Optical system for a coherent light illuminating source

Claim 2

An optical system for an object illuminating light source, comprising a source for emitting a collimated coherent light beam, means for converting the collimated light beam into a multiplicity of secondary collimated light beams travelling in different directions, a lens for focusing each secondary light beam at a unique convergence area in the focal plane of the lens and means located substantially at the focal plane for giving either one of "0"-relative phase or "π"-relative phase to each secondary light beam convergence area to cancel at a plane spaced from the phase giving means all interference fringes, created by the interference of the secondary light beams, except for those interference fringes caused by the secondary light beams incident on the lens having the greatest angle relative to the optical axis of the lens.

Claim 3

An optical system for a coherent illuminating light source, comprising a source for emitting a collimated coherent light beam, diffraction means for converting by diffraction the collimated light beam into a multiplicity of secondary collimated light beams travelling in different directions, the secondary light beams parallel to the collimated light beam defining zero order secondary light beam and the secondary light beams travelling at discretely increasing angles from the zero order secondary light beam defining incrementally increasing orders, the secondary light beam orders having angles increasing in one direction from the zero order secondary light beam defining positive orders and the secondary light beam orders having angles increasing in the other direction defining negative orders, a lens for focusing each secondary light beam at a unique, discrete convergence area in the focal plane of the lens, and a phase plate located substantially at the focal plane for imparting such a phase distribution that either one of "0"-relative phase and "π"-relative phase is given to the zero order secondary light beam, "0"-relative phase is given to either one of the odd order secondary light beams different in sign and equal in absolute value to each other and "π"-relative phase is given to the other one of the odd order secondary light beams, and "0"-relative phase is given to even order secondary light beams.

Claim 4

An optical system for a coherent illuminating light source, comprising a source for emitting a collimated coherent light beam, diffraction means for converting by diffraction the collimated light beam into a multiplicity of secondary collimated light beams travelling in different directions, the secondary light beams parallel to the collimated light beam defining zero order secondary light beam and the secondary light beams travelling at discretely increasing angles from the zero order secondary light beam defining incrementally increasing orders, the secondary light beam orders having angles increasing in one direction from the zero order secondary light beam defining positive orders and the secondary light beam orders having angles increasing in the other direction defining negative orders, a lens for focusing each secondary light beam at a unique, discrete convergence area in the focal plane of the lens, and a phase plate located substantially at the focal plane for imparting such a phase distribution that either one of "0"-relative phase and "π"-relative phase is given to the zero order secondary light beam, "0"-relative phase is given to either one of the odd order secondary light beams different in sign and equal in absolute value to each other and "π"-relative phase is given to the other one of the odd order secondary light beams, and "0"-relative phase is given to even order secondary light beams.

Claim 5

An optical system according to claim 2, in which said source includes a laser source.

Claim 6

An optical system according to claim 2, in which said diffraction means comprises a diffraction grating for receiving the light from the source and converting it into secondary light beams.

Claim 7

An optical system according to claim 4, in which another lens is further provided for converging the secondary light beams which are passed through the phase plate.

Claim 8

An optical system according to claim 2, in which said phase plate has first and second groups of sections, the sections of said first group being different in thickness from those of said second group, whereby "π"-relative phase is given to the secondary light beams passed through said first group of sections and "0"-relative phase is given to the secondary light beams passed through said second group of sections.