POLARIZATION OF THE LATTICE

Date and time

Let in some area of the Lattice consisting of N fudls, at present n of fudls be directed on axis X; m of fudls – against axis X; p – on axis Y; q – against axis Y; r – on axis Z; s – against axis Z.
Value is called as the instantaneous polarization of the considered Lattice area on axis X.
Value is the instantaneous polarization of the considered Lattice area on axis Y.
Value is the instantaneous polarization of the considered Lattice area on axis Z.
Wx, Wy and Wz values lie on an interval [−1; 1].
If the area consists only of the whole triads of fudls, n+m = p+q = r+s = u, n+m+p+q+r+s = 3u = N.
If the fudl oscillates only spontaneously, the probability of its oscillation in any chronon is equal in accuracy 1/2. During τ chronons the fudl oscillates, on average, τ/2 time.
If the quantity of oscillations of a fudl for τ considerably differs chronons from τ/2, so fluctuation takes place, or the fudl is influenced by other fudls, or that and another is simultaneous.
Value where n – number of oscillations of a fudl for τ chronons, m – the number of nonoscillations for the same time, is called as polarization of a fudl on time. It is possible to write down also.
If to consider the Lattice area consisting of N fudls, value , where n – number of the fudls oscillated in this chronon, and m – number of the fudls which were not pro-oscillated in this chronon, n+m = N, is the instantaneous polarization of the considered Lattice area on time. It is possible to write down also.
Apparently, the instantaneous polarization cannot be traced in physical experiment because of the limiting short duration. Polarization on time of a separate fudl can't also be measured – because of its extremely small size.
Physical devices trace cooperative polarization rather large (on microcosm scales) Lattice areas on rather long (from the quantum point of view) a time interval.