Thin film beamsplitter optical element for use in an image-forming lens system

Claim 1

A beamsplitter structure producing a division of wavefront in each of a plurality of beams of radiation propagating between object and image fields of an optical lens system, wherein said divided wavefronts propagate to the image field of said optical system substantially free of aberration, distortion, and apodization, said beamsplitter structure comprising: first and second prisms disposed in an optical lens system, said first and second prisms composed of a material capable of supporting the propagation of image-forming beams of radiation having divergence angles and wavelength employed by said optical system and including at least one plane surface prism face on each prism, a plurality of thin-film coatings of dielectric materials layered on said plane surface of said first prism, wherein said plurality of thin-film coatings on said first prism include a first number of coating materials having selected composition and thicknesses to establish the approximate overall reflectivity of said beamsplitter, each of said coating materials having phase thickness less than one quarter of the minimum wavelength present in the central one of said image-forming beams; and a second number of coating materials having selected composition and thicknesses for correcting any non-trivial phase aberration and any non-uniform amplitude reflectance and transmittance provided by the initial plurality of coatings with minimal added net reflectivity said materials and having uniform thicknesses over said surface to produce a compensating phase distribution and a compensating amplitude distribution in the reflected and transmitted portions of said beams, when said beams are incident at said plane surface from outside said first prism or from inside said first prism; said compensating phase and amplitude distributions being substantially the algebraic negatives of the phase aberrations and amplitude nonuniformities of the remainder of said optical lens system, wherein said compensating phase distribution produced by said thin-film coatings, corresponds to the trivial aberrations of piston and field-independent image shift, and wherein said compensating amplitude distribution corresponds to substantially equal and uniform reflection and transmission of each of said beams over their full divergence, said at least one plane surface of said second prism being bonded to said thin film coatings on said first prism, on the opposite side of said thin film coatings from said first prism on which said thin film coatings are layered.

Claim 10

A method for adjusting trial thickness values of a thin film coating prior to reflection and transmission of a plurality of beams of radiation from said thin film coating, so as to set a demerit function to an extremum; said method for adjusting said trial thickness values of said thin film coating providing beams of radiation that are image-forming by comprising the steps of: (a) representing each of said beams as a vector of rays that intercept a reference sphere, (b) forming a vector of x direction cosine coordinates and a vector of y direction cosine coordinates for the intersections of said vector of rays with said reference sphere, (c) forming a vector of ray incidence angles for the intersections of said grid of rays with said thin film coatings, (d) transforming said vector of ray incidence angles into a vector of reflected amplitudes and a vector of transmitted amplitudes, (e) transforming said vector of reflected amplitudes and said vector of transmitted amplitudes into a vector of ray effective path lengths, a grid of total ray amplitudes, and a grid of field illumination values, (f) deriving image aberrations, image displacements, and illumination nonuniformities, for incorporation in said demerit function.

Claim 11

A method for adjusting trial thickness values of a thin film coating prior to reflection and transmission of a plurality of beams of radiation from said thin film coating, so as to set a demerit function to an extremum; said method for adjusting said trial thickness values of said thin film coating providing beams of radiation that are image-forming by comprising the steps of: (a) representing each of said beams as a vector of rays that intercept a reference sphere, (b) forming a vector of x direction cosine coordinates and a vector of y direction cosine coordinates for the intersections of said vector of rays with said reference sphere, (c) forming a vector of ray incidence angles for the intersections of said grid of rays with said thin film coatings, (d) transforming said vector of ray incidence angles into a vector of reflected amplitudes and a vector of transmitted amplitudes, (e) transforming said vector of reflected amplitudes and said vector of transmitted amplitudes into a vector of ray effective path lengths, a grid of total ray amplitudes, and a grid of field illumination values, (f) deriving image aberrations, image displacements, and illumination nonuniformities, for incorporation in said demerit function.