances on the sample surface with a high resolving power.
Abstract:
A microscope capable of being shaped into a beam with complete hollow shape by removing the disorder of the wavefront to the erase light, particularly, and capable of improving the spatial resolution by inducing a super-resolution near the limit, is provided. In the microscope, wherein a first light to excite a molecule from a ground-state to first electron excited state or a second light to excite the molecule from the first electron excited state to the second electron excited state with higher energy level, for a sample 56 including the molecule with three electronic states including at least a ground-state, are spatial phase-modulated into the prescribed beam shape, and parts of these first light and the second light are overlapped and focused to detect luminescence from the sample 56, a wavefront compensation means 61 is provided in the optical path of the first light and/or in the optical path of the second light, and the wavefront aberration caused in the first light and/or in the second light, is removed by the wavefront compensation means 61.
Abstract:
A high-accuracy multi-wavelength optical microscope for providing a satisfactory contrast of image and much information about a sample. The microscope includes a plurality of light sources, a wavelength varietor independently varying the wavelength of the individual light sources, and polarization plane rotators on the optical path for each light source.
Abstract:
A vacuum optical system has a vacuum chamber for housing an optical system used in a vacuum. The vacuum chamber is equipped with a member, on which the optical system is at least mounted, supported by such parts that when a pressure in the vacuum chamber changes to deform the vacuum chamber, the amount of displacement transmitted to the optical system is smaller than a predetermined tolerance depending on an accuracy necessary for the optical system. Thus, the vacuum optical system can be obtained which does away with the need for readjustment of optical alignment and is compact.
Abstract:
The present invention provides an optical microscope capable of suppressing unnecessary response light as a background and detecting desired response light in nonlinear optical response process with a good S/N ratio. The optical microscope for collecting, on a sample 8, stimulation light emitted from a stimulation light source 1 and having a single wavelength or a plurality of different wavelengths, and detecting response light emitted from the sample 8 in nonlinear optical response process, comprises: an erase light source 2 for emitting erase light having a wavelength different from that of the stimulation light and inducing an effect of suppressing secondary response light which appears due to irradiation of the stimulation light on the sample 8, wherein the erase light and the stimulation light are simultaneously irradiated on the sample 8 such that the erase light does not suppress response light emitted from a light-collecting area of the stimulation light but suppresses the secondary response light other than the response light emitted from a light-collecting area of the stimulation light.
Abstract:
A microscope for observing a sample containing a substance having at least two excited quantum states includes a pump light source 21 for emitting pump light, an erase light source 22 for emitting erase light, a light combining section 23 to 26 for coaxially combining the pump light and the erase light, a light collecting section 62 for collecting the combined lights, a scanning section 44 and 45 for scanning the sample with the combined lights, a detecting section 50 for detecting photoresponsive signals generated from the sample, a wavelength selecting element 42 arranged in the light path of the combined lights and provided with an erase light selecting region having a high wavelength selectivity for the erase light and with a pump light selecting region having a high wavelength selectivity for the pump light, and a space modulating element 43 arranged in the light path of the combined lights for spatially modulating the erase light corresponding to the erase light selecting region of the wavelength selecting element.
Abstract:
A method for observing a sample containing photochromic molecules having a quantum state of at least a first stable state S0 and a second stable state S3. Used are first light for exciting the photochromic molecules from the first stable state S0 to a first excited state S1 enabling optical response, and second light for exciting the photochromic molecules from the first excited state S1 to a second excited state S2 of another energy level. The sample is irradiated with the first light and the second light partly overlapping each other so that the photochromic molecules in the region irradiated with the overlapping first and second lights are transformed through the second excited state S2 to the second stable state S3, and the photochromic molecules in the region irradiated with the first light only are transformed to the first excited state S1, thereby observing the sample.
Abstract:
[Task] To provide a super-resolution microscope whereby the light source of pump light and erase light can be selected easily and a super-resolution can be reliably achieved through a simple and inexpensive arrangement. [Solution of the Task] A super-resolution microscope includes an optical system (3, 4, 9) for combining a part of a first coherent light from a first light source (2) and a part of a second coherent light from a second light source (1) and focusing the coherent lights onto a sample (10), scanning means (6, 7) for scanning the coherent lights, and detecting means (16) for detecting an optical response signal from the sample (10). The microscope is configured so as to satisfy the following conditions: σ01Ipτ≦1, and 0.65(λe/λp)≦τσdipIe where λp is the wavelength of the first coherent light, λe is the wavelength of the second coherent light, τ is the excited lifetime in which the molecule is excited by the first coherent light from the ground state to the first electron-excited state, Ip is the maximum photon flux on the sample surface of the first coherent light, Ie is the maximum photon flux on the sample surface of the second coherent light, σ01, is the absorption cross-sectional area when the molecule is exited from the ground state to the first electron-excited state, and σdip is the fluorescence suppression cross-sectional area.