Hamamatsu-photonics K.k.

Hamamatsu Photonics Kabushiki Kaisha

Artnow Ltd.

Tamiki Takemori

Yutaka Tsuchiya

Takashi Inoue

Shinichiro Aoshima

Yuu Takiguchi

Naoya Matsumoto

Norihiro Fukuchi

Takahiro Ikeda

Naohisa Mukozaka

Hironori Takahashi

Tsuneyuki Urakami

Tsutomu Hara

Yuji Kobayashi

Isuke Hirano

Naohisa Mukohzaka

Narihiro Yoshida

Makoto Hosoda

Kenji Kon

Katsuyoshi Fujita

A laser processing apparatus including a laser light source, a phase modulation type spatial light modulator, a driving unit, a control unit, and an imaging optical system. A storage unit that is included in the driving unit stores a plurality of basic holograms corresponding to a plurality of basic processing patterns and a focusing hologram corresponding to a Fresnel lens pattern. The control unit arranges in parallel two or more basic holograms selected from the plurality of basic holograms stored in the storage unit, overlaps the focusing hologram with each of the basic holograms arranged in parallel to form the whole hologram, and presents the formed whole hologram to the spatial light modulator.

Laser emitting apparatus using a basic hologram and a focusing hologram

A laser processing apparatusincludes a laser light source, a phase modulation type spatial light modulator, a driving unit, a control unit, and an imaging optical system. The imaging optical systemmay be a telecentric optical system. A storage unitA included in the driving unit stores a plurality of basic holograms corresponding to a plurality of basic processing patterns and a focusing hologram corresponding to a Fresnel lens pattern. The control unitarranges in parallel two or more basic holograms selected from the plurality of basic holograms stored in the storage unitA, overlaps the focusing hologram with each of the basic holograms arranged in parallel to form the whole hologram, and presents the formed whole hologram to the spatial light modulator

Laser processing apparatus and laser processing method

A three-dimensional image displaying apparatus comprises a spatial light modulation element having a discrete pixel structure and expressing a hologram, an illumination optical system generating reconstruction light by causing illumination light to enter said spatial light modulation element that expresses the hologram, and a lens as a reconstruction image converting optical system displaying a reconstruction image by producing a virtual image wavefront-converted from the reconstruction light.

Three-dimensional image display and three-dimensional image displaying method

A small, inexpensive three-dimensional image display having a structure for displaying a color three-dimensional image sharply even if a low-resolution spatial optical modulating element is used. The three-dimensional image display has an illumination light source unit, a transmission spatial optical modulating element, a lens, and a mask. The illumination light source unit includes three point light sources outputting illumination light components having wavelengths (red, green, blue) different from one another. The point light source outputting the blue illumination light component of the shortest wavelength is disposed in position B() on the optical axis of an illumination optical system, the point light source outputting the red illumination light component is disposed in position R(x), and the point light source outputting the green illumination light component is disposed in position G(x). An aperture section of the mask is disposed in the region where the zero-order diffracted waves of the reproduction light components of the three wavelengths after subjected to wavefront conversion by the lens are superposed on one another. The illumination optical system determines the direction of incidence of each of the illumination optical components of the three wavelengths on the spatial optical modulation element.

3D image display and 3D image display method

In the method for producing holograms, a plurality of images displayed on a spatial optical modulating elementis used as the object light. Through a lens arraycomposed of a plurality of lenses disposed corresponding to each of the images, which are included in the object light, and a reducing optical systemandfor reducing the object light emitted from the lens array, the object light is made to irradiate a recording surfacealong with a reference light; thereby interference light between the object light and the reference light is recorded on the recording surface. Between the spatial optical modulating elementand the lens array, partitionsfor separating the respective images are provided; thereby noise is reduced.

Hologram preparing method

Used as a propagation function is a half-plane propagation function which is restricted such that it has a value only within a half plane in a predetermined direction perpendicular to a propagating axis in a plane which is perpendicular to the propagating axis. According to a convolution integration with this function, the wavefront of object light on a hologram surface is determined, whereby hologram data is produced. Thus produced hologram is read out by means of readout light. After the light with a wavefront forming the conjugate image of the object to be viewed is blocked, the image of the object to be viewed is observed. Thus, a hologram, which has a high quality and from which the conjugate image is easily eliminated at the time of image reproduction, is produced while a recording device with a relatively low spatial resolution is used, and a three-dimensional form is displayed while the distortion with respect to the original image is reduced in thus produced hologram and the conjugate image is eliminated therefrom.

Apparatus and method for producing hologram and apparatus and method for

A diaphragm having an aperture, the size of which is equal to or smaller than .lambda.f/p (.lambda. is the wavelength, p is the imaging resolution, and f is the focal length of an imaging optical system) is arranged on the focal plane of the object space of the imaging optical system, and object light via the aperture is imaged by the imaging optical system. The object light via the imaging optical system and reference light are brought to interference to form interference fringes, and an image of the interference fringes is sensed. Using the hologram sensed in this manner, the image of the object to be sensed is reconstructed by adopting an imaging optical system equivalent to that upon imaging, and setting the positional relationship between the formed hologram and the imaging optical system in correspondence with that between the imaging optical system and the imaging surface upon imaging. In this way, a holography imaging apparatus which can vary the field of view and can sense a high-quality hologram using an imaging device having a relatively low spatial resolution is realized, and a holography display apparatus which can display an image by eliminating distortion with respect to the original image from a hologram sensed by the holography imaging apparatus of this invention is realized.

