There is no distinction between spin and time axis. In quantum mechanics, spin is quantized with values of [math]\pm\frac{1}{2}\hbar[/math]. Since the zero point energy of one harmonic oscillator is given by [math]\frac{1}{2}\hbar \omega_0[/math], it means that the zero point energy is just the product of spin and the fundamental angular frequency. Time axis is dual (showing similarity with spinors), meaning it has a positive and a negative component or positive and negative direction. On the average, the orientation of these two components is nearly opposite. However, their absolute magnitudes have wide differences. These differences are relatively small for bosons, relatively big for fermions. Nevertheless, unlike spinors it is not necessary to represent these magnitudes by complex numbers unless the imaginary parts of the orthogonal space axes (as analogy of phase factor [math]e^{i\alpha}[/math]) are included in the formulation. Real numbers representations are more than sufficient. The maximum magnitude is equivalent to [math]\frac{1}{2}\hbar[/math], the minimum is theoretically zero. In other words, the upper limit of the absolute difference between the magnitude of these dual time axes can never be greater than [math]\frac{1}{2}\hbar[/math]. The lower limit is identically zero, the zero of all zeros. The photon should have its absolute difference magnitude of dual time axis nearly the true zero. It is the wide differences of these magnitudes, which are responsible for double rotations (720 degrees instead of the normal 360 degrees) of fermions returning to their initial quantum states.
The normalized column eigenvectors of the bosonic axes are [math]b_1=\left(\begin{array}{c}+1&-1\end{array}\right)[/math] and [math]b_2=\left(\begin{array}{c}-1&+1\end{array}\right)[/math]
For the fermions, there are four normalized eigenvectors
[math]f_1=\left(\begin{array}{c}+0&-1\end{array}\right)[/math], [math]f_2=\left(\begin{array}{c}-0&+1\end{array}\right)[/math],
[math]f_3=\left(\begin{array}{c}+1&-0\end{array}\right)[/math], [math]f_4=\left(\begin{array}{c}-1&+0\end{array}\right)[/math].
If we are allowed to join two eigenvectors into 2 by 2 matrices then the concatenations of the f’s give two of Pauli spin matrices (except for the one with complex elements), e.g., [math]\sigma_x=f_2 f_3 [/math] and [math]\sigma_z=f_3 f_1[/math]. Furthermore, the concatenations of the normalized column bosonic eigenvectors formed the singular matrices (zero determinants) of quantized space.


LinkBack URL
About LinkBacks
Reply With Quote

