The principle of a finite density of information
... up to a renormalization factor. Hence it is infinite, and the finite density principle cannot be formulated as the fact that the set of states of a bounded region of space is finite. These complex amplitudes λ and µ can be compared with probabilities. But this comparison has its limits. Indeed, sinc ...
... up to a renormalization factor. Hence it is infinite, and the finite density principle cannot be formulated as the fact that the set of states of a bounded region of space is finite. These complex amplitudes λ and µ can be compared with probabilities. But this comparison has its limits. Indeed, sinc ...
PrntFile text - Electrogravity
... the quantum particles would radiate in a non-coherant manner and in all directions which would be noise to a spectrum analyzer. However, if a material is used which has its quantum particles (atomic domains) aligned in a coherent manner, such as is the case for a quartz or ruby crystal, accelerating ...
... the quantum particles would radiate in a non-coherant manner and in all directions which would be noise to a spectrum analyzer. However, if a material is used which has its quantum particles (atomic domains) aligned in a coherent manner, such as is the case for a quartz or ruby crystal, accelerating ...
on the fine structure of spacetime
... is: an infinite dimensional complex linear space with a positive inner product, while matrices are replaced in this infinite dimensional set-up by linear operators. Thus in quantum mechanics the basic change of paradigm has to do with the observable quantities which one would classically describe as ...
... is: an infinite dimensional complex linear space with a positive inner product, while matrices are replaced in this infinite dimensional set-up by linear operators. Thus in quantum mechanics the basic change of paradigm has to do with the observable quantities which one would classically describe as ...
Full text
... of Fibonacci numbers with nonconsecutive indices and with each index greater than 1, where F0 = 0, Fx = 1, and Fi+2 = Ft +Fi+l form the Fibonacci numbers for i > 0 (see [13] and [17], or see [16, pp. 108-09]). The Zeckendorf decompositions of products of the forms kFm and kLm with fc,m GN (where Lm ...
... of Fibonacci numbers with nonconsecutive indices and with each index greater than 1, where F0 = 0, Fx = 1, and Fi+2 = Ft +Fi+l form the Fibonacci numbers for i > 0 (see [13] and [17], or see [16, pp. 108-09]). The Zeckendorf decompositions of products of the forms kFm and kLm with fc,m GN (where Lm ...