Phase conjugation

Any dipole has a scalar potential between its ends, as is well known. Extending earlier work by Stoney [23], in 1903 Whittaker [8] showed that the scalar potential decomposes into—and identically is—a harmonic set of bidirectional longitudinal EM wavepairs. Each wavepair is comprised of a longitudinal EM wave (LEMW) and its phase conjugate LEMW replica. Hence the formation of the dipole actually initiates the ongoing production of a harmonic set of such biwaves in 4-space (see Section III.A.l). 

We separate the Whittaker waves into two sets (1) the convergent phase conjugate set, in the imaginary plane and (2) the divergent real wave set, in... 

The Priore effort in France demonstrated an amplification of this exact action in cells, in thousands of successful lab animal tests in the 1960s and early 1970s, but no one could understand the mechanism. At the time, phase conjugate optics as we know it today had not been developed—much less its extension into NLO pumping in the time dimension. Nonetheless, revolutionary cures of terminal tumors, infectious trypanosomiasis, and atherosclerosis were rigorously demonstrated by the scientists working with the Priore method. 

T. Whittaker, Math. Ann. 57, 333-355 (1903) (an excellent paper which decomposes the scalar potential into a harmonic set of bi-directional phase conjugate longitudinal wavepairs). 

So let us consider the -potential most simply as being replaced with such a Whittaker [1,56] decomposition. Then each of these scalar potentials—from which the A potential function is made—is decomposable into a set of harmonic phase conjugate wavepairs (of longitudinal EM waves). If one takes all the phase conjugate half-set, those phase conjugate waves are converging on... 

Figure 1 graphically shows Whittaker s decomposition [1] of the scalar potential into a harmonic set of phase conjugate longitudinal EM wavepairs. The 3-symmetry of EM energy flow is broken [16,20] by the dipolarity of the potential, and 4-symmetry in energy flow without 3-flow symmetry is implemented [1,16]. 

In each wavepair the two waves superpose spatially, but travel in opposite directions. The two are phase conjugates and time-reversed replicas of each other. 

Figure 1. The scalar potential is a harmonic set of phase conjugate longitudinal EM waves.

Beyond the scope of this article, Anderson explains the operation of the gyroscope in intimate detail and describes two problems that have proved most vexing to manufacturers of the rtng-laser gyroscope, namely, frequency locking at low rotation rates and the bias effect. Improvements In this instrument are expected in the relatively near future heeause of what scientists have recently learned pertaining to the phenomenon of optical phase conjugation. 

Figure 19. Top A phase conjugate material in the absence of an applied field. Middle Beams 1 and 2 create a refractive index grating. Bottom Beam 3 interacts with the grating creating beam 4 that is the phase conjugate of beam 1.

Figure 20. Left A diverging set of beams reflected off of a normal mirror continue to diverge. Right A diverging set of beams reflected off of a phase conjugate minor exactly retrace their original path and are therefore recombined at their point of origin.

Poly(diacetylenes) also exhibit large %(3) values in resonant modes. Optical phase conjugation (DFWM) was demonstrated at 532 nm in solutions of a soluble diacetylene polymer, with %(3) 5 x 10-12 esu. 136) No... 

---