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ul u2 s2 s3 <= u n s i g n e d ( s 1 ) ; -- o k , t y p e c a s t i n g <= t o - u n s i g n e d ( 5 , 4 ) ; -- o k , c o n v e r s i o n f u n c t i o n <= s t d - l o g i c - v e c t o r ( u 3 ) ; -- o k , t y p e c a s t i n g <= s t d - l o g i c - v e c t o r ( t o - u n s i g n e d ( 5 , 4 ) ) ; -- o k

i. Denisyuk, Y. N. (1962). Photographic Reconstruction of the Optical Properties of an Object in Its Own Scattered Radiation Field, Soviet Physiks Doklady, 7 , pp. 543-545. ii. Denisyuk, Y. N. (1963). On the Reproduction of the Optical Properties of an Object by the Wave Field of Its Own Scattered Radiation, Optics & SpecrrosCOPY, pp. 365-368. 18, iii. Denisyuk, Y. N. (1992). My Way in Holography, Leonardo, 2 5 , 5 , p. 425. iv. Klein, W. R. and B. D. Cook (1967). Unified Approach to Ultrasonic Light Diffraction, IEEE Trans. on Sonics and Ultrasonics, SU-14, pp. 123-134. v. Kogelnik, H. (1969). Coupled Wave Theory for Thick Hologram Gratings, Bell Systems Technical Journal, 48, pp. 2909-2947. vi. Liu, D., G. Manivannan, H. H. Arsenault, and R. A. Lessard (1995). Asymmetry in the Diffraction Spectrum of a Reflection Hologram Grating, J . Modern Optics, 42,3, pp. 639-653.

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(12.4) Now we hypothesize a medium for which K << 1 (the medium is antiIt is easy to demonstrate that a test charge immersed in such a medium will dig a hole in the medium, the hole will be stable, and inside the hole surrounding the test charge the dielectric constant IE is unity, while in the surrounding medium K. << 1 [see Lee (1981), Baym ( 1 9 8 2 ~and )~ Fig. 12.laj. On the other hand, it is not difficult to show that if a test charge is placed in a screening vacuum ( K > l),the radius of the hole created in the medium will shrink to zero. Thus test charges can produce structures of finite spacetime extent in a vacuum, provided the vacuum is antiscreening. This model can be used in conjunction with QCD to produce confinement (Lee, 1981; Baym, 1982c; Callan, Dashen, and Gross, 1979). We introduce a

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