TAARP - Appendix D - Section D2.0, General Nature of the Three Level, Nested, Adaptive Mechanism

D2.0 General Nature of the Three Level, Nested, Adaptive Mechanism

      Figure D-2 presents a flow diagram of the proposed three level, nested, adaptive mechanism that will implement the pattern recognition methodology presented in Figure D-1.

      For each of the three adaptive loops in Figure D-2, there is a search process over a multidimensional parameter space.

      For LOOP I it is important to understand that for each geocentric planetary configuration there is one f(). Each f() is comprised of a sum of nine exponential functions, with two parameters xi and yi determining the amplitude and "width", respectively, of each exponential function. So, for a given iteration of this loop, there will be 60 f()s, one for each of the 60 geocentric planetary configurations in the 60-Item Perdurabo/TAARP Data Base, and 540 exponential functions, where 60 x 9 = 540. Thus, for each iteration of this loop there will be 60 X's and 60 Y's, where:

= x1
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x9
and = y1
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y9

      There is one and one for each geocentric planetary configuration. Furthermore, each xi and each yi of each individual and is a function of a number of parameters (p1,...,pq) that define how a set of factors, such as the diurnal position of a planet, the cosmic (i.e., zodiacal) position of a planet, and the very fact that a planet is unique (e.g., Mars is Mars and is not Jupiter) are to be treated.

      The space over which an adaptive search for LOOP I is carried out is the space defined by this set of parameters. Therefore, one iteration of LOOP I will correspond to one point in the q dimensional space defined by parameters p1,...,pq, which comprise vector . One point in P space will define exactly how the set of factors are to be transformed into the numerical values xi, yi. So, for each geocentric planetary configuration, there are nine planets (i=1,...9), and each planet exists within the realm of the set of factors. Each of the factors is manipulated in a certain way, depending on the particular point in P space that the current iteration of LOOP I has determined, and these factors are conglomerated together to give a value for xi and a value for yi for a given planet. The particular form of the manipulation for a given factor is the same for each geocentric planetary configuration for each iteration of LOOP I.

      Consider the following example. One factor of importance is the position of a planet relative to the eastern horizon. Assume that the way it has been determined to handle this factor is to model it with an exponential function:

AeB(H-i)2

Therefore, three of the parameters of would be assigned to this factor: one parameter for A specifying the amplitude, one parameter for B specifying the "width," and one parameter for H specifying where relative to the horizon the exponential function is centered. Therefore, since every planet in each of the 60 geocentric planetary configurations has a distinct location, i, every planet will have a unique value for this exponential function for any given iteration of LOOP I based on the particular values of the three parameters A, B, H that the LOOP I search process has determined. For each planet of each geocentric planetary configuration, the unique exponential function value will be conglomerated together with all the other factors to determine one value for xi and one value for yi. (Note that the exponential functions discussed here will help determine the xi and yi for the exponential functions in the 2nd Transformation of Figure D-1. In other words, two different sets of exponential functions are under discussion.)

      Section E6.0 of Appendix E discusses this subject in more detail. For now, suffice it to say that for LOOP I there is an adaptive search process over a q-dimensional space, where the parameters defining the space are p1, p2, ..., pq.

      For LOOP II, the search space is of dimension 2n, and the parameters of the search space are ci, di, where:


= c1
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cn
and = d1
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dn

are the parameter vectors. n is to be determined by the judgment of the analyst. The objective here is to partition the axis of Figure D-1, Part "e" into n windows, each of which with a center point, ci, and a width, di.

      Each point in the 2n dimensional parameter space of LOOP II will define a specific sampling of the amplitude and phase of the Fourier transform space of Figure D-1, Part "e." Thus the amplitude features, fai, and the phase features, fpi, of Figure D-1, Part "f" are determined by a single point in the 2n dimensional parameter space of LOOP II. So, for each iteration of LOOP II, for each of the 60 geocentric planetary configurations, there will be n Fourier amplitude features and n Fourier phase features. It will be the job of LOOP III to operate upon the 60 feature vector pairs , from LOOP II to see if it is possible to produce a correct separation of the 60 pairs into the three classes of High PHENOMENON, Medium PHENOMENON, and Low PHENOMENON.

      For LOOP III, the search space is of dimension 2m, and the parameters of the search space are wai, wpi, where

= wa1
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wam
and = wp1
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wpm

are the parameter vectors. m is to be determined by the judgment of the analyst, and is dependent upon the kind and degree of the polynomial operator that serves to define the discriminant function of the 6th Transformation of Figure D-1. (See Section D3.0 for a discussion of an example of a polynomial discriminant function.)

      Note that for each of the three adaptive loops in Figure D-2, there is a performance measure, PM, which plays two roles.

The exact form and function of the three PMs is to be determined by the analyst.

      One option for the PMs vis-a-vis ROLE I is:

      One option for the PMs vis-a-vis ROLE 2 is:

      Note that all of these ideas are simply meant to serve as food for thought for the execution of Task 2 in Section 7.2.

      Figures E-5 through E-9 in Appendix E are a continuation of the vein of thought presented above.