Analyzing the encoding range of amplitude-phase coupled spatial light modulators

Most spatial light modulators (SLMs) are limited in that they cannot produce arbitrary complex modulations. Because phase and amplitude are usually coupled, it is difficult to computer design appropriate modulation patterns fast enough for the real-time applications for which SLMs are suited. Dramatic computational speedups can be achieved by using encoding algorithms that directly translate desired complex values into values that the modulator can produce. For coherently illuminated SLMs in a Fourier transform arrangement, pseudorandom encoding can be used. Each SLM pixel is programmed in sequence by selecting a single value of pixel modulation from a random distribution having an average that is identical to the desired fully complex modulation. While the method approximates fairly arbitrary complex modulations, there are always some complex values that are outside the encoding range for each SLM coupling characteristic and for each specific pseudorandom algorithm. Using the binary random distribution leads to methods of evaluating and geometrically interpreting the encoding range. Evaluations are presented of achieving fully complex encoding with SLMs that produce less than 2? of phase shift, identifying an infinite set of encoding algorithms that encode the same value, identification of the maximum encoding range, and geometric interpretation of encoding errors.

[1]  A. Lohmann,et al.  Complex spatial filtering with binary masks. , 1966, Applied optics.

[2]  Robert W. Cohn,et al.  Pseudorandom encoding of complex-valued functions onto amplitude-coupled phase modulators , 1998 .

[3]  E. Tam,et al.  Full complex modulation using liquid-crystal televisions. , 1992, Applied optics.

[4]  R. Juday Optimal realizable filters and the minimum Euclidean distance principle. , 1993, Applied optics.

[5]  J W Goodman,et al.  Optimal maximum correlation filter for arbitrarily constrained devices. , 1989, Applied optics.

[6]  Richard D. Juday,et al.  HOLOMED: an algorithm for computer-generated holograms , 1996, Defense, Security, and Sensing.

[7]  L. B. Lesem,et al.  The kinoform: a new wavefront reconstruction device , 1969 .

[8]  Joseph N. Mait,et al.  Understanding diffractive optical design in the scalar domain , 1995, OSA Annual Meeting.

[9]  R. Gerchberg A practical algorithm for the determination of phase from image and diffraction plane pictures , 1972 .

[10]  Robert W. Cohn,et al.  Fully complex diffractive optics by means of patterned diffuser arrays: encoding concept and implications for fabrication , 1997 .

[11]  Wenyao Liu,et al.  Pseudorandom encoding of fully complex modulation to biamplitude phase modulators , 1996 .

[12]  N. C. Gallagher,et al.  Method for Computing Kinoforms that Reduces Image Reconstruction Error. , 1973, Applied optics.

[13]  O. Bryngdahl,et al.  I Digital Holography – Computer-Generated Holograms , 1990 .

[14]  A. W. Lohmann,et al.  Computer-generated binary holograms , 1969 .

[15]  Jari Turunen,et al.  Zeroth-order coding of complex amplitude in two dimensions , 1997 .

[16]  M P Dames,et al.  Efficient optical elements to generate intensity weighted spot arrays: design and fabrication. , 1991, Applied optics.

[17]  Colin Soutar,et al.  Measurement of the complex transmittance of the Epson liquid crystal television , 1994 .

[18]  Ernst Lueder,et al.  Complex transmission of liquid crystal spatial light modulators in optical signal processing applications , 1993, Electronic Imaging.

[19]  Francis T. S. Yu,et al.  Self-organizing optical neural network for unsupervised learning , 1990 .

[20]  O. Bryngdahl,et al.  Computer-generated holograms with pulse-density modulation , 1984 .

[21]  James M. Florence,et al.  Full-complex modulation with two one-parameter SLMs , 1991, Optics & Photonics.

[22]  Eric G. Johnson,et al.  Microgenetic-algorithm optimization methods applied to dielectric gratings , 1995 .

[23]  R. Juday Correlation with a spatial light modulator having phase and amplitude cross coupling. , 1989, Applied optics.

[24]  Robert W. Cohn Real-time multispot beam steering with electrically controlled spatial light modulators , 1997, Optics & Photonics.

[25]  Y Sheng,et al.  Full-range, continuous, complex modulation by the use of two coupled-mode liquid-crystal televisions. , 1996, Applied optics.

[26]  R. Cohn,et al.  Pseudorandom phase-only encoding of real-time spatial light modulators. , 1996, Applied optics.

[27]  James M. Florence,et al.  Full-complex spatial filtering with a phase mostly DMD , 1991, Optics & Photonics.

[28]  Henry Stark,et al.  Design of phase gratings by generalized projections , 1991 .

[29]  J. L. Pezzaniti,et al.  Phase-only modulation of a twisted nematic liquid-crystal TV by use of the eigenpolarization states. , 1993, Optics letters.

[30]  Bahaa E. A. Saleh,et al.  Theory and design of the liquid crystal TV as an optical spatial phase modulator , 1990 .