Holography imaging apparatus holography display apparatus holography

An optical digital holding apparatus of the present invention carries out functions of a flip-flop apparatus (RS flip-flop, D flip-flop etc.) which are one kind of electrical digital holding apparatus, and can be achieved by placing optical connecting wiring having a direct or indirect feedback circuit between multistage optical selectors having selector functions. The optical digital holding apparatus of the present invention includes multistage selectors which receive an aggregation of spatially distributed optical digital information signals propagating in a predetermined direction and bearing binary digital information and an optical control signal bearing binary digital information. These selectors selectively output a portion of an aggregation of the digital information signals received in accordance with a value of the digital information carried by the optical control signal. The optical digital holding apparatus also includes optical connection wiring for connecting an output optical signal of one of the selectors to an input optical signal of one of the other selectors.

Optical digital holding apparatus

Operation results for all combinations of input optical signal values to be operated are previously determined and substantially parallel light beams reflecting the operation results for all combinations are generated. Selectors for selecting transmission area of the input light beams in accordance with digital information born by optical signals are arranged for the respective optical signals along the direction of propagation of the light beams. Through the logically cascade-connected selectors, an optical signal corresponding to a combination of current input optical signals is selected from the operation results for all combinations.

Optical digital apparatus

Young's interferometer consisting of a single slit and a double slit member, and an analyzer are arranged along the axis of light to be measured. Parallel slits of the double slit member are provided with respective polarizers whose paralyzing directions are at .+-.45.degree. to the longitudinal direction of the parallel slits. The polarizing direction of the analyzer is set in parallel with the parallel slits. The incident light passes through Young's interferometer and the analyzer to form an interference fringe, which is detected by an image detector unit. An image analyzer unit produces an intensity profile of the interference fringe and determines the polarization state of the incident light, for instance, by comparing the produced intensity profile with conceivable profiles stored in advance.

Polarized light measuring apparatus and phase plate measuring apparatus

An object is typically illuminated by laser light, and reflected light carrying a speckle pattern is amplified by an image intensifier. First and second speckle patterns representing the object before and after its deformation, respectively are written by double writing into a ferroelectric liquid crystal spatial light modulator (FLC-SLM). The double-written image is read out from the FLC-SLM, and converted by a Fourier transform optical system into an output optical image, i.e., Young's fringe. The output optical image is detected by a photoelectric converter, and analyzed by an image processing device to determine a deformation of the object.

Optical deformation measuring apparatus by double-writing speckle images

A deformation measuring method and device in which an object is irradiated with a laser beam before and after deformation of the object to obtain speckle patterns, the speckle patterns thus obtained are photoelectrically converted into electrical signals, and the cross-correlation function between the speckle patterns is calculated using the electrical signals to obtain displacement of the speckle pattern on the basis of the shift of position of the extreme value of the cross-correlation function and to determine the amount of deformation of the object from the displacement of the speckle pattern. Each of photosensitive elements for converting the speckle patterns into the electrical signals has a rectangular form of a large ratio of a long side to a short side and a photosensitive element array comprising the photosensitive elements has a comb structure in which the photosensitive elements having the above structure are arranged in a strip form.

Deformation measuring method and device using comb-type photosensitive

In a deformation measuring method and device in which an object is irradiated with a laser beam before and after deformation of the object to obtain speckle patterns, the speckle patterns thus obtained are photoelectrically converted into electrical signals, and the cross-correlation function between the speckle patterns is calculated using the electrical signals to obtain displacement of the speckle pattern on the basis of the shift of position of the extreme value of the mutual-correlation function and to determine the amount of deformation of the object from the displacement of the speckle pattern, (1) the reference speckle pattern data for calculation of the cross-correlation function is renewed when the extreme value of the cross-correlation function is lower in level than a predetermined value or when the position of the extreme value is out of a predetermined range, or (2) the reference speckle pattern data is renewed when the extreme value of the cross-correlation function is lower in level than a predetermined value and a calculation range for calculating the cross-correlation function is shifted when the position of the extreme value is out of a predetermined range.

Deformation measuring method and device using cross-correlation function

A realtime monitor of an astronomical object such as a double star using speckle interferometry comprises a TV camera for picking up an image of a star which is formed by a telescope, first means for producing an incoherent still picture of the star on the basis of an output from the TV camea, second means for producing a power spectrum of the star by converting the incoherent still picture to a coherent image and then optically Fourier-transforming it, third means for adding the consecutively produced power spectra to obtain an average power spectrum, and fourth means for controlling first, second and third means and calculating a normalized average power spectrum of an object star through dividing the average power spectrum of the object star by that of a reference star.

Method and apparatus for realtime-monitoring astronomical object with

An optical heterodyne detector comprising means for causing two light beams to interfere with each other and producing interference light beams thereof, a streak camera for receiving the interference light beams and analyzing means for analyzing an output of the streak camera, thereby to detect a beat frequency of the two light beams.

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Hamamatsu, Japan

Tamiki Takemori