Epstein Secrets

MEL,EDWARD A SLIFKA,ALFRED A LORBER,STANLEY H MEYER,ELIZA S HIRSCH,CARL SI

VIN,SANFORD F ELLIOTT,WALTER J COOK,STANLEY SCHEERER,DR R DOLLENS,SUSAN MILLER,R

ER HOLDER,DOUG A MYERS,JAMES DELANEY,KATHY RAMSING,BYRON L COOK,CYNTHIA

niversality” (see above) entered the parlance of physics in the context of the statistical mechanics of phase transitions near their critical points (Stanley, 1971; Stauffer, 1985; Yeomans, 1993) and has come to refer to the finite set of transitions and quantities common to nonlinear systems arising in_ t

ike tents, sine functions and parabolas can be extracted from and represent the behavior of higher dimensional, nonlinear differential equations (see Devaney, 1989; Schuster, 1989 or Moon, 1992 for intuitive descriptions). They varied a parameter, such as the height of the tent or parabola, to systematical

esses are not a sign of measurement error, but rather evidence consonant with the statistical physics of nonequilibrium states and phase transitions (Stanley, 1971; Stauffer, 1985; Yeomans, 1993). Very high amplitude fluctuations and multiple, up to infinite, correlation lengths are characteristic of the n

orbits recursively as the dynamics proceed; and (3) Indecomposability—the attractor is not separable into isolated regions and no points escape (see Devaney, 1989, for one of the clearest definitions). Of particular relevance to information encoding and transport by brain mechanisms, it is important to vi