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Lens for holographic systems

Lens for holographic systems
IPC classes for russian patent Lens for holographic systems (RU 2132077):
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(57) Abstract:

Lens for holographic systems relates to the field of optical measurements. Lens for holographic systems contains located in a homogeneous environment on the same optical axis concentric spherical meniscus and a biconvex lens in such a way that their principal optical plane coincide. While the object under examination is placed in the front focal plane of the lens, and the radiation receiver in the rear. Randomly located source of coherent light illuminates the object under examination. As a consequence, each point of the investigated object becomes a source of secondary waves. Concentric spherical meniscus plays the role of a multi-beam interferometer, and a biconvex lens projecting the resulting interference pattern on the detector. Lens for holographic systems allows to obtain a holographic image of the investigated object, locking the phase and amplitude components of the signal. As the radiation receiver selects a matrix of photosensitive elements on the charge-coupled devices with high resolution. Lens for holographic systems pozvolyaet. 1 C.p. f-crystals, 1 Il.

The invention relates to the field of optical measurement and can be used in optical surveillance systems, photographic recording, and holographic systems.

Known multibeam interference device (application N 94035715/50 from 23.09.94 g, a positive decision from 05.04.96, containing on one optical axis point source of coherent linearly polarized radiation, installed on a course of radiation two parallel surfaces are spherical from optically transparent material, with a single center of curvature but different radii of curvature, and a photosensitive detector. In this device, the multipath interference occurs due to the interference of secondary waves, the centers of which are located on the first spherical surface. Svetalana occurs due to partial reflection of the incident light flux from the first and second spherical surfaces of multipath interference device. Focusing of optical beams occurs with lens with concentric spherical surfaces.

The disadvantage of this multipath interference device is that its what you can get information about the geometrical dimensions of the object (the amplitude component of the signal).

The closest in technical essence to the proposed lens for holographic systems is the system of recording of the hologram of the Fourier Fraunhofer, which is known as the schema entries in the focal planes (scheme focus-focus). This scheme is described in the monograph Optical holography: TRANS. c angl. Ed., Caulfield.-M.:Mir, 1982, c. 187. In this scheme, the object and reference point source located in the front focal plane of the lenticular lens, and the photographic plate is placed at the back focal plane of this lens. Each point of the object creates a parallel beam of light incident on the photographic plate. Off-axis point reference source also converted biconvex lens, resulting in collimated reference beam propagating at an angle to the optical axis. Watching from the side of the hologram, you can see that the object and reference source is actually located in infinity.

The disadvantage of the prototype is the inability to determine the spatial position of the object relative to the holographic system.

The task to be solved by the invention, is the lack of definition is the ache is solved by that lens for a holographic system that includes a biconvex lens 1 and a concentric spherical meniscus 2, in which the main plane coincide, the front focus of the lens coincides with the front focus F2concentric spherical meniscus 2, the back focus back focus (F1) lenticular lens 1, the object is located in the front focal plane of the concentric spherical meniscus 2, the object is located in the front focal plane of the concentric spherical meniscus 2, and a three-dimensional image is formed in the rear focal plane of the lenticular lens 1.

The technical result that can be obtained when implementing the present invention lies in the fact that this lens allows you to create a monocular holographic television system by taking into account diffraction effects occur on the concentric meniscus lens.

The drawing shows a diagram of the lens for holographic systems.

Lens for holographic systems contains located on the same optical axis concentric spherical meniscus 2 and the lenticular lens 1. The main optical plane holographic oboloi lens 1. The center of curvature C2concentric spherical meniscus 2 is located at the intersection of main optical plane of the lens HH' and the optical axis, r1and r2the radii of curvature of the larger and the smaller spherical surfaces concentric spherical meniscus 2, respectively. The object And the observation is located in the area of the front focus lens F2and the image receiver is located in the rear focus of the holographic lens (F1).

Lens for holographic systems works as follows.

The object And observations located in the region of the front focus lens F2, illuminated randomly located source of coherent light (not illustrated). Thus, each point of the object of observation is a source of secondary waves. Concentric spherical meniscus 2 plays the role of a multibeam interferometer, whose thickness d is determined by the formula:
d = n r21/(f (n - n0) + n r1), (1)
where r1the radius of curvature of the first spherical surface,
n is the refractive index of optically homogeneous material,
n0the refractive index of the medium,
f - focusnode in the front focus F2seems a planar wave front for the main optical plane HH' concentric spherical meniscus. With a small curvature radius r1the first spherical surface and a small thickness d of concentric spherical meniscus 2 main optical plane HH' is outside the scope of this lens. Concentric spherical meniscus 2 has a main plane center of curvature C2concentric spherical surfaces. Biconvex lens 1 has a main optical plane HH'. The design of the holographic lens is such that the plane of the concentric spherical meniscus 2, located at the point C2combined with the main plane HH' lenticular lens 1. This allows you to form a three-dimensional image in the rear focus of the lenticular lens, defined by the formula:
f = n r / (n - n0), (2)
where f is the focal length,
n is the refractive index of optically homogeneous material,
n0the refractive index of the medium,
r is the radius of curvature of the spherical surface,
without the distortion of information about the geometric dimensions of the test object. Recording a holographic image registration means as phase images on the radiation receiver. If the sensor is in the rear focus lens falls flat luminous flux, the amplitude of light on the photodetector is maximized. If a point source of radiation is in the front focus of concentric spherical meniscus 2, the spherical wave passing through the meniscus will have a flat wave front. In this case, the phase modulation signal. Flat wavefront after passing through concentric spherical meniscus using a lenticular lens 1 is converted into a dot image in the rear focus lens, that is the amplitude modulation of the light signal. Thus, this lens allows you to get a holographic image of the investigated object, the locking of the phase component signal by using concentric spherical meniscus 2 role of the multibeam interferometer, and the amplitude component by using a biconvex lens 1. As the radiation receiver, you can use the matrix of photosensitive elements on the charge-coupled devices (CCD) or a film. To obtain a high definition image you want to use photoresistive matenience with a grain size not more than 2 μm.

The proposed lens for holographic systems has the following advantages: the possibility of obtaining a holographic image, simple design and small size of the lens.

Industrial application: the proposed lens for holographic systems will find application in holographic information processing systems, particularly in systems of precise pozycjonowanie.

1. The holographic lens for systems containing a biconvex lens, characterized in that it further comprises a concentric spherical meniscus, located in front of the lenticular lens, with the main plane of the meniscus and the lenticular lens are the same, the front focus of the lens coincides with the front focus of concentric spherical meniscus, and the back focus of the lens coincides with the rear focus of the lenticular lens.

2. The lens under item 1, characterized in that the object is located in the front focal plane of the concentric spherical meniscus, and a three-dimensional image is formed in the rear focal plane of the lenticular lens.

 

 

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