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Home Optical Systems Superresolution-scanning-optical-device

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 Superresolution scanning optical device

Details
Inventors: Kato, Makoto; Kasazumi, Kenichi;
Assignee: Matsushita Electric Industrial Co., Ltd. (Osaka, JP)
Primary Examiner: Davie; James W.
Assistant Examiner:
Attorney, Agent or Firm: Willian Brinks Hofer Gilson & Lione

A superresolution scanning optical device has image forming means for forming the image of light from a coherent light source unit in the form of a fine spot on a conjugate face through an image forming optical system, and scanning means for scanning the fine spot formed on the conjugate face. The coherent light source unit has first and second light sources of which phases are reverse to each other. The first and second light sources have the relationship that the main lobe of the image of the second light source on the conjugate face is superposed on the lateral sides of the main lobe of the image of the first light source on the conjugate face.

DETAILED DESCRIPTION A first superresolution scanning optical device according to the present invention comprises image forming means for forming the image of light from a coherent light source unit in the form of a fine spot on a conjugator or imaging face through an image forming optical system, and scanning means for scanning the fine spot formed on the conjugate face, the coherent light source unit having at least first and second light sources of which phases are reverse to each other, the first and second light sources having the relationship that the main lobe of the image of the second light source on the conjugate face is superposed on the lateral sides of the main lobe of the image of the first light source on the conjugate face.
Accordingly, the amplitudes of the lateral sides of the main lobe of the image of the first light source are cancelled by the amplitude of the main lobe of the image of the second light source, thus reducing the width of the main lobe of the image of the first light source.
It is therefore possible to obtain superresolution smaller than the diffraction limit without slit-like or annular openings formed.
Thus, with a simple optical system, superresolution can be achieved without the amount of light of the main lobe remarkably decreased.
In the first superresolution scanning optical device, the coherent light source unit may further include a third light source presenting the same phase as that of the first light source, and the second and third light sources may have the relationship that the main lobe of the image of the third light source on the conjugate face is superposed on the lateral sides of the main lobe of the image of the second light source on the conjugate face.
In such an arrangement, that remaining portion of the reverse phase component of the image of the second light source which has not been cancelled in the interference of the phase component of the image of the first light source with the reverse phase component of the image of the second light source, is cancelled by the regular phase component of the image of the third light source



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